Menu
Home Explore People Places Arts History Plants & Animals Science Life & Culture Technology
On this page
Timeline of the far future
Scientific projections regarding the far future

While the far future cannot be known with certainty, fields like astrophysics, which studies planets and stars, and particle physics, which explores matter at the smallest scales, help predict broad future events. Similarly, evolutionary biology, plate tectonics, and sociology examine life, shifting continents, and human societies over time. Timelines starting from 3001 CE cover possible events such as human extinction, Earth’s fate as the Sun becomes a red giant, and the role of proton decay as a potential end to all matter, offering insights into our distant future.

Earth, the Solar System, and the universe

See also: Formation and evolution of the Solar System and List of future astronomical events

All projections of the future of Earth, the Solar System and the universe must account for the second law of thermodynamics, which states that entropy, or a loss of the energy available to do work, must rise over time.5 Stars will eventually exhaust their supply of hydrogen fuel via fusion and burn out. The Sun will likely expand sufficiently to overwhelm most of the inner planets (Mercury, Venus, and possibly Earth) but not the giant planets, including Jupiter and Saturn. Afterwards, the Sun will be reduced to the size of a white dwarf, and the outer planets and their moons will continue to orbit this diminutive solar remnant. This future situation may be similar to the white dwarf star MOA-2010-BLG-477L and the Jupiter-sized exoplanet orbiting it.678

Long after the death of the Solar System, physicists expect that matter itself will eventually disintegrate under the influence of radioactive decay, as even the most stable materials break apart into subatomic particles.9 Current data suggests that the universe has a flat geometry (or very close to flat) and will therefore not collapse in on itself after a finite time.10 This infinite future could allow for the occurrence of massively improbable events, such as the formation of Boltzmann brains.11

Keys

Astronomy and astrophysics
Geology and planetary science
Biology
Particle physics
Mathematics
Technology and culture
Years from nowEvent
1,000Due to the lunar tides decelerating the Earth's rotation, the average length of a solar day will be 1⁄30 of an SI second longer than it is today. To compensate, either a leap second will have to be added to the end of a day multiple times during each month, or one or more consecutive leap seconds will have to be added at the end of some or all months.12
1,100As Earth's poles precess, Gamma Cephei replaces Polaris as the northern pole star.13
5,000As one of the long-term effects of global warming, the Greenland ice sheet will have completely melted.1415
10,000If a failure of the Wilkes Subglacial Basin "ice plug" in the next few centuries were to endanger the East Antarctic Ice Sheet, it would take up to this long to melt completely. Sea levels would rise 3 to 4 metres.16 One of the potential long-term effects of global warming, this is separate from the shorter-term threat to the West Antarctic Ice Sheet.
10,000If humans were extinct, Earth would be midway through a stable warm period with the next glacial period of the Quaternary glaciation due in 10,000 years, but if humans survived and did impact their planet, the greenhouse gas emissions would disrupt this natural cycle.17 According to research, the carbon dioxide released from burning fossil fuels could cause the planet to skip glacial periods repeatedly for at least the next 500,000 years.18
10,000 – 1 million19The red supergiant stars Betelgeuse and Antares will likely have exploded as supernovae. For a few months, the explosions should be easily visible on Earth in daylight.2021222324
11,700As Earth's poles precess, Vega, the fifth-brightest star in the sky, becomes the northern pole star.25 Although Earth cycles through many different naked-eye northern pole stars, Vega is the brightest.
11,000–15,000By this point, halfway through Earth's precessional cycle, Earth's axial tilt will be mirrored, causing summer and winter to occur on opposite sides of Earth's orbit. This means that the seasons in the Southern Hemisphere will be less extreme than they are today, as it will face away from the Sun at Earth's perihelion and towards the Sun at aphelion; the seasons in the Northern Hemisphere will be more extreme, as it experiences more pronounced seasonal variation because of a higher percentage of land.26
15,000The oscillating tilt of Earth's poles will have moved the North African Monsoon far enough north to change the climate of the Sahara back into a tropical one such as it had 5,000–10,000 years ago.2728
17,00029The best-guess recurrence rate for a "civilization-threatening" supervolcanic eruption large enough to eject one teratonne (one trillion tonnes) of pyroclastic material.3031
25,000The northern polar ice cap of Mars could recede as the planet reaches a warming peak of its northern hemisphere during the c. 50,000-year perihelion precession aspect of its Milankovitch cycle.3233
36,000The small red dwarf Ross 248 will pass within 3.024 light-years of Earth, becoming the closest star to the Sun.34 It will recede after about 8,000 years, making first Alpha Centauri (again) and then Gliese 445 the nearest stars35 (see timeline).
50,000According to Berger and Loutre, the current interglacial period will end,36 sending the Earth back into a glacial period of the Quaternary glaciation, regardless of the effects of anthropogenic global warming.

However, according to more recent studies in 2016, anthropogenic climate change, if left unchecked, may delay this otherwise expected glacial period by as much as an additional 50,000 years, potentially skipping it entirely.37

Niagara Falls will have eroded the remaining 32 km to Lake Erie and will therefore cease to exist.38

The many glacial lakes of the Canadian Shield will have been erased by post-glacial rebound and erosion.39

50,000Due to lunar tides decelerating the Earth's rotation, a day on Earth is expected to be one SI second longer than it is today. To compensate, either a leap second will have to be added to the end of every day, or the length of the day will have to be officially lengthened by one SI second.40
60,000It is possible that the current cooling trend might be interrupted by an interstadial phase (a warmer period), with the next glacial maximum of the Quaternary glaciation reached only in about 100 kyr AP.41
100,000The proper motion of stars across the celestial sphere, which results from their movement through the Milky Way, renders many of the constellations unrecognizable.42
100,00043The red hypergiant star VY Canis Majoris will likely have exploded in a supernova.44
100,000Native North American earthworms, such as Megascolecidae, will have naturally spread north through the United States Upper Midwest to the Canada–US border, recovering from the Laurentide ice sheet glaciation (38°N to 49°N), assuming a migration rate of 10 metres per year, and that a possible renewed glaciation by this time has not prevented this.45 (However, humans have already introduced non-native invasive earthworms of North America on a much shorter timescale, causing a shock to the regional ecosystem.)
100,000 – 10 million46Cupid and Belinda, moons of Uranus, will likely have collided.47
100,00048Earth will likely have undergone a supervolcanic eruption large enough to erupt 400 km3 (96 cubic miles) of magma.49
100,000According to Berger and Loutre, the next glacial maximum of the Quaternary glaciation is expected to be the most intense, regardless of the effects of anthropogenic global warming.50
> 100,000As one of the long-term effects of global warming, ten percent of anthropogenic carbon dioxide will still remain in a stabilized atmosphere.51
250,000Kamaʻehuakanaloa (formerly Lōʻihi), the youngest volcano in the Hawaiian–Emperor seamount chain, will rise above the surface of the ocean and become a new volcanic island.52
c. 300,00053At some point in the next few hundred thousand years, the Wolf–Rayet star WR 104 may explode in a supernova. There is a small chance that WR 104 is spinning fast enough to produce a gamma-ray burst (GRB), and an even smaller chance that such a GRB could pose a threat to life on Earth.5455
500,00056Earth will likely have been hit by an asteroid of roughly 1 km in diameter, assuming that it is not averted.57
500,000The rugged terrain of Badlands National Park in South Dakota will have eroded completely.58
600,00059The estimated time for the third super-eruption of the Toba supervolcano by this date. The first super-eruption occurred around 840,000 years ago, after 1.4 million years of magma input, whereas magma fed the second super-eruption at 75,000 years.6061
1 millionMeteor Crater, a large impact crater in Arizona considered the "freshest" of its kind, will have worn away.62
1 million63Desdemona and Cressida, moons of Uranus, will likely have collided.64

The stellar system Eta Carinae will likely have exploded in a supernova.65

1 million66Earth will likely have undergone a supervolcanic eruption large enough to erupt 3,200 km3 (770 cubic miles) of magma, an event comparable to the Toba supereruption 75,000 years ago.67
1.29 ± 0.04 millionThe star Gliese 710 will pass as close as 0.051 parsecs (0.1663 light-years; 10,520 astronomical units)68 to the Sun before moving away. This will gravitationally perturb members of the Oort cloud, a halo of icy bodies orbiting at the edge of the Solar System, thereafter raising the likelihood of a cometary impact in the inner Solar System.69
2 millionThe estimated time for the full recovery of coral reef ecosystems from human-caused ocean acidification if such acidification goes unchecked; the recovery of marine ecosystems after the acidification event that occurred about 65 million years ago took a similar length of time.70
2 million+The Grand Canyon will erode further, deepening slightly, but principally widening into a broad valley surrounding the Colorado River.71
2.7 millionThe average orbital half-life of current centaurs, which are unstable because of gravitational interactions with the several outer planets.72 See predictions for notable centaurs.
3 millionDue to tidal deceleration gradually slowing Earth's rotation, a day on Earth is expected to be one minute longer than it is today. To compensate, either a "leap minute" will have to be added to the end of every day, or the length of the day will have to be officially lengthened by one SI minute.73
6 millionEstimated time for comet C/1999 F1 (Catalina), one of the longest-period comets known to return to the inner Solar System, after having travelled in its orbit out to its aphelion 66,600 AU (1.053 light-years) from the Sun and back.74
10 millionThe Red Sea will flood the widening East African Rift valley, causing a new ocean basin to divide the continent of Africa75 and the African plate into the newly formed Nubian plate and the Somali plate.

The Indian plate will advance into Tibet by 180 km (110 mi). Nepali territory, whose boundaries are defined by the Himalayan peaks and the plains of India, will cease to exist.76

10 millionThe estimated time for the full recovery of biodiversity after a potential Holocene extinction, if it were on the scale of the five previous major extinction events.77

Even without a mass extinction, by this time most current species will have disappeared through the background extinction rate, with many clades gradually evolving into new forms.7879

15 millionAn estimated 694 stars will approach the Solar System to less than 5 parsecs. Of these, 26 have a good probability to come within 1.0 parsec (3.3 light-years) and 7 within 0.5 parsecs (1.6 light-years).80
20 millionThe Strait of Gibraltar will have closed due to subduction and a Ring of Fire will form in the Atlantic, similar to that in the Pacific.8182
30 million83Earth will likely have been hit by an asteroid of roughly 5 km in diameter, assuming that it is not averted.84
50 millionThe maximum estimated time before the moon Phobos collides with Mars.85
50 millionAccording to Christopher Scotese, the movement of the San Andreas Fault will cause the Gulf of California to flood into the California Central Valley. This will form a new inland sea on the West Coast of North America, causing the current locations of Los Angeles and San Francisco in California to merge.86 The Californian coast will begin to be subducted into the Aleutian Trench.87

Africa's collision with Eurasia will close the Mediterranean basin and create a mountain range similar to the Himalayas.88

The Appalachian Mountains peaks will have largely worn away,89 weathering at 5.7 Bubnoff units, although topography will actually rise as regional valleys deepen at twice this rate.90

50–60 millionThe Canadian Rockies will have worn away to a plain, assuming a rate of 60 Bubnoff units.91 The Southern Rockies in the United States are eroding at a somewhat slower rate.92
50–400 millionThe estimated time for Earth to naturally replenish its fossil fuel reserves.93
80 millionThe Big Island will have become the last of the current Hawaiian Islands to sink beneath the surface of the ocean, while a more recently formed chain of "new Hawaiian Islands" will then have emerged in their place.94
100 million95Earth will likely have been hit by an asteroid comparable in size to the one that triggered the K–Pg extinction 66 million years ago, assuming this is not averted.96
100 millionAccording to the Pangaea Proxima model created by Christopher R. Scotese, a new subduction zone will open in the Atlantic Ocean, and the Americas will begin to converge back toward Africa.97

Upper estimate for the lifespan of Saturn's rings in their current state.98

110 millionThe Sun's luminosity will have increased by one percent.99
125 millionAccording to the Pangaea Proxima model created by Christopher R. Scotese, the Atlantic Ocean is predicted to stop widening and begin to shrink as the Mid-Atlantic Ridge seafloor spreading gives way to subduction. In this scenario, the mid-ocean ridge between South America and Africa will probably be subducted first; the Atlantic Ocean is predicted to narrow as a result of subduction beneath the Americas. The Indian Ocean is also predicted to be smaller due to northward subduction of oceanic crust into the Central Indian trench. Antarctica is expected to split in two and shift northwards, colliding with Madagascar and Australia, enclosing a remnant of the Indian Ocean, which Scotese calls the "Medi-Pangaean Sea".100101
180 millionDue to the gradual slowing of Earth's rotation, a day on Earth will be one hour longer than it is today. To compensate, either a "leap hour" will have to be added to the end of every day, or the length of the day will have to be officially lengthened by one SI hour.102
230 millionPrediction of the orbits of the Solar System's planets is impossible over timespans greater than this, due to the limitations of Lyapunov time.103
240 millionFrom its present position, the Solar System completes one full orbit of the Galactic Center.104
250 millionAccording to Christopher R. Scotese, due to the northward movement of the West Coast of North America, the coast of California will collide with Alaska.105
250–350 millionAll the continents on Earth may fuse into a supercontinent.106107 Four potential arrangements of this configuration have been dubbed Amasia, Novopangaea, Pangaea Proxima and Aurica. This will likely result in a glacial period, lowering sea levels and increasing oxygen levels, further lowering global temperatures.108109
> 250 millionThe supercontinent's formation, thanks to a combination of continentality increasing distance from the ocean, an increase in volcanic activity resulting in atmospheric CO2 at double current levels, increased interspecific competition, and a 2.5 percent increase in solar flux, is likely to trigger an extinction event comparable to the Great Dying 250 million years ago. Mammals in particular are unlikely to survive, assuming they still exist in their current forms by this point.110111
300 millionDue to a shift in the equatorial Hadley cells to roughly 40° north and south, the amount of arid land will increase by 25%.112
300–600 millionThe estimated time for Venus's mantle temperature to reach its maximum. Then, over a period of about 100 million years, major subduction occurs and the crust is recycled.113
350 millionAccording to the extroversion model first developed by Paul F. Hoffman, subduction ceases in the Pacific Ocean basin.114115
400–500 millionThe supercontinent (Pangaea Proxima, Novopangaea, Amasia, or Aurica) will likely have rifted apart.116 This will likely result in higher global temperatures, similar to the Cretaceous period.117
500 million118The estimated time until a gamma-ray burst, or massive, hyperenergetic supernova, occurs within 6,500 light-years of Earth; close enough for its rays to affect Earth's ozone layer and potentially trigger a mass extinction, assuming the hypothesis is correct that a previous such explosion triggered the Ordovician–Silurian extinction event. However, the supernova would have to be precisely oriented relative to Earth to have such effect.119
600 millionTidal acceleration moves the Moon far enough from Earth that total solar eclipses are no longer possible.120
500–600 millionThe Sun's increasing luminosity begins to disrupt the carbonate–silicate cycle; higher luminosity increases weathering of surface rocks, which traps carbon dioxide in the ground as carbonate. As water evaporates from the Earth's surface, rocks harden, causing plate tectonics to slow and eventually stop once the oceans evaporate completely. With less volcanism to recycle carbon into the Earth's atmosphere, carbon dioxide levels begin to fall.121 By this time, carbon dioxide levels will fall to the point at which C3 photosynthesis is no longer possible. All plants that use C3 photosynthesis (roughly 99 percent of present-day species) will die.122 The extinction of C3 plant life is likely to be a long-term decline rather than a sharp drop. It is likely that plant groups will die one by one well before the critical carbon dioxide level is reached. The first plants to disappear will be C3 herbaceous plants, followed by deciduous forests, evergreen broad-leaf forests, and finally evergreen conifers.123

However, A 2024 paper by RJ Graham et al. argues that silicate weathering is far less temperature-dependent than initially thought, and that falling carbon dioxide levels are unlikely to lead to the death of life on Earth.124

500–800 millionAs Earth begins to warm and carbon dioxide levels fall, plants—and, by extension, animals—could survive longer by evolving other strategies such as requiring less carbon dioxide for photosynthetic processes, becoming carnivorous, adapting to desiccation, or associating with fungi. These adaptations are likely to appear near the beginning of the moist greenhouse.125 The decrease in plant life will result in less oxygen in the atmosphere, allowing for more DNA-damaging ultraviolet radiation to reach the surface. The rising temperatures will increase chemical reactions in the atmosphere, further lowering oxygen levels. Plant and animal communities become increasingly sparse and isolated as the Earth becomes more barren. Flying animals would be better off because of their ability to travel large distances looking for cooler temperatures.126 Many animals may be driven to the poles or possibly underground. These creatures would become active during the polar night and aestivate during the polar day due to the intense heat and radiation. Much of the land would become a barren desert, and plants and animals would primarily be found in the oceans.127
500–800 millionAs pointed out by Peter Ward and Donald Brownlee in their book The Life and Death of Planet Earth, according to NASA Ames scientist Kevin Zahnle, this is the earliest time for plate tectonics to eventually stop, due to the gradual cooling of the Earth's core, which could potentially turn the Earth back into a water world. This would, in turn, likely cause the extinction of Earth's remaining land life.128
800–900 millionCarbon dioxide levels will fall to the point at which C4 photosynthesis is no longer possible.129 Without plant life to recycle oxygen in the atmosphere, free oxygen and the ozone layer will disappear from the atmosphere allowing for intense levels of deadly UV light to reach the surface. Animals in food chains that were dependent on live plants will disappear shortly afterward.130 At most, animal life could survive about 3 to 100 million years after plant life dies out. Just like plants, the extinction of animals will likely coincide with the loss of plants. It will start with large animals, then smaller animals and flying creatures, then amphibians, followed by reptiles and, finally, invertebrates.131 In the book The Life and Death of Planet Earth, authors Peter D. Ward and Donald Brownlee state that some animal life may be able to survive in the oceans. Eventually, however, all multicellular life will die out.132 The first sea animals to go extinct will be large fish, followed by small fish and then, finally, invertebrates.133 The last animals to go extinct will be animals that do not depend on living plants, such as termites, or those near hydrothermal vents, such as worms of the genus Riftia.134 The only life left on the Earth after this will be single-celled organisms.
1 billion13527% of the ocean's mass will have been subducted into the mantle. If this were to continue uninterrupted, it would reach an equilibrium where 65% of present-day surface water would be subducted.136
1 billionBy this point, the Sagittarius Dwarf Spheroidal Galaxy will have been completely consumed by the Milky Way.137
1.1 billionThe Sun's luminosity will have increased by 10%, causing Earth's surface temperatures to reach an average of around 320 K (47 °C; 116 °F). The atmosphere will become a "moist greenhouse", resulting in a runaway evaporation of the oceans.138139 This would cause plate tectonics to stop completely, if not already stopped before this time.140 Pockets of water may still be present at the poles, allowing abodes for simple life.141142
1.2 billionHigh estimate until all plant life dies out, assuming some form of photosynthesis is possible despite extremely low carbon dioxide levels. If this is possible, rising temperatures will make any animal life unsustainable from this point on.143144145
1.3 billionEukaryotic life dies out on Earth due to carbon dioxide starvation. Only prokaryotes remain.146
1.5 billionCallisto is captured into the mean-motion resonance of the other Galilean moons of Jupiter, completing the 1:2:4:8 chain. (Currently only Io, Europa and Ganymede participate in the 1:2:4 resonance.)147
1.5–1.6 billionThe Sun's rising luminosity causes its circumstellar habitable zone to move outwards; as carbon dioxide rises in Mars's atmosphere, its surface temperature increases to levels akin to Earth during the ice age.148149
1.5–4.5 billionTidal acceleration moves the Moon far enough from the Earth to the point where it can no longer stabilize Earth's axial tilt. As a consequence, Earth's true polar wander becomes chaotic and extreme, leading to dramatic shifts in the planet's climate due to the changing axial tilt.150
1.6 billionLower estimate until all remaining life, which by now had been reduced to colonies of unicellular organisms in isolated microenvironments such as high-altitude lakes and caves, goes extinct.151152153
< 2 billionThe first close passage of the Andromeda Galaxy and the Milky Way.154
2 billionHigh estimate until the Earth's oceans evaporate if the atmospheric pressure were to decrease via the nitrogen cycle.155
2.55 billionThe Sun will have reached a maximum surface temperature of 5,820 K (5,550 °C; 10,020 °F). From then on, it will become gradually cooler while its luminosity will continue to increase.156
2.8 billionEarth's surface temperature will reach around 420 K (147 °C; 296 °F), even at the poles.157158
2.8 billionHigh estimate until all remaining Earth life goes extinct.159160
3–4 billionThe Earth's core freezes if the inner core continues to grow in size, based on its current growth rate of 1 mm (0.039 in) in diameter per year.161162163 Without its liquid outer core, Earth's magnetosphere shuts down,164 and solar winds gradually deplete the atmosphere.165
c. 3 billion166There is a roughly 1-in-100,000 chance that the Earth will be ejected into interstellar space by a stellar encounter before this point, and a 1-in-300-billion chance that it will be both ejected into space and captured by another star around this point. If this were to happen, any remaining life on Earth could potentially survive for far longer if it survived the interstellar journey.167
3.3 billion168There is a roughly one percent chance that Jupiter's gravity may make Mercury's orbit so eccentric as to cross Venus's orbit by this time, sending the inner Solar System into chaos. Other possible scenarios include Mercury colliding with the Sun, being ejected from the Solar System, or colliding with Venus or Earth.169170
3.5–4.5 billionThe Sun's luminosity will have increased by 35–40%, causing all water currently present in lakes and oceans to evaporate, if it had not done so earlier. The greenhouse effect caused by the massive, water-rich atmosphere will result in Earth's surface temperature rising to 1,400 K (1,130 °C; 2,060 °F), which is hot enough to melt some surface rock.171172173174
3.6 billionNeptune's moon Triton falls through the planet's Roche limit, potentially disintegrating into a planetary ring system similar to Saturn's.175
4.32 billionDue to the gradual slowing of Earth's rotation, a day on Earth will be twice as long as it is today. To compensate, either a "leap day" will have to be added to the end of every day, or the length of the day will have to be officially lengthened by one day.176
4.5 billionMars reaches the same solar flux as that of the Earth when it first formed 4.5 billion years ago from today.177
< 5 billionThe Andromeda Galaxy will have fully merged with the Milky Way, forming an elliptical galaxy dubbed "Milkomeda".178 There is also a small chance of the Solar System being ejected.179180 The planets of the Solar System will almost certainly not be disturbed by these events.181182183
5.4 billionThe Sun, having now exhausted its hydrogen supply, leaves the main sequence and begins evolving into a red giant.184
6.5 billionMars reaches the same solar radiation flux as Earth today, after which it will suffer a similar fate to the Earth as described above.185
6.6 billionThe Sun may experience a helium flash, resulting in its core becoming as bright as the combined luminosity of all the stars in the Milky Way galaxy.186
7.5 billionEarth and Mars may become tidally locked with the expanding red giant Sun.187
7.59 billionThe Earth and Moon are very likely destroyed by falling into the Sun, just before the Sun reaches the top of its red giant phase.188189 Before the final collision, the Moon possibly spirals below Earth's Roche limit, breaking into a ring of debris, most of which falls to the Earth's surface.190

During this era, Saturn's moon Titan, if not already ejected from the Saturnian system, may reach surface temperatures necessary to support life and would orbit further out from Saturn.191

7.9 billionThe Sun reaches the top of the red-giant branch of the Hertzsprung–Russell diagram, achieving its maximum radius of 256 times the present-day value.192 In the process, Mercury, Venus and Earth are likely destroyed.193
8 billionThe Sun becomes a carbon–oxygen white dwarf with about 54.05% of its present mass.194195196197 At this point, if the Earth survives, temperatures on the surface of the planet, as well as the other planets in the Solar System, will begin dropping rapidly, due to the white dwarf Sun emitting much less energy than it does today.
>22.3 billion22.3 billion years is the estimated time until the end of the universe in a Big Rip, assuming a model of dark energy with w = −1.5.198199 If the density of dark energy is less than −1, then the universe's expansion will continue to accelerate and the observable universe will grow ever sparser. Around 200 million years before the Big Rip, galaxy clusters like the Local Group or the Sculptor Group will be destroyed; 60 million years before the Big Rip, all galaxies will begin to lose stars around their edges and will completely disintegrate in another 40 million years; three months before the Big Rip, star systems will become gravitationally unbound, and planets will fly off into the rapidly expanding universe; thirty minutes before the Big Rip, planets, stars, asteroids and even extreme objects like neutron stars and black holes will evaporate into atoms; one hundred zeptoseconds (10−19 seconds) before the Big Rip, atoms will break apart. Ultimately, once the Rip reaches the Planck scale, cosmic strings would be disintegrated as well as the fabric of spacetime itself. The universe would enter into a "rip singularity" when all non-zero distances become infinitely large. Whereas a "crunch singularity" involves all matter being infinitely concentrated, in a "rip singularity", all matter is infinitely spread out.200

Observations of galaxy cluster speeds by the Chandra X-ray Observatory suggest that the value of w is c. −0.991, meaning the Big Rip is unlikely to occur.201 Meanwhile, more recent data (2018) from the Planck mission indicates the value of w to be c. −1.028 (±0.031), pushing the earliest possible time of the Big Rip to approximately 200 billion years into the future.202

50 billionIf the Earth and Moon are not engulfed by the Sun, by this time they will become tidally locked, with each showing only one face to the other.203204 Thereafter, the tidal action of the white dwarf Sun will extract angular momentum from the system, causing the lunar orbit to decay and the Earth's spin to accelerate.205
65 billionThe Moon may collide with the Earth or be torn apart to form an orbital ring due to the decay of its orbit, assuming the Earth and Moon have not already been destroyed.206
100 billion – 1 trillionAll the ≈47 galaxies207 of the Local Group will coalesce into a single large galaxy—an expanded "Milkomeda"/"Milkdromeda"; the last galaxies of the Local Group coalescing will mark the effective completion of its evolution.208
100–150 billionThe universe's expansion causes all galaxies beyond the former Local Group to disappear beyond the cosmic light horizon, removing them from the observable universe.209210
150 billionThe universe will have expanded by a factor of 6,000, and the cosmic microwave background will have cooled by the same factor to around 4.5×10−4 K. The temperature of the background will continue to cool in proportion to the expansion of the universe.211
325 billionThe estimated time by which the expansion of the universe will have isolated all gravitationally bound structures within their own cosmological horizon. At this point, the universe will have expanded by a factor of more than 100 million from today, and even individual exiled stars will be isolated.212
800 billionThe expected time when the net light emission from the combined "Milkomeda" galaxy begins to decline as the red dwarf stars pass through their blue dwarf stage of peak luminosity.213
1 trillionA low estimate for the time until star formation ends in galaxies as galaxies are depleted of the gas clouds they need to form stars.214

The universe's expansion, assuming a constant dark energy density, multiplies the wavelength of the cosmic microwave background by 1029, exceeding the scale of the cosmic light horizon and rendering its evidence of the Big Bang undetectable. However, it may still be possible to determine the expansion of the universe through the study of hypervelocity stars.215

1.05 trillionThe estimated time by which the universe will have expanded by a factor of more than 1026, reducing the average particle density to less than one particle per cosmological horizon volume. Beyond this point, particles of unbound intergalactic matter are effectively isolated, and collisions between them cease to affect the future evolution of the universe.216
1.4 trillionThe estimated time by which the cosmic background radiation cools to a floor temperature of 10−30 K and does not decline further. This residual temperature comes from horizon radiation, which does not decline over time.217
2 trillionThe estimated time by which all objects beyond our former Local Group are redshifted by a factor of more than 1053. Even gamma rays that they emit are stretched so that their wavelengths are greater than the physical diameter of the horizon. The resolution time for such radiation will exceed the physical age of the universe.218
4 trillionThe estimated time until the red dwarf star Proxima Centauri, the closest star to the Sun today, at a distance of 4.25 light-years, leaves the main sequence and becomes a white dwarf.219
10 trillionThe estimated time of peak habitability in the universe, unless habitability around low-mass stars is suppressed.220
12 trillionThe estimated time until the red dwarf star VB 10—as of 2016, the least-massive main-sequence star with an estimated mass of 0.075 M☉—runs out of hydrogen in its core and becomes a white dwarf.221222
30 trillionThe estimated time for stars (including the Sun) to undergo a close encounter with another star in local stellar neighborhoods. Whenever two stars (or stellar remnants) pass close to each other, their planets' orbits can be disrupted, potentially ejecting them from the system entirely. On average, the closer a planet's orbit to its parent star the longer it takes to be ejected in this manner, because it is gravitationally more tightly bound to the star.223
100 trillionA high estimate for the time by which normal star formation ends in galaxies.224 This marks the transition from the Stelliferous Era to the Degenerate Era; with too little free hydrogen to form new stars, all remaining stars slowly exhaust their fuel and die.225 By this time, the universe will have expanded by a factor of approximately 102554.226
110–120 trillionThe time by which all stars in the universe will have exhausted their fuel (the longest-lived stars, low-mass red dwarfs, have lifespans of roughly 10–20 trillion years).227 After this point, the stellar-mass objects remaining are stellar remnants (white dwarfs, neutron stars, black holes) and brown dwarfs.

Collisions between brown dwarfs will create new red dwarfs on a marginal level: on average, about 100 stars will shine in what was once "Milkomeda". Collisions between stellar remnants will create occasional supernovae.228

1015 (1 quadrillion)The estimated time until stellar close encounters detach all planets in star systems (including the Solar System) from their orbits.229

By this point, the black dwarf that was once the Sun will have cooled to 5 K (−268.15 °C; −450.67 °F).230

1019 to 1020(10–100 quintillion)The estimated time until 90–99% of brown dwarfs and stellar remnants (including the Sun) are ejected from galaxies. When two objects pass close enough to each other, they exchange orbital energy, with lower-mass objects tending to gain energy. Through repeated encounters, the lower-mass objects can gain enough energy in this manner to be ejected from their galaxy. This process eventually causes "Milkomeda"/"Milkdromeda" to eject the majority of its brown dwarfs and stellar remnants.231232
1020 (100 quintillion)The estimated time until the Earth collides with the black dwarf Sun due to the decay of its orbit via emission of gravitational radiation,233 if the Earth is not ejected from its orbit by a stellar encounter or engulfed by the Sun during its red giant phase.234
1023 (100 sextillion)Around this timescale most stellar remnants and other objects are ejected from the remains of their galactic cluster.235
1030 (1 nonillion)The estimated time until most or all of the remaining 1–10% of stellar remnants not ejected from galaxies fall into their galaxies' central supermassive black holes. By this point, with binary stars having fallen into each other, and planets into their stars, via emission of gravitational radiation, only solitary objects (stellar remnants, brown dwarfs, ejected planetary-mass objects, black holes) will remain in the universe.236
2×1036 (2 undecillion)The estimated time for all nucleons in the observable universe to decay, if the hypothesized proton half-life takes its smallest possible value (8.2 × 1033 years).237238
1036–1038 (1–100 undecillion)The estimated time for all remaining planets and stellar-mass objects, including the Sun, to disintegrate if proton decay can occur.239
3×1043 (30 tredecillion)The estimated time for all nucleons in the observable universe to decay, if the hypothesized proton half-life takes the largest possible value of 1041 years,240 assuming that the Big Bang was inflationary and that the same process that made baryons predominate over anti-baryons in the early universe makes protons decay. By this time, if protons do decay, the Black Hole Era, in which black holes are the only remaining celestial objects, begins.241242
3.14×1050 (314 quindecillion)The estimated time until a micro black hole of one Earth mass today will have decayed into subatomic particles by the emission of Hawking radiation.243
1065 (100 vigintillion)Assuming that protons do not decay, the estimated time for rigid objects, from free-floating rocks in space to planets, to rearrange their atoms and molecules via quantum tunnelling. On this timescale, any discrete body of matter "behaves like a liquid" and becomes a smooth sphere due to diffusion and gravity.244
1.16×1067 (11.6 unvigintillion)The estimated time until a black hole of one solar mass today will have decayed by the emission of Hawking radiation.245
1.54×1091–1.41×1092 (15.4–141 novemvigintillion)The estimated time until the resulting supermassive black hole of "Milkomeda"/"Milkdromeda" from the merger of Sagittarius A* and the P2 concentration during the collision of the Milky Way and Andromeda galaxies246 will have vanished by the emission of Hawking radiation,247 assuming it does not accrete any additional matter nor merge with other black holes—though it is most likely that this supermassive black hole will nonetheless merge with other supermassive black holes during the gravitational collapse towards "Milkomeda"/"Milkdromeda" of other Local Group galaxies.248 This supermassive black hole might be the very last entity from the former Local Group to disappear—and the last evidence of its existence.
10106 – 2.1×10109The estimated time until ultramassive black holes of 1014 (100 trillion) solar masses, predicted to form during the gravitational collapse of galaxy superclusters,249 decay by Hawking radiation.250 This marks the end of the Black Hole Era. Beyond this time, if protons do decay, the universe enters the Dark Era, in which all physical objects have decayed to subatomic particles, gradually winding down to their final energy state in the heat death of the universe.251252
10161A 2018 estimate of Standard Model lifetime before collapse of a false vacuum; 95% confidence interval is 1065 to 101383 years due in part to uncertainty about the top quark's mass.253254
10200The highest estimate for the time it would take for all nucleons in the observable universe to decay, provided they do not decay via the above process but instead through any one of many different mechanisms allowed in modern particle physics (higher-order baryon non-conservation processes, virtual black holes, sphalerons, etc.) on timescales of 1046 to 10200 years.255
101100–32000The estimated time for black dwarfs of 1.2 solar masses or more to undergo supernovae as a result of slow siliconnickeliron fusion, as the declining electron fraction lowers their Chandrasekhar limit, assuming protons do not decay.256
101500Assuming that protons do not decay, the estimated time until all baryonic matter in stellar remnants, planets and planetary-mass objects will have either fused together via muon-catalyzed fusion to form iron-56 or decayed from a higher mass element into iron-56 to form iron stars.257
10 10 26 {\displaystyle 10^{10^{26}}} 258259A low estimate for the time until all iron stars collapse via quantum tunnelling into black holes, assuming no proton decay or virtual black holes, and that Planck-scale black holes can exist.260

On this vast timescale, even ultra-stable iron stars will have been destroyed by quantum-tunnelling events. At this lower end of the timescale, iron stars decay directly to black holes, as this decay mode is much more favourable than decaying into a neutron star (which has an expected timescale of 10 10 76 {\displaystyle 10^{10^{76}}} years)261 and later decaying into a black hole. On these timescales, the subsequent evaporation of each resulting black hole into subatomic particles (a process lasting roughly 10100 years) and the subsequent shift to the Dark Era is instantaneous.

10 10 50 {\displaystyle 10^{10^{50}}} 262263264The estimated time for a Boltzmann brain to appear in the vacuum via a spontaneous entropy decrease.265
10 10 76 {\displaystyle 10^{10^{76}}} 266Highest estimate for the time until all iron stars collapse via quantum tunnelling into neutron stars or black holes, assuming no proton decay or virtual black holes, and that black holes below the Chandrasekhar mass cannot form directly.267 On these timescales, neutron stars above the Chandrasekhar mass rapidly collapse into black holes, and black holes formed by these processes instantly evaporate into subatomic particles.

This is also the highest estimated possible time for the Black Hole Era (and subsequent Dark Era) to commence. Beyond this point, it is almost certain that the universe will be an almost pure vacuum, gradually winding down its energy level until it reaches its final energy state, assuming it does not happen before this time.

10 10 120 {\displaystyle 10^{10^{120}}} 268The highest estimate for the time it takes for the universe to reach its final energy state.269
10 10 10 56 {\displaystyle 10^{10^{10^{56}}}} 270271Around this vast timeframe, quantum tunnelling in any isolated patch of the universe could generate new inflationary events, resulting in new Big Bangs giving birth to new universes.272

(Because the total number of ways in which all the subatomic particles in the observable universe can be combined is 10 10 115 {\displaystyle 10^{10^{115}}} ,273274 a number which, when multiplied by 10 10 10 56 {\displaystyle 10^{10^{10^{56}}}} , is approximately 10 10 10 56 {\displaystyle 10^{10^{10^{56}}}} , this is also the time required for a quantum-tunnelled and quantum fluctuation-generated Big Bang to produce a new universe identical to our own, assuming that every new universe contained at least the same number of subatomic particles and obeyed laws of physics within the landscape predicted by string theory.)275276

Humanity and human constructs

Keys

Astronomy and astrophysics
Geology and planetary science
Biology
Particle physics
Mathematics
Technology and culture

To date, five spacecraft (Voyager 1, Voyager 2, Pioneer 10, Pioneer 11 and New Horizons) are on trajectories that will take them out of the Solar System and into interstellar space. Barring an extremely unlikely collision with some object, all five should persist indefinitely.277

Date (CE) or years from nowEvent
3183 CEThe Zeitpyramide (time pyramid), a public art work started in 1993 at Wemding, Germany, is scheduled for completion.278
4017 CEMaximum lifespan of the data films in Arctic World Archive, a repository that contains code of open-source projects on GitHub along with other data of historical interest (if stored in optimum conditions).279
5207 CEAccording to Michio Kaku, the time by which humanity will be a Type II civilization, capable of harnessing all the energy of its host star.280
10,000The Waste Isolation Pilot Plant for nuclear weapons waste is planned to be protected until this time, with a "Permanent Marker" system designed to warn off visitors through multiple languages (the six UN languages and Navajo) and pictograms.281 The Human Interference Task Force has provided the theoretical basis for United States plans for future nuclear semiotics.282
10,000Planned lifespan of the Long Now Foundation's several ongoing projects, including a 10,000-year clock known as the Clock of the Long Now, the Rosetta Project and the Long Bet Project.283

Estimated lifespan of the HD-Rosetta analog disc—an ion beam-etched writing medium on nickel plate, a technology developed at Los Alamos National Laboratory and later commercialized. (The Rosetta Project uses this technology, named after the Rosetta Stone.)

10,000Projected lifespan of Norway's Svalbard Global Seed Vault.284
10,000Most probable estimated lifespan of technological civilization, according to Frank Drake's original formulation of the Drake equation.285
10,000If globalization trends lead to panmixia, human genetic variation will no longer be regionalized, as the effective population size will equal the actual population size.286
20,000According to the glottochronology linguistic model of Morris Swadesh, future languages should retain just one out of every 100 "core vocabulary" words on their Swadesh list compared to that of their current progenitors.287

The Chernobyl exclusion zone is expected to become habitable again.288

24,110Half-life of plutonium-239.289 At this point the Chernobyl Exclusion Zone, the 2,600-square-kilometre (1,000 sq mi) area of Ukraine and Belarus left deserted by the 1986 Chernobyl disaster, will return to normal levels of radiation.290
25,000The Arecibo message, a collection of radio data transmitted on 16 November 1974, will reach the distance of its destination: the globular cluster Messier 13.291 This is the only interstellar radio message sent to such a distant region of the galaxy. There will be a 24-light-year shift in the cluster's position in the galaxy during the time taken for the message to reach it, but as the cluster is 168 light-years in diameter, the message will still reach its destination.292 Any reply will take at least another 25,000 years from the time of its transmission.
14 September 30828 CEMaximum system time for 64-bit NTFS-based Windows operating system.293
33,800Pioneer 10 passes within 3.4 light-years of Ross 248.294
42,200Voyager 2 passes within 1.7 light-years of Ross 248.295
44,100Voyager 1 passes within 1.8 light-years of Gliese 445.296
46,600Pioneer 11 passes within 1.9 light-years of Gliese 445.297
50,000Estimated atmospheric lifetime of tetrafluoromethane, the most durable greenhouse gas.298
90,300Pioneer 10 passes within 0.76 light-years of HIP 117795.299
100,000+Time required to terraform Mars with an oxygen-rich breathable atmosphere, using only plants with solar efficiency comparable to the biosphere currently found on Earth.300
100,000–1 millionEstimated time by which humanity will be a Type III civilization, and could colonize the Milky Way galaxy and become capable of harnessing all the energy of the galaxy, assuming a velocity of 10% the speed of light.301
250,000The estimated minimum time at which the spent plutonium stored at New Mexico's Waste Isolation Pilot Plant will cease to be radiologically lethal to humans.302
13 September 275760 CEMaximum system time for the JavaScript programming language.303
492,300Voyager 1 passes within 1.3 light-years of HD 28343.304
1 millionEstimated lifespan of Memory of Mankind (MOM) self storage-style repository in Hallstatt salt mine in Austria, which stores information on inscribed tablets of stoneware.305

Planned lifespan of the Human Document Project being developed at the University of Twente in the Netherlands.306

1 millionCurrent glass objects in the environment will be decomposed.307

Various public monuments composed of hard granite will have eroded by one metre, in a moderate climate and assuming a rate of 1 Bubnoff unit (1 mm in 1,000 years, or ≈1 inch in 25,000 years).308

Without maintenance, the Great Pyramid of Giza will have eroded to the point where it is unrecognizable.309

On the Moon, Neil Armstrong's "one small step" footprint at Tranquility Base will erode by this time, along with those left by all twelve Apollo moonwalkers, due to the accumulated effects of space weathering.310311 (Normal erosion processes active on Earth are not present on the Moon because of its almost complete lack of atmosphere.)

1.2 millionPioneer 11 comes within three light-years of Delta Scuti.312
2 millionPioneer 10 passes near the bright star Aldebaran.313
2 millionVertebrate species separated for this long will generally undergo allopatric speciation.314 Evolutionary biologist James W. Valentine predicted that if humanity has been dispersed among genetically isolated space colonies over this time, the galaxy will host an evolutionary radiation of multiple human species with a "diversity of form and adaptation that would astound us".315 This would be a natural process of isolated populations, unrelated to potential deliberate genetic enhancement technologies.
4 millionPioneer 11 passes near one of the stars in the constellation Aquila.316
5–10 millionDue to gradual degeneration, the Y chromosome will have disappeared.317318
7.2 millionWithout maintenance, Mount Rushmore will have eroded to the point where it is unrecognizable.319
8 millionHumanity has a 95% probability of extinction by this date, according to J. Richard Gott's formulation of the controversial Doomsday argument.320
8 millionMost probable lifespan of the Pioneer 10 plaques before the etching is destroyed by poorly understood interstellar erosion processes.321

The LAGEOS satellites' orbits will decay, and they will re-enter Earth's atmosphere, carrying with them a message to any far future descendants of humanity and a map of the continents as they are expected to appear then.322

100 millionMaximal estimated lifespan of technological civilization, according to Frank Drake's original formulation of the Drake equation.323
100 millionFuture archaeologists should be able to identify an "Urban Stratum" of fossilized great coastal cities, mostly through the remains of underground infrastructure such as building foundations and utility tunnels.324
1 billionEstimated lifespan of "Nanoshuttle memory device" using an iron nanoparticle moved as a molecular switch through a carbon nanotube, a technology developed at the University of California at Berkeley.325
1 billionEstimated lifespan of the two Voyager Golden Records before the information stored on them is rendered unrecoverable.326

Estimated time for an astroengineering project to alter the Earth's orbit, compensating for the Sun's increasing brightness and outward migration of the habitable zone, accomplished by repeated asteroid gravity assists.327328

292277026596 CE (292 billion)Numeric overflow in system time for 64-bit Unix systems.329
1020 (100 quintillion)Estimated timescale for the Pioneer and Voyager spacecrafts to collide with a star (or stellar remnant).330
3×1019 – 3×1021(30 quintillion to 3 sextillion)Estimated lifespan of "Superman memory crystal" data storage using femtosecond laser-etched nanostructures in glass, a technology developed at the University of Southampton, at an ambient temperature of 30 °C (86 °F; 303 K).331332

See also

  • Astronomy portal
  • Stars portal
  • Outer space portal
  • World portal

Notes

Bibliography

References

  1. Overbye, Dennis (2 May 2023). "Who Will Have the Last Word on the Universe? – Modern science suggests that we and all our achievements and memories are destined to vanish like a dream. Is that sad or good?". The New York Times. Archived from the original on 2 May 2023. Retrieved 2 May 2023. /wiki/Dennis_Overbye

  2. "Deep Time Reckoning". MIT Press. Retrieved 14 August 2022. https://mitpress.mit.edu/9780262539265/deep-time-reckoning/

  3. Rescher, Nicholas (1998). Predicting the future: An introduction to the theory of forecasting. State University of New York Press. ISBN 978-0791435533. 978-0791435533

  4. Adams, Fred C.; Laughlin, Gregory (1 April 1997). "A dying universe: the long-term fate and evolution of astrophysical objects" (PDF). Reviews of Modern Physics. 69 (2): 337–372. arXiv:astro-ph/9701131. Bibcode:1997RvMP...69..337A. doi:10.1103/RevModPhys.69.337. ISSN 0034-6861. S2CID 12173790. Archived from the original (PDF) on 27 July 2018. Retrieved 10 October 2021. https://web.archive.org/web/20180727015521/https://cds.cern.ch/record/318436/files/9701131.pdf

  5. Nave, C.R. "Second Law of Thermodynamics". Georgia State University. Archived from the original on 13 May 2012. Retrieved 3 December 2011. http://hyperphysics.phy-astr.gsu.edu/hbase/thermo/seclaw.html

  6. Blackman, J. W.; Beaulieu, J. P.; Bennett, D. P.; Danielski, C.; et al. (13 October 2021). "A Jovian analogue orbiting a white dwarf star". Nature. 598 (7880): 272–275. arXiv:2110.07934. Bibcode:2021Natur.598..272B. doi:10.1038/s41586-021-03869-6. PMID 34646001. S2CID 238860454. Retrieved 14 October 2021. https://www.nature.com/articles/s41586-021-03869-6

  7. Blackman, Joshua; Bennett, David; Beaulieu, Jean-Philippe (13 October 2021). "A Crystal Ball Into Our Solar System's Future – Giant Gas Planet Orbiting a Dead Star Gives Glimpse Into the Predicted Aftermath of our Sun's Demise". Keck Observatory. Retrieved 14 October 2021. https://keckobservatory.org/white-dwarf-system/

  8. Ferreira, Becky (13 October 2021). "Astronomers Found a Planet That Survived Its Star's Death – The Jupiter-size planet orbits a type of star called a white dwarf, and hints at what our solar system could be like when the Sun burns out". The New York Times. Archived from the original on 28 December 2021. Retrieved 14 October 2021. https://ghostarchive.org/archive/20211228/https://www.nytimes.com/2021/10/13/science/white-dwarf-planet.html

  9. Adams, Fred C.; Laughlin, Gregory (1997). "A dying universe: the long-term fate and evolution of astrophysical objects". Reviews of Modern Physics. 69 (2): 337–372. arXiv:astro-ph/9701131. Bibcode:1997RvMP...69..337A. doi:10.1103/RevModPhys.69.337. S2CID 12173790. /wiki/ArXiv_(identifier)

  10. Komatsu, E.; Smith, K. M.; Dunkley, J.; Bennett, C. L.; et al. (2011). "Seven-Year Wilkinson Microwave Anisotropy Probe (WMAP) Observations: Cosmological Interpretation". The Astrophysical Journal Supplement Series. 192 (2): 18. arXiv:1001.4731. Bibcode:2011ApJS..192...19W. doi:10.1088/0067-0049/192/2/18. S2CID 17581520. /wiki/ArXiv_(identifier)

  11. Linde, Andrei (2007). "Sinks in the landscape, Boltzmann brains and the cosmological constant problem". Journal of Cosmology and Astroparticle Physics. 2007 (1): 022. arXiv:hep-th/0611043. Bibcode:2007JCAP...01..022L. CiteSeerX 10.1.1.266.8334. doi:10.1088/1475-7516/2007/01/022. ISSN 1475-7516. S2CID 16984680. /wiki/ArXiv_(identifier)

  12. Finkleman, David; Allen, Steve; Seago, John; Seaman, Rob; et al. (June 2011). "The Future of Time: UTC and the Leap Second". American Scientist. 99 (4): 312. arXiv:1106.3141. Bibcode:2011arXiv1106.3141F. doi:10.1511/2011.91.312. S2CID 118403321. /wiki/ArXiv_(identifier)

  13. McClure, Bruce; Byrd, Deborah (22 September 2021). "Gamma Cephei, aka Errai, a future North Star". earthsky.org. Retrieved 25 December 2021. https://earthsky.org/brightest-stars/gamma-cephei-errai-future-north-star/

  14. LOUTRE, MF (1 April 1995). "Greenland Ice Sheet over the next 5000 years". Geophysical Research Letters. 22 (7): 783–786. Bibcode:1995GeoRL..22..783L. doi:10.1029/95GL00362. Retrieved 16 February 2025. https://www.webofscience.com/wos/woscc/full-record/WOS:A1995QR15300011

  15. Bochow, N; Poltronieri, A; Robinson, A (2023). "Overshooting the critical threshold for the Greenland ice sheet". Nature. 622 (7983): 528–536. Bibcode:2023Natur.622..528B. doi:10.1038/s41586-023-06503-9. hdl:10261/359219. PMC 10584691. PMID 37853149. https://doi.org/10.1038/s41586-023-06503-9

  16. Mengel, M.; Levermann, A. (4 May 2014). "Ice plug prevents irreversible discharge from East Antarctica". Nature Climate Change. 4 (6): 451–455. Bibcode:2014NatCC...4..451M. doi:10.1038/nclimate2226. /wiki/Bibcode_(identifier)

  17. Shavit, Joseph (27 February 2025). "New research links ice ages to shifts in the Earth's orbit". The Brighter Side of News. Retrieved 28 February 2025. https://www.thebrighterside.news/post/new-research-links-ice-ages-to-shifts-in-the-earths-orbit/

  18. Schwaller, Fred (3 March 2025). "Our next ice age is due in 10,000 years, but there's a catch". Deutsche Welle. Retrieved 11 March 2025. https://www.dw.com/en/earths-next-ice-age-is-due-in-10000-years-but-theres-a-catch/a-71786018

  19. This represents the time by which the event will most probably have happened. It may occur randomly at any time from the present.

  20. Hockey, T.; Trimble, V. (2010). "Public reaction to a V = −12.5 supernova". The Observatory. 130 (3): 167. Bibcode:2010Obs...130..167H. /wiki/Bibcode_(identifier)

  21. "A giant star is acting strange, and astronomers are buzzing". National Geographic. 26 December 2019. Archived from the original on 8 January 2021. Retrieved 15 March 2020. https://web.archive.org/web/20210108042242/https://www.nationalgeographic.com/science/2019/12/betelgeuse-is-acting-strange-astronomers-are-buzzing-about-supernova/

  22. Sessions, Larry (29 July 2009). "Betelgeuse will explode someday". EarthSky Communications, Inc. Archived from the original on 23 May 2021. Retrieved 16 November 2010. http://earthsky.org/brightest-stars/betelgeuse-will-explode-someday

  23. Saio, Hideyuki; Nandal, Devesh; Meynet, Georges; Ekstöm, Sylvia (2 June 2023). "The evolutionary stage of Betelgeuse inferred from its pulsation periods". Monthly Notices of the Royal Astronomical Society. 526 (2): 2765. arXiv:2306.00287. Bibcode:2023MNRAS.526.2765S. doi:10.1093/mnras/stad2949. https://doi.org/10.1093%2Fmnras%2Fstad2949

  24. Neuhäuser, R.; Torres, G.; Mugrauer, M.; Neuhäuser, D. L.; et al. (July 2022). "Colour evolution of Betelgeuse and Antares over two millennia, derived from historical records, as a new constraint on mass and age". Monthly Notices of the Royal Astronomical Society. 516 (1): 693–719. arXiv:2207.04702. Bibcode:2022MNRAS.516..693N. doi:10.1093/mnras/stac1969. https://doi.org/10.1093%2Fmnras%2Fstac1969

  25. Howell, Elizabeth (9 November 2018). "Vega: The North Star of the Past and the Future". Space.com. Retrieved 25 December 2021. https://www.space.com/21719-vega.html

  26. Plait, Phil (2002). Bad Astronomy: Misconceptions and Misuses Revealed, from Astrology to the Moon Landing "Hoax". John Wiley and Sons. pp. 55–56. ISBN 978-0-471-40976-2. 978-0-471-40976-2

  27. Mowat, Laura (14 July 2017). "Africa's desert to become lush green tropics as monsoons MOVE to Sahara, scientists say". Daily Express. Archived from the original on 8 March 2021. Retrieved 23 March 2018. https://www.express.co.uk/news/world/828144/Climate-change-Africa-Sahel-Sahara-region-monsoon-rainfall-drought

  28. "Orbit: Earth's Extraordinary Journey". ExptU. 23 December 2015. Archived from the original on 14 July 2018. Retrieved 23 March 2018. https://web.archive.org/web/20180714131638/https://mymultiplesclerosis.co.uk/btbb/gilf-kebir-the-great-barrier-nick-drake-wadi-bakht/

  29. This represents the time by which the event will most probably have happened. It may occur randomly at any time from the present.

  30. "'Super-eruption' timing gets an update – and not in humanity's favour". Nature. 552 (7683): 8. 30 November 2017. doi:10.1038/d41586-017-07777-6. PMID 32080527. S2CID 4461626. Archived from the original on 24 July 2021. Retrieved 28 August 2020. https://www.nature.com/articles/d41586-017-07777-6

  31. "Scientists predict a volcanic eruption that would destroy humanity could happen sooner than previously thought". The Independent. Archived from the original on 9 November 2020. Retrieved 28 August 2020. https://www.independent.co.uk/news/science/volcano-super-eruption-apocalypse-wipe-out-life-human-kind-timeline-how-long-a8082006.html

  32. Schorghofer, Norbert (23 September 2008). "Temperature response of Mars to Milankovitch cycles". Geophysical Research Letters. 35 (18): L18201. Bibcode:2008GeoRL..3518201S. doi:10.1029/2008GL034954. S2CID 16598911. /wiki/Bibcode_(identifier)

  33. Beech, Martin (2009). Terraforming: The Creating of Habitable Worlds. Springer. pp. 138–142. Bibcode:2009tchw.book.....B. /wiki/Bibcode_(identifier)

  34. Matthews, R. A. J. (Spring 1994). "The Close Approach of Stars in the Solar Neighborhood". Quarterly Journal of the Royal Astronomical Society. 35 (1): 1. Bibcode:1994QJRAS..35....1M. /wiki/Quarterly_Journal_of_the_Royal_Astronomical_Society

  35. Matthews, R. A. J. (Spring 1994). "The Close Approach of Stars in the Solar Neighborhood". Quarterly Journal of the Royal Astronomical Society. 35 (1): 1. Bibcode:1994QJRAS..35....1M. /wiki/Quarterly_Journal_of_the_Royal_Astronomical_Society

  36. Berger, A.; Loutre, M. F. (23 August 2002). "An Exceptionally Long Interglacial Ahead?". Science. 297 (5585): 1287–1288. doi:10.1126/science.1076120. ISSN 0036-8075. PMID 12193773. S2CID 128923481. /wiki/Doi_(identifier)

  37. "Human-made climate change suppresses the next ice age – Potsdam Institute for Climate Impact Research". pik-potsdam.de. Archived from the original on 7 January 2021. Retrieved 21 October 2020. https://www.pik-potsdam.de/en/news/latest-news/human-made-climate-change-suppresses-the-next-ice-age

  38. "Niagara Falls Geology Facts & Figures". Niagara Parks. Archived from the original on 19 July 2011. Retrieved 29 April 2011. https://web.archive.org/web/20110719093559/http://www.niagaraparks.com/media/geology-facts-figures.html

  39. Bastedo, Jamie (1994). Shield Country: The Life and Times of the Oldest Piece of the Planet. Komatik Series, ISSN 0840-4488. Vol. 4. Arctic Institute of North America of the University of Calgary. p. 202. ISBN 9780919034792. Archived from the original on 3 November 2020. Retrieved 15 March 2020. 9780919034792

  40. Finkleman, David; Allen, Steve; Seago, John; Seaman, Rob; et al. (June 2011). "The Future of Time: UTC and the Leap Second". American Scientist. 99 (4): 312. arXiv:1106.3141. Bibcode:2011arXiv1106.3141F. doi:10.1511/2011.91.312. S2CID 118403321. /wiki/ArXiv_(identifier)

  41. Loutre, MF; Berger, A (1 July 2000). "Future climatic changes: Are we entering an exceptionally long interglacial?". Climatic Change. 46 (1–2): 61–90. Bibcode:2000ClCh...46...61L. doi:10.1023/A:1005559827189. Retrieved 25 February 2025. https://www.webofscience.com/wos/woscc/full-record/WOS:000087703900003

  42. Tapping, Ken (2005). "The Unfixed Stars". National Research Council Canada. Archived from the original on 8 July 2011. Retrieved 29 December 2010. https://web.archive.org/web/20110708075519/http://www.nrc-cnrc.gc.ca/eng/education/astronomy/tapping/2005/2005-08-31.html

  43. This represents the time by which the event will most probably have happened. It may occur randomly at any time from the present.

  44. Monnier, J. D.; Tuthill, P.; Lopez, GB; Cruzalebes, P.; et al. (1999). "The Last Gasps of VY Canis Majoris: Aperture Synthesis and Adaptive Optics Imagery". The Astrophysical Journal. 512 (1): 351–361. arXiv:astro-ph/9810024. Bibcode:1999ApJ...512..351M. doi:10.1086/306761. S2CID 16672180. /wiki/The_Astrophysical_Journal

  45. Schaetzl, Randall J.; Anderson, Sharon (2005). Soils: Genesis and Geomorphology. Cambridge University Press. p. 105. ISBN 9781139443463. 9781139443463

  46. This represents the time by which the event will most probably have happened. It may occur randomly at any time from the present.

  47. French, Robert S.; Showalter, Mark R. (August 2012). "Cupid is doomed: An analysis of the stability of the inner uranian satellites". Icarus. 220 (2): 911–921. arXiv:1408.2543. Bibcode:2012Icar..220..911F. doi:10.1016/j.icarus.2012.06.031. S2CID 9708287. /wiki/ArXiv_(identifier)

  48. This represents the time by which the event will most probably have happened. It may occur randomly at any time from the present.

  49. "Frequency, locations and sizes of super-eruptions". The Geological Society. Retrieved 27 June 2025. https://web.archive.org/web/20130613170422/https://www.geolsoc.org.uk/Education-and-Careers/Resources/Papers-and-Reports/~/media/shared/documents/education%20and%20careers/Super_eruptions.ashx

  50. Loutre, MF; Berger, A (1 July 2000). "Future climatic changes: Are we entering an exceptionally long interglacial?". Climatic Change. 46 (1–2): 61–90. Bibcode:2000ClCh...46...61L. doi:10.1023/A:1005559827189. Retrieved 25 February 2025. https://www.webofscience.com/wos/woscc/full-record/WOS:000087703900003

  51. Archer, David (2009). The Long Thaw: How Humans Are Changing the Next 100,000 Years of Earth's Climate. Princeton University Press. p. 123. ISBN 978-0-691-13654-7. 978-0-691-13654-7

  52. "Frequently Asked Questions". Hawai'i Volcanoes National Park. 2011. Archived from the original on 27 October 2012. Retrieved 22 October 2011. https://web.archive.org/web/20121027191821/http://www.nps.gov/havo/faqs.htm

  53. This represents the time by which the event will most probably have happened. It may occur randomly at any time from the present.

  54. Tuthill, Peter; Monnier, John; Lawrance, Nicholas; Danchi, William; et al. (2008). "The Prototype Colliding-Wind Pinwheel WR 104". The Astrophysical Journal. 675 (1): 698–710. arXiv:0712.2111. Bibcode:2008ApJ...675..698T. doi:10.1086/527286. S2CID 119293391. /wiki/ArXiv_(identifier)

  55. Tuthill, Peter. "WR 104: Technical Questions". Archived from the original on 3 April 2018. Retrieved 20 December 2015. http://www.physics.usyd.edu.au/~gekko/pinwheel/tech_faq.html

  56. This represents the time by which the event will most probably have happened. It may occur randomly at any time from the present.

  57. Bostrom, Nick (March 2002). "Existential Risks: Analyzing Human Extinction Scenarios and Related Hazards". Journal of Evolution and Technology. 9 (1). Archived from the original on 27 April 2011. Retrieved 10 September 2012. /wiki/Nick_Bostrom

  58. "Badlands National Park – Nature & Science – Geologic Formations". Archived from the original on 15 February 2015. Retrieved 21 May 2014. https://web.archive.org/web/20150215201841/http://www.nps.gov/badl/naturescience/geologicformations.htm

  59. This represents the time by which the event will most probably have happened. It may occur randomly at any time from the present.

  60. Fuge, Lauren (2 November 2021). "From the vault: Can we predict the next supervolcano eruption?". Cosmos. Retrieved 14 April 2025. https://cosmosmagazine.com/earth/earth-sciences/can-we-predict-the-next-supervolcano-eruption/

  61. "Estimating Future Super-Eruptions at Toba Volcano". Innovations Report. 2 November 2021. https://www.innovations-report.com/agriculture-environment/earth-sciences/the-silent-build-up-to-a-super-eruption/

  62. Landstreet, John D. (2003). Physical Processes in the Solar System: An introduction to the physics of asteroids, comets, moons and planets. Keenan & Darlington. p. 121. ISBN 9780973205107. Archived from the original on 28 October 2020. Retrieved 15 March 2020. 9780973205107

  63. This represents the time by which the event will most probably have happened. It may occur randomly at any time from the present.

  64. "Uranus's colliding moons". astronomy.com. 2017. Archived from the original on 26 February 2021. Retrieved 23 September 2017. http://www.astronomy.com/news/2017/09/uranus-colliding-moons

  65. "Preview of a Forthcoming Supernova". 24 February 2012. Retrieved 22 April 2025. https://www.nasa.gov/image-article/preview-of-forthcoming-supernova/

  66. This represents the time by which the event will most probably have happened. It may occur randomly at any time from the present.

  67. "Frequency, locations and sizes of super-eruptions". The Geological Society. Retrieved 27 June 2025. https://web.archive.org/web/20130613170422/https://www.geolsoc.org.uk/Education-and-Careers/Resources/Papers-and-Reports/~/media/shared/documents/education%20and%20careers/Super_eruptions.ashx

  68. de la Fuente Marcos, Raúl; de la Fuente Marcos, Carlos (2020). "An Update on the Future Flyby of Gliese 710 to the Solar System Using Gaia EDR3: Slightly Closer and a Tad Later than Previous Estimates". Research Notes of the AAS. 4 (12): 222. doi:10.3847/2515-5172/abd18d. https://doi.org/10.3847%2F2515-5172%2Fabd18d

  69. Berski, Filip; Dybczyński, Piotr A. (November 2016). "Gliese 710 will pass the Sun even closer: Close approach parameters recalculated based on the first Gaia data release". Astronomy & Astrophysics. 595: L10. Bibcode:2016A&A...595L..10B. doi:10.1051/0004-6361/201629835. ISSN 0004-6361. /wiki/Bibcode_(identifier)

  70. Goldstein, Natalie (2009). Global Warming. Infobase Publishing. p. 53. ISBN 9780816067695. Archived from the original on 7 November 2020. Retrieved 15 March 2020. The last time acidification on this scale occurred (about 65 mya) it took more than 2 million years for corals and other marine organisms to recover; some scientists today believe, optimistically, that it could take tens of thousands of years for the ocean to regain the chemistry it had in preindustrial times. 9780816067695

  71. "Grand Canyon – Geology – A dynamic place". Views of the National Parks. National Park Service. Archived from the original on 25 April 2021. Retrieved 11 October 2020. https://www.nps.gov/grca/learn/nature/grca-geology.htm

  72. Horner, J.; Evans, N. W.; Bailey, M. E. (2004). "Simulations of the Population of Centaurs I: The Bulk Statistics". Monthly Notices of the Royal Astronomical Society. 354 (3): 798–810. arXiv:astro-ph/0407400. Bibcode:2004MNRAS.354..798H. doi:10.1111/j.1365-2966.2004.08240.x. S2CID 16002759. https://doi.org/10.1111%2Fj.1365-2966.2004.08240.x

  73. Finkleman, David; Allen, Steve; Seago, John; Seaman, Rob; et al. (June 2011). "The Future of Time: UTC and the Leap Second". American Scientist. 99 (4): 312. arXiv:1106.3141. Bibcode:2011arXiv1106.3141F. doi:10.1511/2011.91.312. S2CID 118403321. /wiki/ArXiv_(identifier)

  74. Horizons output. "Barycentric Osculating Orbital Elements for Comet C/1999 F1 (Catalina)". Archived from the original on 9 March 2021. Retrieved 7 March 2011. /wiki/JPL_Horizons_On-Line_Ephemeris_System

  75. Haddok, Eitan (29 September 2008). "Birth of an Ocean: The Evolution of Ethiopia's Afar Depression". Scientific American. Archived from the original on 24 December 2013. Retrieved 27 December 2010. http://www.scientificamerican.com/article.cfm?id=birth-of-an-ocean

  76. Bilham, Roger (November 2000). "NOVA Online | Everest | Birth of the Himalaya". pbs.org. Archived from the original on 19 June 2021. Retrieved 22 July 2021. https://www.pbs.org/wgbh/nova/everest/earth/birth.html

  77. Kirchner, James W.; Weil, Anne (9 March 2000). "Delayed biological recovery from extinctions throughout the fossil record". Nature. 404 (6774): 177–180. Bibcode:2000Natur.404..177K. doi:10.1038/35004564. PMID 10724168. S2CID 4428714. /wiki/James_Kirchner

  78. Wilson, Edward O. (1999). The Diversity of Life. W.W. Norton & Company. p. 216. ISBN 9780393319408. Archived from the original on 4 October 2020. Retrieved 15 March 2020. 9780393319408

  79. Wilson, Edward Osborne (1992). "The Human Impact". The Diversity of Life. London, England: Penguin UK (published 2001). ISBN 9780141931739. Archived from the original on 1 August 2020. Retrieved 15 March 2020. 9780141931739

  80. Bailer-Jones, C. A. L.; Rybizki, J.; Andrae, R.; Fouesnea, M. (2018). "New stellar encounters discovered in the second Gaia data release". Astronomy & Astrophysics. 616 (37): A37. arXiv:1805.07581. Bibcode:2018A&A...616A..37B. doi:10.1051/0004-6361/201833456. S2CID 56269929. /wiki/ArXiv_(identifier)

  81. Duarte, João C.; Riel, Nicolas; Rosas, Filipe M.; Popov, Anton; et al. (13 February 2024). "Gibraltar subduction zone is invading the Atlantic". Scientific Research. 52 (5): 331–335. Bibcode:2024Geo....52..331D. doi:10.1130/G51654.1. Retrieved 17 January 2025. https://pubs.geoscienceworld.org/gsa/geology/article-abstract/52/5/331/634682/Gibraltar-subduction-zone-is-invading-the-Atlantic?redirectedFrom=fulltext

  82. Phiddian, Ellen (18 February 2024). "The Atlantic Ocean is growing – but only for now". Retrieved 17 January 2025. https://cosmosmagazine.com/earth/earth-sciences/atlantic-ocean-shrinking-gibraltar/

  83. This represents the time by which the event will most probably have happened. It may occur randomly at any time from the present.

  84. "This is what would happen if scientists found an asteroid heading to Earth". 6 April 2023. Retrieved 27 June 2025. https://www.space.com/nasa-models-hypothetical-asteroid-impact-scenario

  85. Bills, Bruce G.; Gregory A. Neumann; David E. Smith; Maria T. Zuber (2005). "Improved estimate of tidal dissipation within Mars from MOLA observations of the shadow of Phobos". Journal of Geophysical Research. 110 (E7). E07004. Bibcode:2005JGRE..110.7004B. doi:10.1029/2004je002376. https://doi.org/10.1029%2F2004je002376

  86. Scotese, Christopher R. "Pangea Ultima will form 250 million years in the Future". Paleomap Project. Archived from the original on 25 February 2019. Retrieved 13 March 2006. http://www.scotese.com/newpage11.htm

  87. Garrison, Tom (2009). Essentials of Oceanography (5th ed.). Brooks/Cole. p. 62. ISBN 978-1337098649. 978-1337098649

  88. "Continents in Collision: Pangea Ultima". NASA. 2000. Archived from the original on 17 April 2019. Retrieved 29 December 2010. https://science.nasa.gov/science-news/science-at-nasa/2000/ast06oct_1/

  89. "Geology". Encyclopedia of Appalachia. University of Tennessee Press. 2011. Archived from the original on 21 May 2014. Retrieved 21 May 2014. https://web.archive.org/web/20140521203455/http://www.encyclopediaofappalachia.com/category.php?rec=2

  90. Hancock, Gregory; Kirwan, Matthew (January 2007). "Summit erosion rates deduced from 10Be: Implications for relief production in the central Appalachians" (PDF). Geology. 35 (1): 89. Bibcode:2007Geo....35...89H. doi:10.1130/g23147a.1. Archived (PDF) from the original on 23 December 2018. Retrieved 21 May 2014. http://pages.geo.wvu.edu/~kite/HancockKirwan2007SummitErosion.pdf

  91. Yorath, C. J. (2017). Of rocks, mountains and Jasper: a visitor's guide to the geology of Jasper National Park. Dundurn Press. p. 30. ISBN 9781459736122. [...] 'How long will the Rockies last?' [...] The numbers suggest that in about 50 to 60 million years the remaining mountains will be gone, and the park will be reduced to a rolling plain much like the Canadian prairies. 9781459736122

  92. Dethier, David P.; Ouimet, W.; Bierman, P. R.; Rood, D. H.; et al. (2014). "Basins and bedrock: Spatial variation in 10Be erosion rates and increasing relief in the southern Rocky Mountains, USA" (PDF). Geology. 42 (2): 167–170. Bibcode:2014Geo....42..167D. doi:10.1130/G34922.1. Archived (PDF) from the original on 23 December 2018. Retrieved 22 May 2014. http://noblegas.berkeley.edu/~balcs/pubs/Dethier_2014_Geology.pdf

  93. Patzek, Tad W. (2008). "Can the Earth Deliver the Biomass-for-Fuel we Demand?". In Pimentel, David (ed.). Biofuels, Solar and Wind as Renewable Energy Systems: Benefits and Risks. Springer. ISBN 9781402086533. Archived from the original on 1 August 2020. Retrieved 15 March 2020. 9781402086533

  94. Perlman, David (14 October 2006). "Kiss that Hawaiian timeshare goodbye / Islands will sink in 80 million years". San Francisco Chronicle. Archived from the original on 17 April 2019. Retrieved 21 May 2014. /wiki/David_Perlman

  95. This represents the time by which the event will most probably have happened. It may occur randomly at any time from the present.

  96. Nelson, Stephen A. "Meteorites, Impacts, and Mass Extinction". Tulane University. Archived from the original on 6 August 2017. Retrieved 13 January 2011. http://www.tulane.edu/~sanelson/geol204/impacts.htm

  97. Scotese, Christopher R. "Pangea Ultima will form 250 million years in the Future". Paleomap Project. Archived from the original on 25 February 2019. Retrieved 13 March 2006. http://www.scotese.com/newpage11.htm

  98. Lang, Kenneth R. (2003). The Cambridge Guide to the Solar System. Cambridge University Press. p. 329. ISBN 9780521813068. [...] all the rings should collapse [...] in about 100 million years. 9780521813068

  99. Schröder, K.-P.; Smith, Robert Connon (2008). "Distant future of the Sun and Earth revisited". Monthly Notices of the Royal Astronomical Society. 386 (1): 155–163. arXiv:0801.4031. Bibcode:2008MNRAS.386..155S. doi:10.1111/j.1365-2966.2008.13022.x. S2CID 10073988. https://doi.org/10.1111%2Fj.1365-2966.2008.13022.x

  100. Scotese, Christopher R. (30 May 2021). "An Atlas of Phanerozoic Paleogeographic Maps: The Seas Come In and the Seas Go Out". Annual Review of Earth and Planetary Sciences. 49 (1): 679–728. Bibcode:2021AREPS..49..679S. doi:10.1146/annurev-earth-081320-064052. S2CID 233708826. https://doi.org/10.1146%2Fannurev-earth-081320-064052

  101. Scotese, Christopher R (2 February 2003). "The Atlantic Ocean begins to Close". Paleomap Project. Archived from the original on 26 April 2021. Retrieved 24 March 2012. http://www.scotese.com/future1.htm

  102. Finkleman, David; Allen, Steve; Seago, John; Seaman, Rob; et al. (June 2011). "The Future of Time: UTC and the Leap Second". American Scientist. 99 (4): 312. arXiv:1106.3141. Bibcode:2011arXiv1106.3141F. doi:10.1511/2011.91.312. S2CID 118403321. /wiki/ArXiv_(identifier)

  103. Hayes, Wayne B. (2007). "Is the Outer Solar System Chaotic?". Nature Physics. 3 (10): 689–691. arXiv:astro-ph/0702179. Bibcode:2007NatPh...3..689H. CiteSeerX 10.1.1.337.7948. doi:10.1038/nphys728. S2CID 18705038. /wiki/ArXiv_(identifier)

  104. Leong, Stacy (2002). "Period of the Sun's Orbit Around the Galaxy (Cosmic Year)". The Physics Factbook. Archived from the original on 10 August 2011. Retrieved 2 April 2007. http://hypertextbook.com/facts/2002/StacyLeong.shtml

  105. Scotese, Christopher R. "Pangea Ultima will form 250 million years in the Future". Paleomap Project. Archived from the original on 25 February 2019. Retrieved 13 March 2006. http://www.scotese.com/newpage11.htm

  106. Scotese, Christopher R. "Pangea Ultima will form 250 million years in the Future". Paleomap Project. Archived from the original on 25 February 2019. Retrieved 13 March 2006. http://www.scotese.com/newpage11.htm

  107. Williams, Caroline; Nield, Ted (20 October 2007). "Pangaea, the comeback". New Scientist. Archived from the original on 13 April 2008. Retrieved 2 January 2014. https://web.archive.org/web/20080413162401/http://www.science.org.au/nova/newscientist/104ns_011.htm

  108. Calkin, P. E.; Young, G. M. (1996), "Global glaciation chronologies and causes of glaciation", in Menzies, John (ed.), Past glacial environments: sediments, forms, and techniques, vol. 2, Butterworth-Heinemann, pp. 9–75, ISBN 978-0-7506-2352-0. 978-0-7506-2352-0

  109. Perry, Perry; Russel, Thompson (1997). Applied climatology : principles and practice. London, England: Routledge. pp. 127–128. ISBN 9780415141000. 9780415141000

  110. Farnsworth, Alexander; Lo, Y. T. Eunice; Valdes, Paul J.; Buzan, Jonathan R.; et al. (25 September 2023). "Climate extremes likely to drive land mammal extinction during next supercontinent assembly" (PDF). Nature Geoscience. 16 (10): 901–908. Bibcode:2023NatGe..16..901F. doi:10.1038/s41561-023-01259-3. https://eprints.whiterose.ac.uk/201952/16/s41561-023-01259-3.pdf

  111. O'Malley-James, Jack T.; Greaves, Jane S.; Raven, John A.; Cockell, Charles S. (2014). "Swansong Biosphere II: The final signs of life on terrestrial planets near the end of their habitable lifetimes". International Journal of Astrobiology. 13 (3): 229–243. arXiv:1310.4841. Bibcode:2014IJAsB..13..229O. doi:10.1017/S1473550413000426. S2CID 119252386. /wiki/ArXiv_(identifier)

  112. O'Malley-James, Jack T.; Greaves, Jane S.; Raven, John A.; Cockell, Charles S. (2014). "Swansong Biosphere II: The final signs of life on terrestrial planets near the end of their habitable lifetimes". International Journal of Astrobiology. 13 (3): 229–243. arXiv:1310.4841. Bibcode:2014IJAsB..13..229O. doi:10.1017/S1473550413000426. S2CID 119252386. /wiki/ArXiv_(identifier)

  113. Strom, Robert G.; Schaber, Gerald G.; Dawson, Douglas D. (25 May 1994). "The global resurfacing of Venus". Journal of Geophysical Research. 99 (E5): 10899–10926. Bibcode:1994JGR....9910899S. doi:10.1029/94JE00388. S2CID 127759323. Archived from the original on 16 September 2020. Retrieved 6 September 2018. https://zenodo.org/record/1231347

  114. Williams, Caroline; Nield, Ted (20 October 2007). "Pangaea, the comeback". New Scientist. Archived from the original on 13 April 2008. Retrieved 2 January 2014. https://web.archive.org/web/20080413162401/http://www.science.org.au/nova/newscientist/104ns_011.htm

  115. Hoffman, Paul F. (November 1992). "Rodinia to Gondwanaland to Pangea to Amasia: alternating kinematics of supercontinental fusion". Atlantic Geology. 28 (3): 284. doi:10.4138/1870. https://journals.lib.unb.ca/index.php/ag/article/view/1870/2234

  116. Williams, Caroline; Nield, Ted (20 October 2007). "Pangaea, the comeback". New Scientist. Archived from the original on 13 April 2008. Retrieved 2 January 2014. https://web.archive.org/web/20080413162401/http://www.science.org.au/nova/newscientist/104ns_011.htm

  117. Perry, Perry; Russel, Thompson (1997). Applied climatology : principles and practice. London, England: Routledge. pp. 127–128. ISBN 9780415141000. 9780415141000

  118. This represents the time by which the event will most probably have happened. It may occur randomly at any time from the present.

  119. Minard, Anne (2009). "Gamma-Ray Burst Caused Mass Extinction?". National Geographic News. Archived from the original on 5 July 2015. Retrieved 27 August 2012. https://archive.today/20150705101800/http://news.nationalgeographic.com/news/2009/04/090403-gamma-ray-extinction.html

  120. "Questions Frequently Asked by the Public About Eclipses". NASA. Archived from the original on 12 March 2010. Retrieved 7 March 2010. https://sunearthday.nasa.gov/2006/faq.php

  121. O'Malley-James, Jack T.; Greaves, Jane S.; Raven, John A.; Cockell, Charles S. (2012). "Swansong Biospheres: Refuges for life and novel microbial biospheres on terrestrial planets near the end of their habitable lifetimes". International Journal of Astrobiology. 12 (2): 99–112. arXiv:1210.5721. Bibcode:2013IJAsB..12...99O. doi:10.1017/S147355041200047X. S2CID 73722450. /wiki/ArXiv_(identifier)

  122. Heath, Martin J.; Doyle, Laurance R. (2009). "Circumstellar Habitable Zones to Ecodynamic Domains: A Preliminary Review and Suggested Future Directions". arXiv:0912.2482 [astro-ph.EP]. /wiki/ArXiv_(identifier)

  123. O'Malley-James, Jack T.; Greaves, Jane S.; Raven, John A.; Cockell, Charles S. (2014). "Swansong Biosphere II: The final signs of life on terrestrial planets near the end of their habitable lifetimes". International Journal of Astrobiology. 13 (3): 229–243. arXiv:1310.4841. Bibcode:2014IJAsB..13..229O. doi:10.1017/S1473550413000426. S2CID 119252386. /wiki/ArXiv_(identifier)

  124. R. J. Graham, Itay Halevy and Dorian Abbot (25 November 2024). "Substantial Extension of the Lifetime of the Terrestrial Biosphere". The Planetary Science Journal. 5 (11): 255. arXiv:2409.10714. Bibcode:2024PSJ.....5..255G. doi:10.3847/PSJ/ad7856. https://doi.org/10.3847%2FPSJ%2Fad7856

  125. O'Malley-James, Jack T.; Greaves, Jane S.; Raven, John A.; Cockell, Charles S. (2014). "Swansong Biosphere II: The final signs of life on terrestrial planets near the end of their habitable lifetimes". International Journal of Astrobiology. 13 (3): 229–243. arXiv:1310.4841. Bibcode:2014IJAsB..13..229O. doi:10.1017/S1473550413000426. S2CID 119252386. /wiki/ArXiv_(identifier)

  126. Ward, Peter D.; Brownlee, Donald (2003). Rare earth : why complex life is uncommon in the universe. New York: Copernicus. pp. 117–128. ISBN 978-0387952895. 978-0387952895

  127. Ward, Peter D.; Brownlee, Donald (2003). Rare earth : why complex life is uncommon in the universe. New York: Copernicus. pp. 117–128. ISBN 978-0387952895. 978-0387952895

  128. Ward, Peter D.; Brownlee, Donald (2003). Rare earth : why complex life is uncommon in the universe. New York: Copernicus. pp. 117–128. ISBN 978-0387952895. 978-0387952895

  129. Heath, Martin J.; Doyle, Laurance R. (2009). "Circumstellar Habitable Zones to Ecodynamic Domains: A Preliminary Review and Suggested Future Directions". arXiv:0912.2482 [astro-ph.EP]. /wiki/ArXiv_(identifier)

  130. O'Malley-James, Jack T.; Greaves, Jane S.; Raven, John A.; Cockell, Charles S. (2014). "Swansong Biosphere II: The final signs of life on terrestrial planets near the end of their habitable lifetimes". International Journal of Astrobiology. 13 (3): 229–243. arXiv:1310.4841. Bibcode:2014IJAsB..13..229O. doi:10.1017/S1473550413000426. S2CID 119252386. /wiki/ArXiv_(identifier)

  131. O'Malley-James, Jack T.; Greaves, Jane S.; Raven, John A.; Cockell, Charles S. (2012). "Swansong Biospheres: Refuges for life and novel microbial biospheres on terrestrial planets near the end of their habitable lifetimes". International Journal of Astrobiology. 12 (2): 99–112. arXiv:1210.5721. Bibcode:2013IJAsB..12...99O. doi:10.1017/S147355041200047X. S2CID 73722450. /wiki/ArXiv_(identifier)

  132. Franck, S.; Bounama, C.; Von Bloh, W. (November 2005). "Causes and timing of future biosphere extinction" (PDF). Biogeosciences Discussions. 2 (6): 1665–1679. Bibcode:2006BGeo....3...85F. doi:10.5194/bgd-2-1665-2005. Archived (PDF) from the original on 31 July 2020. Retrieved 2 September 2019. https://hal.archives-ouvertes.fr/hal-00297823/file/bgd-2-1665-2005.pdf

  133. O'Malley-James, Jack T.; Greaves, Jane S.; Raven, John A.; Cockell, Charles S. (2012). "Swansong Biospheres: Refuges for life and novel microbial biospheres on terrestrial planets near the end of their habitable lifetimes". International Journal of Astrobiology. 12 (2): 99–112. arXiv:1210.5721. Bibcode:2013IJAsB..12...99O. doi:10.1017/S147355041200047X. S2CID 73722450. /wiki/ArXiv_(identifier)

  134. O'Malley-James, Jack T.; Greaves, Jane S.; Raven, John A.; Cockell, Charles S. (2014). "Swansong Biosphere II: The final signs of life on terrestrial planets near the end of their habitable lifetimes". International Journal of Astrobiology. 13 (3): 229–243. arXiv:1310.4841. Bibcode:2014IJAsB..13..229O. doi:10.1017/S1473550413000426. S2CID 119252386. /wiki/ArXiv_(identifier)

  135. Units are short scale. /wiki/Long_and_short_scales#Short_scale

  136. Bounama, Christine; Franck, S.; Von Bloh, David (2001). "The fate of Earth's ocean". Hydrology and Earth System Sciences. 5 (4): 569–575. Bibcode:2001HESS....5..569B. doi:10.5194/hess-5-569-2001. https://doi.org/10.5194%2Fhess-5-569-2001

  137. Antoja, T.; Helmi, A.; Romero-Gómez, M.; Katz, D.; et al. (19 September 2018). "A dynamically young and perturbed Milky Way disk". Nature. 561 (7723): 360–362. arXiv:1804.10196. Bibcode:2018Natur.561..360A. doi:10.1038/s41586-018-0510-7. PMID 30232428. S2CID 52298687. https://www.nature.com/articles/s41586-018-0510-7

  138. O'Malley-James, Jack T.; Greaves, Jane S.; Raven, John A.; Cockell, Charles S. (2012). "Swansong Biospheres: Refuges for life and novel microbial biospheres on terrestrial planets near the end of their habitable lifetimes". International Journal of Astrobiology. 12 (2): 99–112. arXiv:1210.5721. Bibcode:2013IJAsB..12...99O. doi:10.1017/S147355041200047X. S2CID 73722450. /wiki/ArXiv_(identifier)

  139. Schröder, K.-P.; Smith, Robert Connon (1 May 2008). "Distant future of the Sun and Earth revisited". Monthly Notices of the Royal Astronomical Society. 386 (1): 155–163. arXiv:0801.4031. Bibcode:2008MNRAS.386..155S. doi:10.1111/j.1365-2966.2008.13022.x. S2CID 10073988. https://doi.org/10.1111%2Fj.1365-2966.2008.13022.x

  140. Brownlee 2010, p. 95. - Brownlee, Donald E. (2010). "Planetary habitability on astronomical time scales". In Schrijver, Carolus J.; Siscoe, George L. (eds.). Heliophysics: Evolving Solar Activity and the Climates of Space and Earth. Cambridge University Press. ISBN 978-0-521-11294-9. https://books.google.com/books?id=M8NwTYEl0ngC

  141. Brownlee 2010, p. 79. - Brownlee, Donald E. (2010). "Planetary habitability on astronomical time scales". In Schrijver, Carolus J.; Siscoe, George L. (eds.). Heliophysics: Evolving Solar Activity and the Climates of Space and Earth. Cambridge University Press. ISBN 978-0-521-11294-9. https://books.google.com/books?id=M8NwTYEl0ngC

  142. Li, King-Fai; Pahlevan, Kaveh; Kirschvink, Joseph L.; Yung, Luk L. (2009). "Atmospheric pressure as a natural climate regulator for a terrestrial planet with a biosphere". Proceedings of the National Academy of Sciences of the United States of America. 106 (24): 9576–9579. Bibcode:2009PNAS..106.9576L. doi:10.1073/pnas.0809436106. PMC 2701016. PMID 19487662. https://www.ncbi.nlm.nih.gov/pmc/articles/PMC2701016

  143. Caldeira, Ken; Kasting, James F. (1992). "The life span of the biosphere revisited". Nature. 360 (6406): 721–723. Bibcode:1992Natur.360..721C. doi:10.1038/360721a0. PMID 11536510. S2CID 4360963. /wiki/Bibcode_(identifier)

  144. Franck, S. (2000). "Reduction of biosphere life span as a consequence of geodynamics". Tellus B. 52 (1): 94–107. Bibcode:2000TellB..52...94F. doi:10.1034/j.1600-0889.2000.00898.x. /wiki/Bibcode_(identifier)

  145. Lenton, Timothy M.; von Bloh, Werner (2001). "Biotic feedback extends the life span of the biosphere". Geophysical Research Letters. 28 (9): 1715–1718. Bibcode:2001GeoRL..28.1715L. doi:10.1029/2000GL012198. https://doi.org/10.1029%2F2000GL012198

  146. Franck, S.; Bounama, C.; Von Bloh, W. (November 2005). "Causes and timing of future biosphere extinction" (PDF). Biogeosciences Discussions. 2 (6): 1665–1679. Bibcode:2006BGeo....3...85F. doi:10.5194/bgd-2-1665-2005. Archived (PDF) from the original on 31 July 2020. Retrieved 2 September 2019. https://hal.archives-ouvertes.fr/hal-00297823/file/bgd-2-1665-2005.pdf

  147. Lari, Giacomo; Saillenfest, Melaine; Fenucci, Marco (2020). "Long-term evolution of the Galilean satellites: the capture of Callisto into resonance". Astronomy & Astrophysics. 639: A40. arXiv:2001.01106. Bibcode:2020A&A...639A..40L. doi:10.1051/0004-6361/202037445. S2CID 209862163. Retrieved 1 August 2022. https://www.aanda.org/articles/aa/full_html/2020/07/aa37445-20/aa37445-20.html

  148. Franck, S.; Bounama, C.; Von Bloh, W. (November 2005). "Causes and timing of future biosphere extinction" (PDF). Biogeosciences Discussions. 2 (6): 1665–1679. Bibcode:2006BGeo....3...85F. doi:10.5194/bgd-2-1665-2005. Archived (PDF) from the original on 31 July 2020. Retrieved 2 September 2019. https://hal.archives-ouvertes.fr/hal-00297823/file/bgd-2-1665-2005.pdf

  149. Kargel, J. S. (2004). Mars: a warmer, wetter planet. Springer-Praxis books in astronomy and space sciences. London; New York : Chichester: Springer; Praxis. p. 509. ISBN 978-1-85233-568-7. Archived from the original on 27 May 2021. Retrieved 29 October 2007. 978-1-85233-568-7

  150. Neron de Surgey, O.; Laskar, J. (1996). "On the Long Term Evolution of the Spin of the Earth". Astronomy and Astrophysics. 318: 975. Bibcode:1997A&A...318..975N. /wiki/Bibcode_(identifier)

  151. O'Malley-James, Jack T.; Greaves, Jane S.; Raven, John A.; Cockell, Charles S. (2012). "Swansong Biospheres: Refuges for life and novel microbial biospheres on terrestrial planets near the end of their habitable lifetimes". International Journal of Astrobiology. 12 (2): 99–112. arXiv:1210.5721. Bibcode:2013IJAsB..12...99O. doi:10.1017/S147355041200047X. S2CID 73722450. /wiki/ArXiv_(identifier)

  152. Franck, S.; Bounama, C.; Von Bloh, W. (November 2005). "Causes and timing of future biosphere extinction" (PDF). Biogeosciences Discussions. 2 (6): 1665–1679. Bibcode:2006BGeo....3...85F. doi:10.5194/bgd-2-1665-2005. Archived (PDF) from the original on 31 July 2020. Retrieved 2 September 2019. https://hal.archives-ouvertes.fr/hal-00297823/file/bgd-2-1665-2005.pdf

  153. Adams 2008, pp. 33–47. - Adams, Fred C. (2008). "Long term astrophysical processes". In Bostrom, Nick; Ćirković, Milan M. (eds.). Global catastrophic risks. Oxford University Press. ISBN 978-0-19-857050-9. https://books.google.com/books?id=-Jxc88RuJhgC&pg=PA33

  154. Cox, T. J.; Loeb, Abraham (2007). "The collision between the Milky Way and Andromeda". Monthly Notices of the Royal Astronomical Society. 386 (1): 461–474. arXiv:0705.1170. Bibcode:2008MNRAS.386..461C. doi:10.1111/j.1365-2966.2008.13048.x. S2CID 14964036. https://doi.org/10.1111%2Fj.1365-2966.2008.13048.x

  155. Li, King-Fai; Pahlevan, Kaveh; Kirschvink, Joseph L.; Yung, Yuk L. (16 June 2009). "Atmospheric pressure as a natural climate regulator for a terrestrial planet with a biosphere". Proceedings of the National Academy of Sciences of the United States of America. 106 (24): 9576–9579. Bibcode:2009PNAS..106.9576L. doi:10.1073/pnas.0809436106. PMC 2701016. PMID 19487662. https://www.ncbi.nlm.nih.gov/pmc/articles/PMC2701016

  156. Schröder, K.-P.; Smith, Robert Connon (1 May 2008). "Distant future of the Sun and Earth revisited". Monthly Notices of the Royal Astronomical Society. 386 (1): 155–163. arXiv:0801.4031. Bibcode:2008MNRAS.386..155S. doi:10.1111/j.1365-2966.2008.13022.x. S2CID 10073988. https://doi.org/10.1111%2Fj.1365-2966.2008.13022.x

  157. O'Malley-James, Jack T.; Greaves, Jane S.; Raven, John A.; Cockell, Charles S. (2012). "Swansong Biospheres: Refuges for life and novel microbial biospheres on terrestrial planets near the end of their habitable lifetimes". International Journal of Astrobiology. 12 (2): 99–112. arXiv:1210.5721. Bibcode:2013IJAsB..12...99O. doi:10.1017/S147355041200047X. S2CID 73722450. /wiki/ArXiv_(identifier)

  158. Adams 2008, pp. 33–47. - Adams, Fred C. (2008). "Long term astrophysical processes". In Bostrom, Nick; Ćirković, Milan M. (eds.). Global catastrophic risks. Oxford University Press. ISBN 978-0-19-857050-9. https://books.google.com/books?id=-Jxc88RuJhgC&pg=PA33

  159. O'Malley-James, Jack T.; Greaves, Jane S.; Raven, John A.; Cockell, Charles S. (2012). "Swansong Biospheres: Refuges for life and novel microbial biospheres on terrestrial planets near the end of their habitable lifetimes". International Journal of Astrobiology. 12 (2): 99–112. arXiv:1210.5721. Bibcode:2013IJAsB..12...99O. doi:10.1017/S147355041200047X. S2CID 73722450. /wiki/ArXiv_(identifier)

  160. Adams 2008, pp. 33–47. - Adams, Fred C. (2008). "Long term astrophysical processes". In Bostrom, Nick; Ćirković, Milan M. (eds.). Global catastrophic risks. Oxford University Press. ISBN 978-0-19-857050-9. https://books.google.com/books?id=-Jxc88RuJhgC&pg=PA33

  161. Waszek, Lauren; Irving, Jessica; Deuss, Arwen (20 February 2011). "Reconciling the Hemispherical Structure of Earth's Inner Core With its Super-Rotation". Nature Geoscience. 4 (4): 264–267. Bibcode:2011NatGe...4..264W. doi:10.1038/ngeo1083. /wiki/Bibcode_(identifier)

  162. McDonough, W. F. (2004). "Compositional Model for the Earth's Core". Treatise on Geochemistry. Vol. 2. pp. 547–568. Bibcode:2003TrGeo...2..547M. doi:10.1016/B0-08-043751-6/02015-6. ISBN 978-0080437514. 978-0080437514

  163. Meadows, A. J. (2007). The Future of the Universe. Springer. pp. 81–83. ISBN 9781852339463. 9781852339463

  164. Luhmann, J. G.; Johnson, R. E.; Zhang, M. H. G. (1992). "Evolutionary impact of sputtering of the Martian atmosphere by O+ pickup ions". Geophysical Research Letters. 19 (21): 2151–2154. Bibcode:1992GeoRL..19.2151L. doi:10.1029/92GL02485. /wiki/Geophysical_Research_Letters

  165. Shlermeler, Quirin (3 March 2005). "Solar wind hammers the ozone layer". News@nature. doi:10.1038/news050228-12. /wiki/Doi_(identifier)

  166. This represents the time by which the event will most probably have happened. It may occur randomly at any time from the present.

  167. Adams 2008, pp. 33–44. - Adams, Fred C. (2008). "Long term astrophysical processes". In Bostrom, Nick; Ćirković, Milan M. (eds.). Global catastrophic risks. Oxford University Press. ISBN 978-0-19-857050-9. https://books.google.com/books?id=-Jxc88RuJhgC&pg=PA33

  168. This represents the time by which the event will most probably have happened. It may occur randomly at any time from the present.

  169. "Study: Earth May Collide With Another Planet". Fox News Channel. 11 June 2009. Archived from the original on 4 November 2012. Retrieved 8 September 2011. https://www.foxnews.com/story/study-earth-may-collide-with-another-planet

  170. Shiga, David (23 April 2008). "Solar system could go haywire before the Sun dies". New Scientist. https://www.newscientist.com/article/dn13757-solar-system-could-go-haywire-before-the-sun-dies/

  171. Brownlee 2010, p. 95. - Brownlee, Donald E. (2010). "Planetary habitability on astronomical time scales". In Schrijver, Carolus J.; Siscoe, George L. (eds.). Heliophysics: Evolving Solar Activity and the Climates of Space and Earth. Cambridge University Press. ISBN 978-0-521-11294-9. https://books.google.com/books?id=M8NwTYEl0ngC

  172. Li, King-Fai; Pahlevan, Kaveh; Kirschvink, Joseph L.; Yung, Yuk L. (16 June 2009). "Atmospheric pressure as a natural climate regulator for a terrestrial planet with a biosphere". Proceedings of the National Academy of Sciences of the United States of America. 106 (24): 9576–9579. Bibcode:2009PNAS..106.9576L. doi:10.1073/pnas.0809436106. PMC 2701016. PMID 19487662. https://www.ncbi.nlm.nih.gov/pmc/articles/PMC2701016

  173. Guinan, E. F.; Ribas, I. (2002). Montesinos, Benjamin; Gimenez, Alvaro; Guinan, Edward F. (eds.). "Our Changing Sun: The Role of Solar Nuclear Evolution and Magnetic Activity on Earth's Atmosphere and Climate". ASP Conference Proceedings. 269: 85–106. Bibcode:2002ASPC..269...85G. /wiki/Bibcode_(identifier)

  174. Kasting, James F. (June 1988). "Runaway and moist greenhouse atmospheres and the evolution of earth and Venus". Icarus. 74 (3): 472–494. Bibcode:1988Icar...74..472K. doi:10.1016/0019-1035(88)90116-9. PMID 11538226. Archived from the original on 7 December 2019. Retrieved 6 September 2018. https://zenodo.org/record/1253896

  175. Chyba, C. F.; Jankowski, D. G.; Nicholson, P. D. (1989). "Tidal Evolution in the Neptune-Triton System". Astronomy and Astrophysics. 219 (1–2): 23. Bibcode:1989A&A...219L..23C. /wiki/Astronomy_and_Astrophysics

  176. Finkleman, David; Allen, Steve; Seago, John; Seaman, Rob; et al. (June 2011). "The Future of Time: UTC and the Leap Second". American Scientist. 99 (4): 312. arXiv:1106.3141. Bibcode:2011arXiv1106.3141F. doi:10.1511/2011.91.312. S2CID 118403321. /wiki/ArXiv_(identifier)

  177. Kargel, J. S. (2004). Mars: a warmer, wetter planet. Springer-Praxis books in astronomy and space sciences. London; New York : Chichester: Springer; Praxis. p. 509. ISBN 978-1-85233-568-7. Archived from the original on 27 May 2021. Retrieved 29 October 2007. 978-1-85233-568-7

  178. Cox, T. J.; Loeb, Abraham (2007). "The collision between the Milky Way and Andromeda". Monthly Notices of the Royal Astronomical Society. 386 (1): 461–474. arXiv:0705.1170. Bibcode:2008MNRAS.386..461C. doi:10.1111/j.1365-2966.2008.13048.x. S2CID 14964036. https://doi.org/10.1111%2Fj.1365-2966.2008.13048.x

  179. Cox, T. J.; Loeb, Abraham (2007). "The collision between the Milky Way and Andromeda". Monthly Notices of the Royal Astronomical Society. 386 (1): 461–474. arXiv:0705.1170. Bibcode:2008MNRAS.386..461C. doi:10.1111/j.1365-2966.2008.13048.x. S2CID 14964036. https://doi.org/10.1111%2Fj.1365-2966.2008.13048.x

  180. Cain, Fraser (2007). "When Our Galaxy Smashes into Andromeda, What Happens to the Sun?". Universe Today. Archived from the original on 17 May 2007. Retrieved 16 May 2007. http://www.universetoday.com/2007/05/10/when-our-galaxy-smashes-into-andromeda-what-happens-to-the-sun/

  181. "NASA's Hubble Shows Milky Way is Destined for Head-On Collision". NASA. 31 May 2012. Archived from the original on 30 April 2020. Retrieved 13 October 2012. https://www.nasa.gov/mission_pages/hubble/science/milky-way-collide.html

  182. Dowd, Maureen (29 May 2012). "Andromeda Is Coming!". The New York Times. Archived from the original on 8 March 2021. Retrieved 9 January 2014. [NASA's David Morrison] explained that the Andromeda-Milky Way collision would just be two great big fuzzy balls of stars and mostly empty space passing through each other harmlessly over the course of millions of years. /wiki/Maureen_Dowd

  183. Braine, J.; Lisenfeld, U.; Duc, P. A.; Brinks, E.; et al. (2004). "Colliding molecular clouds in head-on galaxy collisions". Astronomy and Astrophysics. 418 (2): 419–428. arXiv:astro-ph/0402148. Bibcode:2004A&A...418..419B. doi:10.1051/0004-6361:20035732. S2CID 15928576. /wiki/ArXiv_(identifier)

  184. Schroder, K. P.; Smith, Robert Connon (2008). "Distant Future of the Sun and Earth Revisited". Monthly Notices of the Royal Astronomical Society. 386 (1): 155–163. arXiv:0801.4031. Bibcode:2008MNRAS.386..155S. doi:10.1111/j.1365-2966.2008.13022.x. S2CID 10073988. https://doi.org/10.1111%2Fj.1365-2966.2008.13022.x

  185. Kargel, J. S. (2004). Mars: a warmer, wetter planet. Springer-Praxis books in astronomy and space sciences. London; New York : Chichester: Springer; Praxis. p. 509. ISBN 978-1-85233-568-7. Archived from the original on 27 May 2021. Retrieved 29 October 2007. 978-1-85233-568-7

  186. Taylor, David. "The End Of The Sun". Archived from the original on 12 May 2021. Retrieved 29 July 2021. https://faculty.wcas.northwestern.edu/~infocom/The%20Website/end.html

  187. Kargel, J. S. (2004). Mars: a warmer, wetter planet. Springer-Praxis books in astronomy and space sciences. London; New York : Chichester: Springer; Praxis. p. 509. ISBN 978-1-85233-568-7. Archived from the original on 27 May 2021. Retrieved 29 October 2007. 978-1-85233-568-7

  188. Schroder, K. P.; Smith, Robert Connon (2008). "Distant Future of the Sun and Earth Revisited". Monthly Notices of the Royal Astronomical Society. 386 (1): 155–163. arXiv:0801.4031. Bibcode:2008MNRAS.386..155S. doi:10.1111/j.1365-2966.2008.13022.x. S2CID 10073988. https://doi.org/10.1111%2Fj.1365-2966.2008.13022.x

  189. See the 2001 paper by Rybicki, K. R. and Denis, C. However, according to the latest calculations, this happens with a very high degree of certainty.

  190. Powell, David (22 January 2007). "Earth's Moon Destined to Disintegrate". Space.com. Tech Media Network. Archived from the original on 27 June 2019. Retrieved 1 June 2010. http://www.space.com/scienceastronomy/070122_temporary_moon.html

  191. Lorenz, Ralph D.; Lunine, Jonathan I.; McKay, Christopher P. (15 November 1997). "Titan under a red giant sun: A new kind of "habitable" moon" (PDF). Geophysical Research Letters. 24 (22): 2905–2908. Bibcode:1997GeoRL..24.2905L. CiteSeerX 10.1.1.683.8827. doi:10.1029/97GL52843. ISSN 0094-8276. PMID 11542268. S2CID 14172341. Archived (PDF) from the original on 23 December 2018. Retrieved 21 March 2008. http://www.lpl.arizona.edu/~rlorenz/redgiant.pdf

  192. Rybicki, K; Denis, C. (May 2001). "On the Final Destiny of the Earth and the Solar System". Icarus. 151 (1): 130–137. Bibcode:2001Icar..151..130R. doi:10.1006/icar.2001.6591. /wiki/Bibcode_(identifier)

  193. Schroder, K. P.; Smith, Robert Connon (2008). "Distant Future of the Sun and Earth Revisited". Monthly Notices of the Royal Astronomical Society. 386 (1): 155–163. arXiv:0801.4031. Bibcode:2008MNRAS.386..155S. doi:10.1111/j.1365-2966.2008.13022.x. S2CID 10073988. https://doi.org/10.1111%2Fj.1365-2966.2008.13022.x

  194. Schroder, K. P.; Smith, Robert Connon (2008). "Distant Future of the Sun and Earth Revisited". Monthly Notices of the Royal Astronomical Society. 386 (1): 155–163. arXiv:0801.4031. Bibcode:2008MNRAS.386..155S. doi:10.1111/j.1365-2966.2008.13022.x. S2CID 10073988. https://doi.org/10.1111%2Fj.1365-2966.2008.13022.x

  195. Balick, Bruce. "Planetary Nebulae and the Future of the Solar System". University of Washington. Archived from the original on 19 December 2008. Retrieved 23 June 2006. https://web.archive.org/web/20081219010229/http://www.astro.washington.edu/balick/WFPC2/

  196. Kalirai, Jasonjot S.; Hansen, Brad M. S.; Kelson, Daniel D.; Reitzel, David B.; et al. (March 2008). "The Initial-Final Mass Relation: Direct Constraints at the Low-Mass End". The Astrophysical Journal. 676 (1): 594–609. arXiv:0706.3894. Bibcode:2008ApJ...676..594K. doi:10.1086/527028. S2CID 10729246. /wiki/ArXiv_(identifier)

  197. Kalirai et al. 2008, p. 16. Based upon the weighted least-squares best fit with the initial mass equal to a solar mass. - Kalirai, Jasonjot S.; Hansen, Brad M. S.; Kelson, Daniel D.; Reitzel, David B.; et al. (March 2008). "The Initial-Final Mass Relation: Direct Constraints at the Low-Mass End". The Astrophysical Journal. 676 (1): 594–609. arXiv:0706.3894. Bibcode:2008ApJ...676..594K. doi:10.1086/527028. S2CID 10729246. https://arxiv.org/abs/0706.3894

  198. "Universe May End in a Big Rip". CERN Courier. 1 May 2003. Archived from the original on 24 October 2011. Retrieved 22 July 2011. http://cerncourier.com/cws/article/cern/28845

  199. "Ask Ethan: Could The Universe Be Torn Apart In A Big Rip?". Forbes. Archived from the original on 2 August 2021. Retrieved 26 January 2021. https://www.forbes.com/sites/startswithabang/2018/06/30/ask-ethan-could-the-universe-be-torn-apart-in-a-big-rip/

  200. Caldwell, Robert R.; Kamionkowski, Marc; Weinberg, Nevin N. (2003). "Phantom Energy and Cosmic Doomsday". Physical Review Letters. 91 (7): 071301. arXiv:astro-ph/0302506. Bibcode:2003PhRvL..91g1301C. doi:10.1103/PhysRevLett.91.071301. PMID 12935004. S2CID 119498512. /wiki/ArXiv_(identifier)

  201. Vikhlinin, A.; Kravtsov, A.V.; Burenin, R.A.; Ebeling, H.; et al. (2009). "Chandra Cluster Cosmology Project III: Cosmological Parameter Constraints". The Astrophysical Journal. 692 (2): 1060–1074. arXiv:0812.2720. Bibcode:2009ApJ...692.1060V. doi:10.1088/0004-637X/692/2/1060. S2CID 15719158. /wiki/ArXiv_(identifier)

  202. The Planck Collaboration (2020). "Planck 2018 results. VI. Cosmological parameters". Astronomy and Astrophysics. 641: A6. arXiv:1807.06209. Bibcode:2020A&A...641A...6P. doi:10.1051/0004-6361/201833910. S2CID 119335614. /wiki/ArXiv_(identifier)

  203. Murray, C. D. & Dermott, S. F. (1999). Solar System Dynamics. Cambridge University Press. p. 184. ISBN 978-0-521-57295-8. Archived from the original on 1 August 2020. Retrieved 27 March 2016. 978-0-521-57295-8

  204. Dickinson, Terence (1993). From the Big Bang to Planet X. Camden East, Ontario: Camden House. pp. 79–81. ISBN 978-0-921820-71-0. 978-0-921820-71-0

  205. Canup, Robin M.; Righter, Kevin (2000). Origin of the Earth and Moon. The University of Arizona space science series. Vol. 30. University of Arizona Press. pp. 176–177. ISBN 978-0-8165-2073-2. Archived from the original on 1 August 2020. Retrieved 27 March 2016. 978-0-8165-2073-2

  206. Dorminey, Bruce (31 January 2017). "Earth and Moon May Be on Long-Term Collision Course". Forbes. Archived from the original on 1 February 2017. Retrieved 11 February 2017. https://www.forbes.com/sites/brucedorminey/2017/01/31/earth-and-moon-may-be-on-long-term-collision-course/

  207. "The Local Group of Galaxies". Students for the Exploration and Development of Space. Archived from the original on 7 January 2019. Retrieved 2 October 2009. http://messier.seds.org/more/local.html

  208. Adams, Fred C.; Laughlin, Gregory (1997). "A dying universe: the long-term fate and evolution of astrophysical objects". Reviews of Modern Physics. 69 (2): 337–372. arXiv:astro-ph/9701131. Bibcode:1997RvMP...69..337A. doi:10.1103/RevModPhys.69.337. S2CID 12173790. /wiki/ArXiv_(identifier)

  209. Loeb, Abraham (2011). "Cosmology with Hypervelocity Stars". Journal of Cosmology and Astroparticle Physics. 2011 (4). Harvard University: 023. arXiv:1102.0007. Bibcode:2011JCAP...04..023L. doi:10.1088/1475-7516/2011/04/023. S2CID 118750775. /wiki/ArXiv_(identifier)

  210. Ord, Toby (5 May 2021). "The Edges of Our Universe". arXiv:2104.01191 [gr-qc]. /wiki/ArXiv_(identifier)

  211. Ord, Toby (5 May 2021). "The Edges of Our Universe". arXiv:2104.01191 [gr-qc]. /wiki/ArXiv_(identifier)

  212. Busha, Michael T.; Adams, Fred C.; Wechsler, Risa H.; Evrard, August E. (20 October 2003). "Future Evolution of Structure in an Accelerating Universe". The Astrophysical Journal. 596 (2): 713–724. arXiv:astro-ph/0305211. doi:10.1086/378043. ISSN 0004-637X. S2CID 15764445. /wiki/ArXiv_(identifier)

  213. Adams, F. C.; Graves, G. J. M.; Laughlin, G. (December 2004). García-Segura, G.; Tenorio-Tagle, G.; Franco, J.; Yorke, H. W. (eds.). "Gravitational Collapse: From Massive Stars to Planets. / First Astrophysics meeting of the Observatorio Astronomico Nacional. / A meeting to celebrate Peter Bodenheimer for his outstanding contributions to Astrophysics: Red Dwarfs and the End of the Main Sequence". Revista Mexicana de Astronomía y Astrofísica, Serie de Conferencias. 22: 46–49. Bibcode:2004RMxAC..22...46A. See Fig. 3. /wiki/Bibcode_(identifier)

  214. Adams, Fred C.; Laughlin, Gregory (1997). "A dying universe: the long-term fate and evolution of astrophysical objects". Reviews of Modern Physics. 69 (2): 337–372. arXiv:astro-ph/9701131. Bibcode:1997RvMP...69..337A. doi:10.1103/RevModPhys.69.337. S2CID 12173790. /wiki/ArXiv_(identifier)

  215. Loeb, Abraham (2011). "Cosmology with Hypervelocity Stars". Journal of Cosmology and Astroparticle Physics. 2011 (4). Harvard University: 023. arXiv:1102.0007. Bibcode:2011JCAP...04..023L. doi:10.1088/1475-7516/2011/04/023. S2CID 118750775. /wiki/ArXiv_(identifier)

  216. Busha, Michael T.; Adams, Fred C.; Wechsler, Risa H.; Evrard, August E. (20 October 2003). "Future Evolution of Structure in an Accelerating Universe". The Astrophysical Journal. 596 (2): 713–724. arXiv:astro-ph/0305211. doi:10.1086/378043. ISSN 0004-637X. S2CID 15764445. /wiki/ArXiv_(identifier)

  217. Ord, Toby (5 May 2021). "The Edges of Our Universe". arXiv:2104.01191 [gr-qc]. /wiki/ArXiv_(identifier)

  218. Krauss, Lawrence M.; Starkman, Glenn D. (March 2000). "Life, The Universe, and Nothing: Life and Death in an Ever-Expanding Universe". The Astrophysical Journal. 531 (1): 22–30. arXiv:astro-ph/9902189. Bibcode:2000ApJ...531...22K. doi:10.1086/308434. ISSN 0004-637X. S2CID 18442980. /wiki/Lawrence_Krauss

  219. Adams, Fred C.; Laughlin, Gregory; Graves, Genevieve J. M. (2004). "RED Dwarfs and the End of The Main Sequence" (PDF). Revista Mexicana de Astronomía y Astrofísica, Serie de Conferencias. 22: 46–49. Archived (PDF) from the original on 23 December 2018. Retrieved 21 May 2016. http://www.astroscu.unam.mx/rmaa/RMxAC..22/PDF/RMxAC..22_adams.pdf

  220. Loeb, Abraham; Batista, Rafael; Sloan, W. (2016). "Relative Likelihood for Life as a Function of Cosmic Time". Journal of Cosmology and Astroparticle Physics. 2016 (8): 040. arXiv:1606.08448. Bibcode:2016JCAP...08..040L. doi:10.1088/1475-7516/2016/08/040. S2CID 118489638. /wiki/ArXiv_(identifier)

  221. "Why the Smallest Stars Stay Small". Sky & Telescope (22). November 1997.

  222. Adams, F. C.; Bodenheimer, P.; Laughlin, G. (2005). "M dwarfs: planet formation and long term evolution". Astronomische Nachrichten. 326 (10): 913–919. Bibcode:2005AN....326..913A. doi:10.1002/asna.200510440. https://doi.org/10.1002%2Fasna.200510440

  223. Tayler, Roger John (1993). Galaxies, Structure and Evolution (2nd ed.). Cambridge University Press. p. 92. ISBN 978-0521367103. 978-0521367103

  224. Adams, Fred C.; Laughlin, Gregory (1997). "A dying universe: the long-term fate and evolution of astrophysical objects". Reviews of Modern Physics. 69 (2): 337–372. arXiv:astro-ph/9701131. Bibcode:1997RvMP...69..337A. doi:10.1103/RevModPhys.69.337. S2CID 12173790. /wiki/ArXiv_(identifier)

  225. Adams, Fred; Laughlin, Greg (1999). The Five Ages of the Universe. New York: The Free Press. ISBN 978-0684854229. 978-0684854229

  226. Busha, Michael T.; Adams, Fred C.; Wechsler, Risa H.; Evrard, August E. (20 October 2003). "Future Evolution of Structure in an Accelerating Universe". The Astrophysical Journal. 596 (2): 713–724. arXiv:astro-ph/0305211. doi:10.1086/378043. ISSN 0004-637X. S2CID 15764445. /wiki/ArXiv_(identifier)

  227. Adams, Fred C.; Laughlin, Gregory (1997). "A dying universe: the long-term fate and evolution of astrophysical objects". Reviews of Modern Physics. 69 (2): 337–372. arXiv:astro-ph/9701131. Bibcode:1997RvMP...69..337A. doi:10.1103/RevModPhys.69.337. S2CID 12173790. /wiki/ArXiv_(identifier)

  228. Adams, Fred C.; Laughlin, Gregory (1997). "A dying universe: the long-term fate and evolution of astrophysical objects". Reviews of Modern Physics. 69 (2): 337–372. arXiv:astro-ph/9701131. Bibcode:1997RvMP...69..337A. doi:10.1103/RevModPhys.69.337. S2CID 12173790. /wiki/ArXiv_(identifier)

  229. Adams, Fred C.; Laughlin, Gregory (1997). "A dying universe: the long-term fate and evolution of astrophysical objects". Reviews of Modern Physics. 69 (2): 337–372. arXiv:astro-ph/9701131. Bibcode:1997RvMP...69..337A. doi:10.1103/RevModPhys.69.337. S2CID 12173790. /wiki/ArXiv_(identifier)

  230. Barrow, John D.; Tipler, Frank J. (19 May 1988). The Anthropic Cosmological Principle. foreword by John A. Wheeler. Oxford: Oxford University Press. ISBN 978-0192821478. LC 87-28148. Archived from the original on 1 August 2020. Retrieved 27 March 2016. 978-0192821478

  231. Adams, Fred C.; Laughlin, Gregory (1997). "A dying universe: the long-term fate and evolution of astrophysical objects". Reviews of Modern Physics. 69 (2): 337–372. arXiv:astro-ph/9701131. Bibcode:1997RvMP...69..337A. doi:10.1103/RevModPhys.69.337. S2CID 12173790. /wiki/ArXiv_(identifier)

  232. Adams, Fred; Laughlin, Greg (1999). The Five Ages of the Universe. New York: The Free Press. pp. 85–87. ISBN 978-0684854229. 978-0684854229

  233. Dyson, Freeman (1979). "Time Without End: Physics and Biology in an Open Universe". Reviews of Modern Physics. 51 (3): 447–460. Bibcode:1979RvMP...51..447D. doi:10.1103/RevModPhys.51.447. Archived from the original on 5 July 2008. Retrieved 5 July 2008. /wiki/Freeman_Dyson

  234. Dyson, Freeman (1979). "Time Without End: Physics and Biology in an Open Universe". Reviews of Modern Physics. 51 (3): 447–460. Bibcode:1979RvMP...51..447D. doi:10.1103/RevModPhys.51.447. Archived from the original on 5 July 2008. Retrieved 5 July 2008. /wiki/Freeman_Dyson

  235. Baez, John C. (7 February 2016). "The End of the Universe". math.ucr.edu. Archived from the original on 30 May 2009. Retrieved 13 February 2021. /wiki/John_C._Baez

  236. Adams, Fred C.; Laughlin, Gregory (1997). "A dying universe: the long-term fate and evolution of astrophysical objects". Reviews of Modern Physics. 69 (2): 337–372. arXiv:astro-ph/9701131. Bibcode:1997RvMP...69..337A. doi:10.1103/RevModPhys.69.337. S2CID 12173790. /wiki/ArXiv_(identifier)

  237. Nishino H, Clark S, Abe K, Hayato Y, et al. (Super-K Collaboration) (2009). "Search for Proton Decay via p+ → e+π0 and p+ → μ+π0 in a Large Water Cherenkov Detector". Physical Review Letters. 102 (14): 141801. arXiv:0903.0676. Bibcode:2009PhRvL.102n1801N. doi:10.1103/PhysRevLett.102.141801. PMID 19392425. S2CID 32385768.{{cite journal}}: CS1 maint: overridden setting (link) /wiki/Super-Kamiokande

  238. Around 264 half-lives. Tyson et al. employ the computation with a different value for half-life.

  239. Adams, Fred C.; Laughlin, Gregory (1997). "A dying universe: the long-term fate and evolution of astrophysical objects". Reviews of Modern Physics. 69 (2): 337–372. arXiv:astro-ph/9701131. Bibcode:1997RvMP...69..337A. doi:10.1103/RevModPhys.69.337. S2CID 12173790. /wiki/ArXiv_(identifier)

  240. Adams, Fred C.; Laughlin, Gregory (1997). "A dying universe: the long-term fate and evolution of astrophysical objects". Reviews of Modern Physics. 69 (2): 337–372. arXiv:astro-ph/9701131. Bibcode:1997RvMP...69..337A. doi:10.1103/RevModPhys.69.337. S2CID 12173790. /wiki/ArXiv_(identifier)

  241. Adams, Fred C.; Laughlin, Gregory (1997). "A dying universe: the long-term fate and evolution of astrophysical objects". Reviews of Modern Physics. 69 (2): 337–372. arXiv:astro-ph/9701131. Bibcode:1997RvMP...69..337A. doi:10.1103/RevModPhys.69.337. S2CID 12173790. /wiki/ArXiv_(identifier)

  242. Adams, Fred; Laughlin, Greg (1999). The Five Ages of the Universe. New York: The Free Press. ISBN 978-0684854229. 978-0684854229

  243. Page, Don N. (1976). "Particle Emission Rates from a Black Hole: Massless Particles from an Uncharged, Nonrotating Hole". Physical Review D. 13 (2): 198–206. Bibcode:1976PhRvD..13..198P. doi:10.1103/PhysRevD.13.198. /wiki/Bibcode_(identifier)

  244. Dyson, Freeman (1979). "Time Without End: Physics and Biology in an Open Universe". Reviews of Modern Physics. 51 (3): 447–460. Bibcode:1979RvMP...51..447D. doi:10.1103/RevModPhys.51.447. Archived from the original on 5 July 2008. Retrieved 5 July 2008. /wiki/Freeman_Dyson

  245. Page, Don N. (1976). "Particle Emission Rates from a Black Hole: Massless Particles from an Uncharged, Nonrotating Hole". Physical Review D. 13 (2): 198–206. Bibcode:1976PhRvD..13..198P. doi:10.1103/PhysRevD.13.198. /wiki/Bibcode_(identifier)

  246. Overbye, Denis (16 September 2015). "More Evidence for Coming Black Hole Collision". The New York Times. https://www.nytimes.com/2015/09/22/science/space/more-evidence-for-coming-black-hole-collision.html

  247. Page, Don N. (1976). "Particle Emission Rates from a Black Hole: Massless Particles from an Uncharged, Nonrotating Hole". Physical Review D. 13 (2): 198–206. Bibcode:1976PhRvD..13..198P. doi:10.1103/PhysRevD.13.198. /wiki/Bibcode_(identifier)

  248. L., Logan Richard (2021). "Black holes can help us answer many long-asked questions". Microscopy UK – Science & Education. Micscape. Retrieved 30 May 2023. When galaxies collide, the supermassive black holes in the central contract eventually find their way into the centre of the newly created galaxy where they are ultimately pulled together. https://www.microscopy-uk.net/black-holes-can-help-us-answer-many-long-asked-questions/

  249. Frautschi, S. (1982). "Entropy in an expanding universe". Science. 217 (4560): 593–599. Bibcode:1982Sci...217..593F. doi:10.1126/science.217.4560.593. PMID 17817517. S2CID 27717447. p. 596: table 1 and section "black hole decay" and previous sentence on that page: "Since we have assumed a maximum scale of gravitational binding – for instance, superclusters of galaxies – black hole formation eventually comes to an end in our model, with masses of up to 1014M☉ ... the timescale for black holes to radiate away all their energy ranges ... to 10106 years for black holes of up to 1014M☉" /wiki/Bibcode_(identifier)

  250. Page, Don N. (1976). "Particle Emission Rates from a Black Hole: Massless Particles from an Uncharged, Nonrotating Hole". Physical Review D. 13 (2): 198–206. Bibcode:1976PhRvD..13..198P. doi:10.1103/PhysRevD.13.198. /wiki/Bibcode_(identifier)

  251. Adams, Fred C.; Laughlin, Gregory (1997). "A dying universe: the long-term fate and evolution of astrophysical objects". Reviews of Modern Physics. 69 (2): 337–372. arXiv:astro-ph/9701131. Bibcode:1997RvMP...69..337A. doi:10.1103/RevModPhys.69.337. S2CID 12173790. /wiki/ArXiv_(identifier)

  252. Adams, Fred; Laughlin, Greg (1999). The Five Ages of the Universe. New York: The Free Press. ISBN 978-0684854229. 978-0684854229

  253. Andreassen, Anders; Frost, William; Schwartz, Matthew D. (12 March 2018). "Scale-invariant instantons and the complete lifetime of the standard model". Physical Review D. 97 (5): 056006. arXiv:1707.08124. Bibcode:2018PhRvD..97e6006A. doi:10.1103/PhysRevD.97.056006. S2CID 118843387. /wiki/ArXiv_(identifier)

  254. Manuscript was updated after publication; lifetime numbers are taken from the latest revision at https://arxiv.org/abs/1707.08124. https://arxiv.org/abs/1707.08124

  255. Adams, Fred; Laughlin, Greg (1999). The Five Ages of the Universe. New York: The Free Press. ISBN 978-0684854229. 978-0684854229

  256. Caplan, M. E. (7 August 2020). "Black Dwarf Supernova in the Far Future". MNRAS. 497 (1–6): 4357–4362. arXiv:2008.02296. Bibcode:2020MNRAS.497.4357C. doi:10.1093/mnras/staa2262. S2CID 221005728. https://doi.org/10.1093%2Fmnras%2Fstaa2262

  257. Dyson, Freeman (1979). "Time Without End: Physics and Biology in an Open Universe". Reviews of Modern Physics. 51 (3): 447–460. Bibcode:1979RvMP...51..447D. doi:10.1103/RevModPhys.51.447. Archived from the original on 5 July 2008. Retrieved 5 July 2008. /wiki/Freeman_Dyson

  258. 10 10 26 {\displaystyle 10^{10^{26}}} is 1 followed by 1026 (100 septillion) zeroes.

  259. Although listed in years for convenience, the numbers at this point are so vast that their digits would remain unchanged regardless of which conventional units they were listed in, be they nanoseconds or star lifespans. /wiki/Numerical_digit

  260. Dyson, Freeman (1979). "Time Without End: Physics and Biology in an Open Universe". Reviews of Modern Physics. 51 (3): 447–460. Bibcode:1979RvMP...51..447D. doi:10.1103/RevModPhys.51.447. Archived from the original on 5 July 2008. Retrieved 5 July 2008. /wiki/Freeman_Dyson

  261. Dyson, Freeman (1979). "Time Without End: Physics and Biology in an Open Universe". Reviews of Modern Physics. 51 (3): 447–460. Bibcode:1979RvMP...51..447D. doi:10.1103/RevModPhys.51.447. Archived from the original on 5 July 2008. Retrieved 5 July 2008. /wiki/Freeman_Dyson

  262. This represents the time by which the event will most probably have happened. It may occur randomly at any time from the present.

  263. Although listed in years for convenience, the numbers at this point are so vast that their digits would remain unchanged regardless of which conventional units they were listed in, be they nanoseconds or star lifespans. /wiki/Numerical_digit

  264. 10 10 50 {\displaystyle 10^{10^{50}}} is 1 followed by 1050 (100 quindecillion) zeroes.

  265. Linde, Andrei (2007). "Sinks in the landscape, Boltzmann brains and the cosmological constant problem". Journal of Cosmology and Astroparticle Physics. 2007 (1): 022. arXiv:hep-th/0611043. Bibcode:2007JCAP...01..022L. CiteSeerX 10.1.1.266.8334. doi:10.1088/1475-7516/2007/01/022. ISSN 1475-7516. S2CID 16984680. /wiki/ArXiv_(identifier)

  266. Although listed in years for convenience, the numbers at this point are so vast that their digits would remain unchanged regardless of which conventional units they were listed in, be they nanoseconds or star lifespans. /wiki/Numerical_digit

  267. Dyson, Freeman (1979). "Time Without End: Physics and Biology in an Open Universe". Reviews of Modern Physics. 51 (3): 447–460. Bibcode:1979RvMP...51..447D. doi:10.1103/RevModPhys.51.447. Archived from the original on 5 July 2008. Retrieved 5 July 2008. /wiki/Freeman_Dyson

  268. Although listed in years for convenience, the numbers at this point are so vast that their digits would remain unchanged regardless of which conventional units they were listed in, be they nanoseconds or star lifespans. /wiki/Numerical_digit

  269. Linde, Andrei (2007). "Sinks in the landscape, Boltzmann brains and the cosmological constant problem". Journal of Cosmology and Astroparticle Physics. 2007 (1): 022. arXiv:hep-th/0611043. Bibcode:2007JCAP...01..022L. CiteSeerX 10.1.1.266.8334. doi:10.1088/1475-7516/2007/01/022. ISSN 1475-7516. S2CID 16984680. /wiki/ArXiv_(identifier)

  270. This represents the time by which the event will most probably have happened. It may occur randomly at any time from the present.

  271. Although listed in years for convenience, the numbers at this point are so vast that their digits would remain unchanged regardless of which conventional units they were listed in, be they nanoseconds or star lifespans. /wiki/Numerical_digit

  272. Carroll, Sean M.; Chen, Jennifer (27 October 2004). "Spontaneous Inflation and the Origin of the Arrow of Time". arXiv:hep-th/0410270. /wiki/Sean_M._Carroll

  273. Tegmark, Max (7 February 2003). "Parallel universes. Not just a staple of science fiction, other universes are a direct implication of cosmological observations". Scientific American. 288 (5): 40–51. arXiv:astro-ph/0302131. Bibcode:2003SciAm.288e..40T. doi:10.1038/scientificamerican0503-40. PMID 12701329. /wiki/Max_Tegmark

  274. Tegmark, Max (7 February 2003). Barrow, J. D.; Davies, P. C. W.; Harper, C. L. (eds.). "Parallel Universes". In "Science and Ultimate Reality: From Quantum to Cosmos", Honoring John Wheeler's 90th Birthday. 288 (5): 40–51. arXiv:astro-ph/0302131. Bibcode:2003SciAm.288e..40T. doi:10.1038/scientificamerican0503-40. PMID 12701329. /wiki/ArXiv_(identifier)

  275. Douglas, M. (21 March 2003). "The statistics of string / M theory vacua". JHEP. 0305 (46): 046. arXiv:hep-th/0303194. Bibcode:2003JHEP...05..046D. doi:10.1088/1126-6708/2003/05/046. S2CID 650509. /wiki/Michael_R._Douglas

  276. Ashok, S.; Douglas, M. (2004). "Counting flux vacua". JHEP. 0401 (60): 060. arXiv:hep-th/0307049. Bibcode:2004JHEP...01..060A. doi:10.1088/1126-6708/2004/01/060. S2CID 1969475. /wiki/ArXiv_(identifier)

  277. "Hurtling Through the Void". Time. 20 June 1983. Archived from the original on 22 December 2008. Retrieved 5 September 2011. https://web.archive.org/web/20081222014522/http://www.time.com/time/magazine/article/0,9171,926062,00.html

  278. Conception Archived 19 July 2011 at the Wayback Machine Official Zeitpyramide website. Retrieved 14 December 2010. http://www.zeitpyramide.de/

  279. Linder, Courtney (15 November 2019). "Microsoft is Storing Source Code in an Arctic Cave". Popular Mechanics. Archived from the original on 16 March 2021. Retrieved 25 July 2021. https://www.popularmechanics.com/technology/security/a29811351/microsoft-secret-code-vault/

  280. Kaku, Michio (2007). "The Physics of Extraterrestrial Civilizations: Official Website of Dr Michio Kaku". Retrieved 17 May 2025. https://mkaku.org/home/articles/the-physics-of-extraterrestrial-civilizations

  281. "Permanent Markers Implementation Plan" (PDF). United States Department of Energy. 30 August 2004. Archived from the original (PDF) on 28 September 2006. https://web.archive.org/web/20060928144722/http://www.wipp.energy.gov/PICsProg/Test1/Permanent_Markers_Implementation_Plan_rev1.pdf

  282. Chapman, Kit (5 May 2022). "How do we warn future generations about our toxic waste?". newhumanist.org.uk. Retrieved 14 August 2022. https://newhumanist.org.uk/5958/how-do-we-warn-future-generations-about-our-toxic-waste

  283. "The Long Now Foundation". The Long Now Foundation. 2011. Archived from the original on 16 June 2021. Retrieved 21 September 2011. http://longnow.org/about/

  284. "A Visit to the Doomsday Vault". CBS News. 20 March 2008. Archived from the original on 8 March 2021. Retrieved 5 January 2018. https://www.cbsnews.com/news/a-visit-to-the-doomsday-vault/

  285. Smith, Cameron; Davies, Evan T. (2012). Emigrating Beyond Earth: Human Adaptation and Space Colonization. Springer. p. 258. ISBN 978-1-4614-1165-9. 978-1-4614-1165-9

  286. Klein, Jan; Takahata, Naoyuki (2002). Where Do We Come From?: The Molecular Evidence for Human Descent. Springer. p. 395. ISBN 978-3-662-04847-4. 978-3-662-04847-4

  287. Greenberg, Joseph (1987). Language in the Americas. Stanford University Press. pp. 341–342. ISBN 978-0804713153. 978-0804713153

  288. Blakemore, Erin (17 May 2019). "Chernobyl disaster facts and information". Culture. National Geographic. Retrieved 5 November 2024. https://www.nationalgeographic.com/culture/article/chernobyl-disaster

  289. Audi, G.; Kondev, F. G.; Wang, M.; Huang, W. J.; et al. (2017). "The NUBASE2016 evaluation of nuclear properties" (PDF). Chinese Physics C. 41 (3): 030001. Bibcode:2017ChPhC..41c0001A. doi:10.1088/1674-1137/41/3/030001. https://www-nds.iaea.org/amdc/ame2016/NUBASE2016.pdf

  290. Time: Disasters that Shook the World. New York City: Time Home Entertainment. 2012. ISBN 978-1-60320-247-3. 978-1-60320-247-3

  291. "Cornell News: "It's the 25th Anniversary of Earth's First (and only) Attempt to Phone E.T."". Cornell University. 12 November 1999. Archived from the original on 2 August 2008. Retrieved 29 March 2008. https://web.archive.org/web/20080802005337/http://www.news.cornell.edu/releases/Nov99/Arecibo.message.ws.html

  292. Deamer, Dave. "In regard to the email from". Science 2.0. Archived from the original on 24 September 2015. Retrieved 14 November 2014. https://web.archive.org/web/20150924095532/http://www.science20.com/comments/28100/In_regard_to_the_email_from

  293. "Interpretation of NTFS Timestamps". Forensic Focus. 6 April 2013. Archived from the original on 8 March 2021. Retrieved 31 July 2021. https://www.forensicfocus.com/articles/interpretation-of-ntfs-timestamps/

  294. Bailer-Jones, Coryn A. L.; Farnocchia, Davide (3 April 2019). "Future stellar flybys of the Voyager and Pioneer spacecraft". Research Notes of the American Astronomical Society. 3 (59): 59. arXiv:1912.03503. Bibcode:2019RNAAS...3...59B. doi:10.3847/2515-5172/ab158e. S2CID 134524048. https://doi.org/10.3847%2F2515-5172%2Fab158e

  295. Bailer-Jones, Coryn A. L.; Farnocchia, Davide (3 April 2019). "Future stellar flybys of the Voyager and Pioneer spacecraft". Research Notes of the American Astronomical Society. 3 (59): 59. arXiv:1912.03503. Bibcode:2019RNAAS...3...59B. doi:10.3847/2515-5172/ab158e. S2CID 134524048. https://doi.org/10.3847%2F2515-5172%2Fab158e

  296. Bailer-Jones, Coryn A. L.; Farnocchia, Davide (3 April 2019). "Future stellar flybys of the Voyager and Pioneer spacecraft". Research Notes of the American Astronomical Society. 3 (59): 59. arXiv:1912.03503. Bibcode:2019RNAAS...3...59B. doi:10.3847/2515-5172/ab158e. S2CID 134524048. https://doi.org/10.3847%2F2515-5172%2Fab158e

  297. Bailer-Jones, Coryn A. L.; Farnocchia, Davide (3 April 2019). "Future stellar flybys of the Voyager and Pioneer spacecraft". Research Notes of the American Astronomical Society. 3 (59): 59. arXiv:1912.03503. Bibcode:2019RNAAS...3...59B. doi:10.3847/2515-5172/ab158e. S2CID 134524048. https://doi.org/10.3847%2F2515-5172%2Fab158e

  298. Artaxo, Paulo; Berntsen, Terje; Betts, Richard; Fahey, David W.; et al. (February 2018). "Changes in Atmospheric Constituents and in Radiative Forcing" (PDF). Intergovernmental Panel on Climate Change. p. 212. Archived (PDF) from the original on 18 February 2019. Retrieved 17 March 2021. https://www.ipcc.ch/site/assets/uploads/2018/02/ar4-wg1-chapter2-1.pdf

  299. Bailer-Jones, Coryn A. L.; Farnocchia, Davide (3 April 2019). "Future stellar flybys of the Voyager and Pioneer spacecraft". Research Notes of the American Astronomical Society. 3 (59): 59. arXiv:1912.03503. Bibcode:2019RNAAS...3...59B. doi:10.3847/2515-5172/ab158e. S2CID 134524048. https://doi.org/10.3847%2F2515-5172%2Fab158e

  300. McKay, Christopher P.; Toon, Owen B.; Kasting, James F. (8 August 1991). "Making Mars habitable". Nature. 352 (6335): 489–496. Bibcode:1991Natur.352..489M. doi:10.1038/352489a0. PMID 11538095. S2CID 2815367. Archived from the original on 8 March 2021. Retrieved 23 June 2019. https://zenodo.org/record/1233115

  301. Kaku, Michio (2010). "The Physics of Interstellar Travel: To one day, reach the stars". mkaku.org. Archived from the original on 10 February 2014. Retrieved 29 August 2010. /wiki/Michio_Kaku

  302. Biello, David (28 January 2009). "Spent Nuclear Fuel: A Trash Heap Deadly for 250,000 Years or a Renewable Energy Source?". Scientific American. Archived from the original on 10 July 2021. Retrieved 5 January 2018. https://www.scientificamerican.com/article/nuclear-waste-lethal-trash-or-renewable-energy-source/

  303. "Date - JavaScript". developer.mozilla.org. Mozilla. Archived from the original on 21 July 2021. Retrieved 27 July 2021. https://developer.mozilla.org/en-US/docs/Web/JavaScript/Reference/Global_Objects/Date

  304. Bailer-Jones, Coryn A. L.; Farnocchia, Davide (3 April 2019). "Future stellar flybys of the Voyager and Pioneer spacecraft". Research Notes of the American Astronomical Society. 3 (59): 59. arXiv:1912.03503. Bibcode:2019RNAAS...3...59B. doi:10.3847/2515-5172/ab158e. S2CID 134524048. https://doi.org/10.3847%2F2515-5172%2Fab158e

  305. "Memory of Mankind". Archived from the original on 16 July 2021. Retrieved 4 March 2019. https://www.memory-of-mankind.com/

  306. "Human Document Project 2014". Archived from the original on 19 May 2014. Retrieved 19 May 2014. http://hudoc2014.manucodiata.org/

  307. "Time it takes for garbage to decompose in the environment" (PDF). New Hampshire Department of Environmental Services. Archived from the original (PDF) on 9 June 2014. Retrieved 23 May 2014. https://web.archive.org/web/20140609083232/http://des.nh.gov/organization/divisions/water/wmb/coastal/trash/documents/marine_debris.pdf

  308. Lyle, Paul (2010). Between Rocks And Hard Places: Discovering Ireland's Northern Landscapes. Geological Survey of Northern Ireland. ISBN 978-0337095870. 978-0337095870

  309. Weisman, Alan (10 July 2007). The World Without Us. New York: Thomas Dunne Books/St. Martin's Press. pp. 171–172. ISBN 978-0-312-34729-1. OCLC 122261590. 978-0-312-34729-1

  310. Meadows, A. J. (2007). The Future of the Universe. Springer. pp. 81–83. ISBN 9781852339463. 9781852339463

  311. "Apollo 11 – First Footprint on the Moon". Student Features. NASA. Archived from the original on 3 April 2021. Retrieved 26 May 2014. https://www.nasa.gov/audience/forstudents/k-4/home/F_Apollo_11.html

  312. Bailer-Jones, Coryn A. L.; Farnocchia, Davide (3 April 2019). "Future stellar flybys of the Voyager and Pioneer spacecraft". Research Notes of the American Astronomical Society. 3 (59): 59. arXiv:1912.03503. Bibcode:2019RNAAS...3...59B. doi:10.3847/2515-5172/ab158e. S2CID 134524048. https://doi.org/10.3847%2F2515-5172%2Fab158e

  313. "The Pioneer Missions". NASA. Archived from the original on 29 June 2011. Retrieved 5 September 2011. https://www.nasa.gov/centers/ames/missions/archive/pioneer.html

  314. Avise, John; D. Walker; G. C. Johns (22 September 1998). "Speciation durations and Pleistocene effects on vertebrate phylogeography". Philosophical Transactions of the Royal Society B. 265 (1407): 1707–1712. doi:10.1098/rspb.1998.0492. PMC 1689361. PMID 9787467. /wiki/John_Avise

  315. Valentine, James W. (1985). "The Origins of Evolutionary Novelty And Galactic Colonization". In Finney, Ben R.; Jones, Eric M. (eds.). Interstellar Migration and the Human Experience. University of California Press. p. 274. ISBN 978-0520058781. 978-0520058781

  316. "The Pioneer Missions". NASA. Archived from the original on 29 June 2011. Retrieved 5 September 2011. https://www.nasa.gov/centers/ames/missions/archive/pioneer.html

  317. Wilson, Jason; Staley, Joshua M.; Wyckoff, Gerald J. (7 February 2020). "Extinction of chromosomes due to specialization is a universal occurrence". Scientific Reports. 10 (1): 2170. Bibcode:2020NatSR..10.2170W. doi:10.1038/s41598-020-58997-2. ISSN 2045-2322. PMC 7005762. PMID 32034231. https://www.ncbi.nlm.nih.gov/pmc/articles/PMC7005762

  318. Graves JA (2004). "The degenerate Y chromosome--can conversion save it?". Reproduction, Fertility, and Development. 16 (5): 527–534. doi:10.1071/RD03096. PMID 15367368. /wiki/Doi_(identifier)

  319. Weisman, Alan (10 July 2007). The World Without Us. New York: Thomas Dunne Books/St. Martin's Press. p. 182. ISBN 978-0-312-34729-1. OCLC 122261590. 978-0-312-34729-1

  320. Gott, J. Richard (May 1993). "Implications of the Copernican principle for our future prospects". Nature. 363 (6427): 315–319. Bibcode:1993Natur.363..315G. doi:10.1038/363315a0. ISSN 0028-0836. S2CID 4252750. /wiki/Bibcode_(identifier)

  321. Lasher, Lawrence. "Pioneer Mission Status". NASA. Archived from the original on 8 April 2000. [Pioneer's speed is] about 12 km/s... [the plate etching] should survive recognizable at least to a distance ≈10 parsecs, and most probably to 100 parsecs. https://web.archive.org/web/20000408152959/http://spaceprojects.arc.nasa.gov/Space_Projects/pioneer/PNStat.html

  322. "LAGEOS 1, 2". NASA. Archived from the original on 21 July 2011. Retrieved 21 July 2012. https://web.archive.org/web/20110721062751/http://space.jpl.nasa.gov/msl/QuickLooks/lageosQL.html

  323. Bignami, Giovanni F.; Sommariva, Andrea (2013). A Scenario for Interstellar Exploration and Its Financing. Springer. p. 23. Bibcode:2013sief.book.....B. ISBN 9788847053373. 9788847053373

  324. Zalasiewicz, Jan (25 September 2008). The Earth After Us: What legacy will humans leave in the rocks?. Oxford University Press., Review in Stanford Archaeology https://web.archive.org/web/20140513011343/http://www.stanford.edu/dept/archaeology/cgi-bin/archaeolog/?p=239

  325. Begtrup, G. E.; Gannett, W.; Yuzvinsky, T. D.; Crespi, V. H.; et al. (13 May 2009). "Nanoscale Reversible Mass Transport for Archival Memory" (PDF). Nano Letters. 9 (5): 1835–1838. Bibcode:2009NanoL...9.1835B. CiteSeerX 10.1.1.534.8855. doi:10.1021/nl803800c. PMID 19400579. Archived from the original (PDF) on 22 June 2010. https://web.archive.org/web/20100622232231/http://www.physics.berkeley.edu/research/zettl/pdf/363.NanoLet.9-Begtrup.pdf

  326. Abumrad, Jad; Krulwich, Robert (12 February 2010). Carl Sagan And Ann Druyan's Ultimate Mix Tape. Radiolab (Radio). NPR. /wiki/Jad_Abumrad

  327. Korycansky, D. G.; Laughlin, Gregory; Adams, Fred C. (2001). "Astronomical engineering: a strategy for modifying planetary orbits". Astrophysics and Space Science. 275 (4): 349–366. arXiv:astro-ph/0102126. Bibcode:2001Ap&SS.275..349K. doi:10.1023/A:1002790227314. hdl:2027.42/41972. S2CID 5550304. Astrophys.Space Sci.275:349-366, 2001. /wiki/ArXiv_(identifier)

  328. Korycansky, D. G. (2004). "Astroengineering, or how to save the Earth in only one billion years" (PDF). Revista Mexicana de Astronomía y Astrofísica. 22: 117–120. Bibcode:2004RMxAC..22..117K. Archived (PDF) from the original on 23 September 2015. Retrieved 7 September 2014. http://www.astroscu.unam.mx/rmaa/RMxAC..22/PDF/RMxAC..22_korycansky.pdf

  329. "Date/Time Conversion Contract Language" (PDF). New York: Office of Information Technology Services. 19 May 2019. Archived (PDF) from the original on 30 April 2021. Retrieved 16 October 2020. https://its.ny.gov/sites/default/files/documents/nys-p98-003_date_time_conversion_contract_language_1.pdf

  330. Bailer-Jones, Coryn A. L.; Farnocchia, Davide (3 April 2019). "Future stellar flybys of the Voyager and Pioneer spacecraft". Research Notes of the American Astronomical Society. 3 (59): 59. arXiv:1912.03503. Bibcode:2019RNAAS...3...59B. doi:10.3847/2515-5172/ab158e. S2CID 134524048. https://doi.org/10.3847%2F2515-5172%2Fab158e

  331. Zhang, J.; Gecevičius, M.; Beresna, M.; Kazansky, P. G. (2014). "Seemingly unlimited lifetime data storage in nanostructured glass". Phys. Rev. Lett. 112 (3): 033901. Bibcode:2014PhRvL.112c3901Z. doi:10.1103/PhysRevLett.112.033901. PMID 24484138. S2CID 27040597. Archived from the original on 2 August 2021. Retrieved 6 September 2018. https://www.researchgate.net/publication/260004721

  332. Zhang, J.; Gecevičius, M.; Beresna, M.; Kazansky, P. G. (June 2013). "5D Data Storage by Ultrafast Laser Nanostructuring in Glass" (PDF). CLEO: Science and Innovations: CTh5D–9. Archived from the original (PDF) on 6 September 2014. https://web.archive.org/web/20140906152109/http://www.orc.soton.ac.uk/fileadmin/downloads/5D_Data_Storage_by_Ultrafast_Laser_Nanostructuring_in_Glass.pdf