An angle is a figure lying in a plane formed by two distinct rays (half-lines emanating indefinitely from an endpoint in one direction), which share a common endpoint. The rays are called the sides or arms of the angle, and the common endpoint is called the vertex. The sides divide the plane into two regions: the interior of the angle and the exterior of the angle.6
An angle symbol ( ∠ {\displaystyle \angle } or ^ {\displaystyle {\widehat {\quad }}} , read as "angle") together with one or three defining points is used to identify angles in geometric figures. For example, the angle with vertex A formed by the rays A B → {\displaystyle {\vec {AB}}} and AC → {\displaystyle {\vec {\text{AC}}}} is denoted as ∠ A {\displaystyle \angle A} (using the vertex alone) or ∠ BAC {\displaystyle \angle {\text{BAC}}} (with the vertex always named in the middle). The size or measure of the angle is denoted m ∠ A {\displaystyle m\angle {\text{A}}} or m ∠ BAC {\displaystyle m\angle {\text{BAC}}} .
In geometric figures and mathematical expressions, it is also common to use Greek letters (α, β, γ, θ, φ, ...) or lower case Roman letters (a, b, c, ...) as variables to represent the size of an angle.7 The Greek letter π is typically not used for this purpose to avoid confusion with the circle constant.
Conventionally, angle size is measured "between" the sides through the interior of the angle and given as a magnitude or scalar quantity. At other times it might be measured through the exterior of the angle or given as a signed number to indicate a direction of measurement (see § Signed angles).
Angles are measured in various units, the most common being the degree (denoted by the symbol °), radian (denoted by the symbol rad) and turn. These units differ in the way they divide up a full angle, an angle where one ray, initially congruent to the other, performs a compete rotation about the vertex to return back to its starting position.
Degrees and turns are defined directly with reference to a full angle, which measures 1 turn or 360°. A measure in turns gives an angle's size as a proportion of a full angle and a degree can be considered as a subdivision of a turn. Radians are not defined directly in relation to a full angle (see § Measuring angles), but in such a way that its measure is 2π rad, approximately 6.28 rad.
The names, intervals, and measuring units are shown in the table below:
The angle addition postulate states that if D is a point lying in the interior of ∠ BAC {\displaystyle \angle {\text{BAC}}} then:13 m ∠ BAC = m ∠ BAD + m ∠ DAC . {\displaystyle m\angle {\text{BAC}}=m\angle {\text{BAD}}+m\angle {\text{DAC}}.} This relationship defines what it means add any two angles: their vertices are placed together while sharing a side to create a new larger angle. The measure of the new larger angle is the sum of the measures of the two angles. Subtraction follows from rearrangement of the formula.
"Oblique angle" redirects here. For the cinematographic technique, see Dutch angle.
"Vertical angle" redirects here and is not to be confused with Zenith angle.
Adjacent angles (abbreviated adj. ∠s), are angles that share a common vertex and edge but do not share any interior points. In other words, they are angles side by side or adjacent, sharing an "arm". Adjacent angles which sum to a right angle, straight angle, or full angle are special and are respectively called complementary, supplementary, and explementary angles (see § Combining angle pairs below).
Vertical angles are formed when two straight lines intersect at a point producing four angles. A pair of angles opposite each other are called vertical angles, opposite angles or vertically opposite angles (abbreviated vert. opp. ∠s),14 where "vertical" refers to the sharing of a vertex, rather than an up-down orientation. The vertical angle theorem states that vertical angles are always congruent or equal to each other.
A transversal is a line that intersects a pair of (often parallel) lines and is associated with exterior angles, interior angles, alternate exterior angles, alternate interior angles, corresponding angles, and consecutive interior angles.15
When summing two angles that are either adjacent or separated in space, three cases are of particular importance.
Complementary angles are angle pairs whose measures sum to a right angle (1/4 turn, 90°, or π/2 rad).16 If the two complementary angles are adjacent, their non-shared sides form a right angle. In a right-angle triangle the two acute angles are complementary as the sum of the internal angles of a triangle is 180°.
The difference between an angle and a right angle is termed the complement of the angle17 which is from the Latin complementum and associated verb complere, meaning "to fill up". An acute angle is "filled up" by its complement to form a right angle.
Complementary angles are fundamental to trigonometry and the Pythagorean theorem.
Two angles that sum to a straight angle (1/2 turn, 180°, or π rad) are called supplementary angles.18 If the two supplementary angles are adjacent, their non-shared sides form a straight angle or straight line and are called a linear pair of angles.19 The difference between an angle and a straight angle is termed the supplement of the angle.
Examples of non-adjacent complementary angles include the consecutive angles a parallelogram and opposite angles of a cyclic quadrilateral. For a circle with center O, and tangent lines from an exterior point P touching the circle at points T and Q, the resulting angles ∠TPQ and ∠TOQ are supplementary.
Two angles that sum to a full angle (1 turn, 360°, or 2π radians) are called explementary angles or conjugate angles.20 The difference between an angle and a full angle is termed the explement or conjugate of the angle.
See also: Angle measuring instrument
Measurement of angles is intrinsically linked with circles and rotation. An angle is measured by placing it within a circle of any size, with the vertex at the circle's centre and the sides intersecting the perimeter.
An arc s is formed as the shortest distance on the perimeter between the two points of intersection, which is said to be the arc subtended by the angle.
The length of s can be used to measure the angle's size θ {\displaystyle \theta } , however as s is dependent on the size of the circle chosen, it must be adjusted so that any arbitrary circle will give the same measure of angle. This can be done in two ways: by taking the ratio to either the radius r or circumference C of the circle.
The ratio of the length s by the radius r is the number of radians in the angle, while the ratio of length s by the circumference C is the number of turns:27 θ r a d = s r r a d θ t u r n = s C = s 2 π r t u r n s {\displaystyle \theta _{\mathrm {rad} }={\frac {s}{r}}\,\mathrm {rad} \qquad \qquad \theta _{\mathrm {turn} }={\frac {s}{C}}\ ={\frac {s}{2\pi r}}\,\mathrm {turns} }
The value of θ thus defined is independent of the size of the circle: if the length of the radius is changed, then both the circumference and the arc length change in the same proportion, so the ratios s/r and s/C are unaltered.28
Angles of the same size are said to be equal congruent or equal in measure.
In addition to the radian and turn, other angular units exist, typically based on subdivisions of the turn, including the degree (°) and the gradian (grad), though many others have been used throughout history.29
Conversion between units may be obtained by multiplying the angular measure in one unit by a conversion constant of the form k a k b {\displaystyle {\tfrac {k_{a}}{k_{b}}}} where k a {\displaystyle {k_{a}}} and k b {\displaystyle {k_{b}}} are the measures of a complete turn in units a and b. For example, to convert an angle of π 2 {\displaystyle {\tfrac {\pi }{2}}} radians to degrees: θ deg = k deg k r a d ⋅ θ r a d = 360 ∘ 2 π r a d ⋅ π 2 r a d = 90 ∘ {\displaystyle \theta _{\deg }={\frac {k_{\deg }}{k_{\mathrm {rad} }}}\cdot \theta _{\mathrm {rad} }={\frac {360^{\circ }}{2\pi \,\mathrm {rad} }}\cdot {\frac {\pi }{2}}\,\mathrm {rad} =90^{\circ }}
The following table lists some units used to represent angles.
Further information: Radian § Dimensional analysis
In mathematics and the International System of Quantities, an angle is defined as a dimensionless quantity, and in particular, the radian is defined as dimensionless in the International System of Units. This convention prevents angles providing information for dimensional analysis.
While mathematically convenient, this has led to significant discussion among scientists and teachers. Some scientists have suggested treating the angle as having its own dimension, similar to length or time. This would mean that angle units like radians would always be explicitly present in calculations, making the dimensional analysis more straightforward. However, this approach would also require changing many well-known mathematical and physics formulas.
Main article: Angle of rotation
See also: Sign (mathematics) § Angles, and Euclidean space § Angle
An angle denoted as ∠BAC might refer to any of four angles: the clockwise angle from B to C about A, the anticlockwise angle from B to C about A, the clockwise angle from C to B about A, or the anticlockwise angle from C to B about A, It is therefore frequently helpful to impose a convention that allows positive and negative angular values to represent orientations and/or rotations in opposite directions or "sense" relative to some reference.
In a two-dimensional Cartesian coordinate system, an angle is typically defined by its two sides, with its vertex at the origin. The initial side is on the positive x-axis, while the other side or terminal side is defined by the measure from the initial side in radians, degrees, or turns, with positive angles representing rotations toward the positive y-axis and negative angles representing rotations toward the negative y-axis. When Cartesian coordinates are represented by standard position, defined by the x-axis rightward and the y-axis upward, positive rotations are anticlockwise, and negative cycles are clockwise.
In many contexts, an angle of −θ is effectively equivalent to an angle of "one full turn minus θ". For example, an orientation represented as −45° is effectively equal to an orientation defined as 360° − 45° or 315°. Although the final position is the same, a physical rotation (movement) of −45° is not the same as a rotation of 315° (for example, the rotation of a person holding a broom resting on a dusty floor would leave visually different traces of swept regions on the floor).
In three-dimensional geometry, "clockwise" and "anticlockwise" have no absolute meaning, so the direction of positive and negative angles must be defined in terms of an orientation, which is typically determined by a normal vector passing through the angle's vertex and perpendicular to the plane in which the rays of the angle lie.
In navigation, bearings or azimuth are measured relative to north. By convention, viewed from above, bearing angles are positive clockwise, so a bearing of 45° corresponds to a north-east orientation. Negative bearings are not used in navigation, so a north-west orientation corresponds to a bearing of 315°.
For an angular unit, it is definitional that the angle addition postulate holds, however some measurements or quantities related to angles are in use that do not satisfy this postulate:
The angle between a line and a curve (mixed angle) or between two intersecting curves (curvilinear angle) is defined to be the angle between the tangents at the point of intersection. Various names (now rarely, if ever, used) have been given to particular cases:—amphicyrtic (Gr. ἀμφί, on both sides, κυρτός, convex) or cissoidal (Gr. κισσός, ivy), biconvex; xystroidal or sistroidal (Gr. ξυστρίς, a tool for scraping), concavo-convex; amphicoelic (Gr. κοίλη, a hollow) or angulus lunularis, biconcave.35
Main articles: Bisection § Angle bisector, and Angle trisection
The ancient Greek mathematicians knew how to bisect an angle (divide it into two angles of equal measure) using only a compass and straightedge but could only trisect certain angles. In 1837, Pierre Wantzel showed that this construction could not be performed for most angles.
In the Euclidean space, the angle θ between two Euclidean vectors u and v is related to their dot product and their lengths by the formula u ⋅ v = cos ( θ ) ‖ u ‖ ‖ v ‖ . {\displaystyle \mathbf {u} \cdot \mathbf {v} =\cos(\theta )\left\|\mathbf {u} \right\|\left\|\mathbf {v} \right\|.}
This formula supplies an easy method to find the angle between two planes (or curved surfaces) from their normal vectors and between skew lines from their vector equations.
To define angles in an abstract real inner product space, we replace the Euclidean dot product ( · ) by the inner product ⟨ ⋅ , ⋅ ⟩ {\displaystyle \langle \cdot ,\cdot \rangle } , i.e. ⟨ u , v ⟩ = cos ( θ ) ‖ u ‖ ‖ v ‖ . {\displaystyle \langle \mathbf {u} ,\mathbf {v} \rangle =\cos(\theta )\ \left\|\mathbf {u} \right\|\left\|\mathbf {v} \right\|.}
In a complex inner product space, the expression for the cosine above may give non-real values, so it is replaced with Re ( ⟨ u , v ⟩ ) = cos ( θ ) ‖ u ‖ ‖ v ‖ . {\displaystyle \operatorname {Re} \left(\langle \mathbf {u} ,\mathbf {v} \rangle \right)=\cos(\theta )\left\|\mathbf {u} \right\|\left\|\mathbf {v} \right\|.} or, more commonly, using the absolute value, with | ⟨ u , v ⟩ | = | cos ( θ ) | ‖ u ‖ ‖ v ‖ . {\displaystyle \left|\langle \mathbf {u} ,\mathbf {v} \rangle \right|=\left|\cos(\theta )\right|\left\|\mathbf {u} \right\|\left\|\mathbf {v} \right\|.}
The latter definition ignores the direction of the vectors. It thus describes the angle between one-dimensional subspaces span ( u ) {\displaystyle \operatorname {span} (\mathbf {u} )} and span ( v ) {\displaystyle \operatorname {span} (\mathbf {v} )} spanned by the vectors u {\displaystyle \mathbf {u} } and v {\displaystyle \mathbf {v} } correspondingly.
The definition of the angle between one-dimensional subspaces span ( u ) {\displaystyle \operatorname {span} (\mathbf {u} )} and span ( v ) {\displaystyle \operatorname {span} (\mathbf {v} )} given by | ⟨ u , v ⟩ | = | cos ( θ ) | ‖ u ‖ ‖ v ‖ {\displaystyle \left|\langle \mathbf {u} ,\mathbf {v} \rangle \right|=\left|\cos(\theta )\right|\left\|\mathbf {u} \right\|\left\|\mathbf {v} \right\|} in a Hilbert space can be extended to subspaces of finite number of dimensions. Given two subspaces U {\displaystyle {\mathcal {U}}} , W {\displaystyle {\mathcal {W}}} with dim ( U ) := k ≤ dim ( W ) := l {\displaystyle \dim({\mathcal {U}}):=k\leq \dim({\mathcal {W}}):=l} , this leads to a definition of k {\displaystyle k} angles called canonical or principal angles between subspaces.
In Riemannian geometry, the metric tensor is used to define the angle between two tangents. Where U and V are tangent vectors and gij are the components of the metric tensor G, cos θ = g i j U i V j | g i j U i U j | | g i j V i V j | . {\displaystyle \cos \theta ={\frac {g_{ij}U^{i}V^{j}}{\sqrt {\left|g_{ij}U^{i}U^{j}\right|\left|g_{ij}V^{i}V^{j}\right|}}}.}
A hyperbolic angle is an argument of a hyperbolic function just as the circular angle is the argument of a circular function. The comparison can be visualized as the size of the openings of a hyperbolic sector and a circular sector since the areas of these sectors correspond to the angle magnitudes in each case.36 Unlike the circular angle, the hyperbolic angle is unbounded. When the circular and hyperbolic functions are viewed as infinite series in their angle argument, the circular ones are just alternating series forms of the hyperbolic functions. This comparison of the two series corresponding to functions of angles was described by Leonhard Euler in Introduction to the Analysis of the Infinite (1748).
The word angle comes from the Latin word angulus, meaning "corner". Cognate words include the Greek ἀγκύλος (ankylοs) meaning "crooked, curved" and the English word "ankle". Both are connected with the Proto-Indo-European root *ank-, meaning "to bend" or "bow".37
Euclid defines a plane angle as the inclination to each other, in a plane, of two lines that meet each other and do not lie straight with respect to each other. According to the Neoplatonic metaphysician Proclus, an angle must be either a quality, a quantity, or a relationship. The first concept, angle as quality, was used by Eudemus of Rhodes, who regarded an angle as a deviation from a straight line; the second, angle as quantity, by Carpus of Antioch, who regarded it as the interval or space between the intersecting lines; Euclid adopted the third: angle as a relationship.38
The equality of vertically opposite angles is called the vertical angle theorem. Eudemus of Rhodes attributed the proof to Thales of Miletus.3940 The proposition showed that since both of a pair of vertical angles are supplementary to both of the adjacent angles, the vertical angles are equal in measure. According to a historical note,41 when Thales visited Egypt, he observed that whenever the Egyptians drew two intersecting lines, they would measure the vertical angles to make sure that they were equal. Thales concluded that one could prove that all vertical angles are equal if one accepted some general notions such as:
When two adjacent angles form a straight line, they are supplementary. Therefore, if we assume that the measure of angle A equals x, the measure of angle C would be 180° − x. Similarly, the measure of angle D would be 180° − x. Both angle C and angle D have measures equal to 180° − x and are congruent. Since angle B is supplementary to both angles C and D, either of these angle measures may be used to determine the measure of Angle B. Using the measure of either angle C or angle D, we find the measure of angle B to be 180° − (180° − x) = 180° − 180° + x = x. Therefore, both angle A and angle B have measures equal to x and are equal in measure.
In geography, the location of any point on the Earth can be identified using a geographic coordinate system. This system specifies the latitude and longitude of any location in terms of angles subtended at the center of the Earth, using the equator and (usually) the Greenwich meridian as references.
In astronomy, a given point on the celestial sphere (that is, the apparent position of an astronomical object) can be identified using any of several astronomical coordinate systems, where the references vary according to the particular system. Astronomers measure the angular separation of two stars by imagining two lines through the center of the Earth, each intersecting one of the stars. The angle between those lines and the angular separation between the two stars can be measured.
In both geography and astronomy, a sighting direction can be specified in terms of a vertical angle such as altitude /elevation with respect to the horizon as well as the azimuth with respect to north.
Astronomers also measure objects' apparent size as an angular diameter. For example, the full moon has an angular diameter of approximately 0.5° when viewed from Earth. One could say, "The Moon's diameter subtends an angle of half a degree." The small-angle formula can convert such an angular measurement into a distance/size ratio.
Other astronomical approximations include:
These measurements depend on the individual subject, and the above should be treated as rough rule of thumb approximations only.
In astronomy, right ascension and declination are usually measured in angular units, expressed in terms of time, based on a 24-hour day.
This article incorporates text from a publication now in the public domain: Chisholm, Hugh, ed. (1911), "Angle", Encyclopædia Britannica, vol. 2 (11th ed.), Cambridge University Press, p. 14
Hilbert, David. The Foundations of Geometry (PDF). p. 9. https://math.berkeley.edu/~wodzicki/160/Hilbert.pdf ↩
Sidorov 2001 - Sidorov, L. A. (2001) [1994], "Angle", Encyclopedia of Mathematics, EMS Press https://www.encyclopediaofmath.org/index.php?title=Angle ↩
Evgrafov, M. A. (2019-09-18). Analytic Functions. Courier Dover Publications. ISBN 978-0-486-84366-7. 978-0-486-84366-7 ↩
Papadopoulos, Athanase (2012). Strasbourg Master Class on Geometry. European Mathematical Society. ISBN 978-3-03719-105-7. 978-3-03719-105-7 ↩
An angular sector can be constructed by the combination of two rotated half-planes, either their intersection or union (in the case of acute or obtuse angles, respectively).[5][6] It corresponds to a circular sector of infinite radius and a flat pencil of half-lines.[7] /wiki/Half-plane ↩
Aboughantous 2010, p. 18. - Aboughantous, Charles H. (2010), A High School First Course in Euclidean Plane Geometry, Universal Publishers, ISBN 978-1-59942-822-2 https://books.google.com/books?id=4JK19X5ZI2IC&pg=PA18 ↩
Moser 1971, p. 41. - Moser, James M. (1971), Modern Elementary Geometry, Prentice-Hall https://archive.org/details/modernelementary0000mose/page/41/mode/2up ↩
Godfrey & Siddons 1919, p. 9. - Godfrey, Charles; Siddons, A. W. (1919), Elementary geometry: practical and theoretical (3rd ed.), Cambridge University Press https://archive.org/details/elementarygeomet00godfuoft/page/9/mode/2up? ↩
Moser 1971, p. 71. - Moser, James M. (1971), Modern Elementary Geometry, Prentice-Hall https://archive.org/details/modernelementary0000mose/page/41/mode/2up ↩
Moise, Edwin, E (1990). Elementary geometry from an advanced standpoint (PDF) (3rd ed.). Addison-Wesley Publishing Company. p. 96.{{cite book}}: CS1 maint: multiple names: authors list (link) https://www.ime.usp.br/~toscano/disc/2021/Moise.pdf ↩
Wong & Wong 2009, pp. 161–163 - Wong, Tak-wah; Wong, Ming-sim (2009), "Angles in Intersecting and Parallel Lines", New Century Mathematics, vol. 1B (1 ed.), Hong Kong: Oxford University Press, pp. 161–163, ISBN 978-0-19-800177-5 ↩
Jacobs 1974, p. 255. - Jacobs, Harold R. (1974), Geometry, W. H. Freeman, pp. 97, 255, ISBN 978-0-7167-0456-0 ↩
"Complementary Angles". www.mathsisfun.com. Retrieved 2020-08-17. https://www.mathsisfun.com/geometry/complementary-angles.html ↩
Chisholm 1911 - Chisholm, Hugh, ed. (1911), "Angle", Encyclopædia Britannica, vol. 2 (11th ed.), Cambridge University Press, p. 14 ↩
"Supplementary Angles". www.mathsisfun.com. Retrieved 2020-08-17. https://www.mathsisfun.com/geometry/supplementary-angles.html ↩
Jacobs 1974, p. 97. - Jacobs, Harold R. (1974), Geometry, W. H. Freeman, pp. 97, 255, ISBN 978-0-7167-0456-0 ↩
Willis, Clarence Addison (1922). Plane Geometry. Blakiston's Son. p. 8. https://archive.org/details/planegeometryexp00willrich/page/8/ ↩
Henderson & Taimina 2005, p. 104. - Henderson, David W.; Taimina, Daina (2005), Experiencing Geometry / Euclidean and Non-Euclidean with History (3rd ed.), Pearson Prentice Hall, p. 104, ISBN 978-0-13-143748-7 ↩
Johnson, Roger A. Advanced Euclidean Geometry, Dover Publications, 2007. ↩
D. Zwillinger, ed. (1995), CRC Standard Mathematical Tables and Formulae, Boca Raton, FL: CRC Press, p. 270 as cited in Weisstein, Eric W. "Exterior Angle". MathWorld. /wiki/Eric_W._Weisstein ↩
International Bureau of Weights and Measures (20 May 2019), The International System of Units (SI) (PDF) (9th ed.), ISBN 978-92-822-2272-0, archived from the original on 18 October 2021 978-92-822-2272-0 ↩
This approach requires, however, an additional proof that the measure of the angle does not change with changing radius r, in addition to the issue of "measurement units chosen". A smoother approach is to measure the angle by the length of the corresponding unit circle arc. Here "unit" can be chosen to be dimensionless in the sense that it is the real number 1 associated with the unit segment on the real line. See Radoslav M. Dimitrić, for instance.[24] ↩
"angular unit". TheFreeDictionary.com. Retrieved 2020-08-31. https://www.thefreedictionary.com/angular+unit ↩
"ooPIC Programmer's Guide - Chapter 15: URCP". ooPIC Manual & Technical Specifications - ooPIC Compiler Ver 6.0. Savage Innovations, LLC. 2007 [1997]. Archived from the original on 2008-06-28. Retrieved 2019-08-05. https://web.archive.org/web/20080628051746/http://www.oopic.com/pgchap15.htm ↩
Jeans, James Hopwood (1947). The Growth of Physical Science. CUP Archive. p. 7. /wiki/James_Hopwood_Jeans ↩
Murnaghan, Francis Dominic (1946). Analytic Geometry. p. 2. /wiki/Francis_Dominic_Murnaghan_(mathematician) ↩
"Mathwords: Reference Angle". www.mathwords.com. Archived from the original on 23 October 2017. Retrieved 26 April 2018. http://www.mathwords.com/r/reference_angle.htm ↩
McKeague, Charles P. (2008). Trigonometry (6th ed.). Belmont, CA: Thomson Brooks/Cole. p. 110. ISBN 978-0495382607. 978-0495382607 ↩
Chisholm 1911; Heiberg 1908, p. 178 - Chisholm, Hugh, ed. (1911), "Angle", Encyclopædia Britannica, vol. 2 (11th ed.), Cambridge University Press, p. 14 ↩
Robert Baldwin Hayward (1892) The Algebra of Coplanar Vectors and Trigonometry, chapter six /wiki/Robert_Baldwin_Hayward ↩
Slocum 2007 - Slocum, Jonathan (2007), Preliminary Indo-European lexicon — Pokorny PIE data, University of Texas research department: linguistics research center, archived from the original on 27 June 2010, retrieved 2 Feb 2010 https://web.archive.org/web/20100627012240/http://www.utexas.edu/cola/centers/lrc/ielex/X/P0089.html ↩
Chisholm 1911; Heiberg 1908, pp. 177–178 - Chisholm, Hugh, ed. (1911), "Angle", Encyclopædia Britannica, vol. 2 (11th ed.), Cambridge University Press, p. 14 ↩
Euclid. The Elements. Proposition I:13. /wiki/Euclid ↩
Shute, Shirk & Porter 1960, pp. 25–27. - Shute, William G.; Shirk, William W.; Porter, George F. (1960), Plane and Solid Geometry, American Book Company, pp. 25–27 ↩