It can be expressed as the simple continued fraction [1; 1, 2, 1, 2, 1, 2, 1, …] (sequence A040001 in the OEIS).
So it is true to say:
then when n → ∞ {\displaystyle n\to \infty } :
The square root of 3 can be found as the leg length of an equilateral triangle that encompasses a circle with a diameter of 1.
If an equilateral triangle with sides of length 1 is cut into two equal halves, by bisecting an internal angle across to make a right angle with one side, the right angle triangle's hypotenuse is length one, and the sides are of length 1 2 {\textstyle {\frac {1}{2}}} and 3 2 {\textstyle {\frac {\sqrt {3}}{2}}} . From this, tan 60 ∘ = 3 {\textstyle \tan {60^{\circ }}={\sqrt {3}}} , sin 60 ∘ = 3 2 {\textstyle \sin {60^{\circ }}={\frac {\sqrt {3}}{2}}} , and cos 30 ∘ = 3 2 {\textstyle \cos {30^{\circ }}={\frac {\sqrt {3}}{2}}} .
The square root of 3 also appears in algebraic expressions for various other trigonometric constants, including3 the sines of 3°, 12°, 15°, 21°, 24°, 33°, 39°, 48°, 51°, 57°, 66°, 69°, 75°, 78°, 84°, and 87°.
It is the distance between parallel sides of a regular hexagon with sides of length 1.
It is the length of the space diagonal of a unit cube.
The vesica piscis has a major axis to minor axis ratio equal to 1 : 3 {\displaystyle 1:{\sqrt {3}}} . This can be shown by constructing two equilateral triangles within it.
In power engineering, the voltage between two phases in a three-phase system equals 3 {\textstyle {\sqrt {3}}} times the line to neutral voltage. This is because any two phases are 120° apart, and two points on a circle 120 degrees apart are separated by 3 {\textstyle {\sqrt {3}}} times the radius (see geometry examples above).
It is known that most roots of the nth derivatives of J ν ( n ) ( x ) {\displaystyle J_{\nu }^{(n)}(x)} (where n < 18 and J ν ( x ) {\displaystyle J_{\nu }(x)} is the Bessel function of the first kind of order ν {\displaystyle \nu } ) are transcendental. The only exceptions are the numbers ± 3 {\displaystyle \pm {\sqrt {3}}} , which are the algebraic roots of both J 1 ( 3 ) ( x ) {\displaystyle J_{1}^{(3)}(x)} and J 0 ( 4 ) ( x ) {\displaystyle J_{0}^{(4)}(x)} .4
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