List of trigonometric identities

Cosines and sines around the unit circle

Trigonometry

Outline History Usage Functions (inverse) Generalized trigonometry
Reference
Identities Exact constants Tables Unit circle
Laws and theorems
Sines Cosines Tangents Cotangents Pythagorean theorem
Calculus
Trigonometric substitution Integrals (inverse functions) Derivatives

In mathematics, trigonometric identities are equalities that involve trigonometric functions and are true for every single value of the occurring variables where both sides of the equality are defined. Geometrically, these are identities involving certain functions of one or more angles. They are distinct from triangle identities, which are identities potentially involving angles but also involving side lengths or other lengths of a triangle.

These identities are useful whenever expressions involving trigonometric functions need to be simplified. An important application is the integration of non-trigonometric functions: a common technique involves first using the substitution rule with a trigonometric function, and then simplifying the resulting integral with a trigonometric identity.

Notation

Angles

This article uses Greek letters such as alpha ( $α$ ), beta ( $β$ ), gamma ( $γ$ ), and theta ( $θ$ ) to represent angles. Several different units of angle measure are widely used, including degrees, radians, and gradians (gons):

1 full circle (turn) = 360 degrees = 2

π

radians = 400 gons.

The following table shows the conversions and values for some common angles:

Conversions of common angles
Turns	Degrees	Radians	Gradians	sine	cosine	tangent
0	0°	0	0^g	0	1	0
1/12	30°	$π$ /6	33 1/3^g	1/2	√3/2	√3/3
1/8	45°	$π$ /4	50^g	√2/2	√2/2	1
1/6	60°	$π$ /3	66 2/3^g	√3/2	1/2	√3
1/4	90°	$π$ /2	100^g	1	0	undef.
1/3	120°	2 $π$ /3	133 1/3^g	√3/2	−1/2	−√3
3/8	135°	3 $π$ /4	150^g	√2/2	−√2/2	−1
5/12	150°	5 $π$ /6	166 2/3^g	1/2	−√3/2	−√3/3
1/2	180°	$π$	200^g	0	−1	0
7/12	210°	7 $π$ /6	233 1/3^g	−1/2	−√3/2	√3/3
5/8	225°	5 $π$ /4	250^g	−√2/2	−√2/2	1
2/3	240°	4 $π$ /3	266 2/3^g	−√3/2	−1/2	√3
3/4	270°	3 $π$ /2	300^g	−1	0	undef.
5/6	300°	5 $π$ /3	333 1/3^g	−√3/2	1/2	−√3
7/8	315°	7 $π$ /4	350^g	−√2/2	√2/2	−1
11/12	330°	11 $π$ /6	366 2/3^g	−1/2	√3/2	−√3/3
1	360°	2 $π$	400^g	0	1	0

Results for other angles can be found at Trigonometric constants expressed in real radicals.

Unless otherwise specified, all angles in this article are assumed to be in radians, but angles ending in a degree symbol (°) are in degrees. Per Niven's theorem multiples of 30° are the only angles that are a rational multiple of one degree and also have a rational sine or cosine, which may account for their popularity in examples.^[1]^[2]

Trigonometric functions

The primary trigonometric functions are the sine and cosine of an angle. These are sometimes abbreviated $sin(θ)$ and $cos(θ)$ , respectively, where $θ$ is the angle, but the parentheses around the angle are often omitted, e.g., $sin θ$ and $cos θ$ .

The sine of an angle is defined in the context of a right triangle, as the ratio of the length of the side that is opposite to the angle divided by the length of the longest side of the triangle (the hypotenuse).

The cosine of an angle is also defined in the context of a right triangle, as the ratio of the length of the side that is adjacent to the angle divided by the length of the longest side of the triangle (the hypotenuse).

The tangent ( $tan$ ) of an angle is the ratio of the sine to the cosine:

\tan \theta ={\frac {\sin \theta }{\cos \theta }}.

Finally, the reciprocal functions secant ( $sec$ ), cosecant ( $csc$ ), and cotangent ( $cot$ ) are the reciprocals of the cosine, sine, and tangent:

\sec \theta ={\frac {1}{\cos \theta }},\quad \csc \theta ={\frac {1}{\sin \theta }},\quad \cot \theta ={\frac {1}{\tan \theta }}={\frac {\cos \theta }{\sin \theta }}.

These definitions are sometimes referred to as ratio identities.

Inverse functions

Main article: Inverse trigonometric functions

The inverse trigonometric functions are partial inverse functions for the trigonometric functions. For example, the inverse function for the sine, known as the inverse sine ( $sin -1$ ) or arcsine ( $arcsin$ or $asin$ ), satisfies

\sin(\arcsin x)=x\quad {\text{for}}\quad |x|\leq 1

and

\arcsin(\sin x)=x\quad {\text{for}}\quad |x|\leq {\frac {\pi }{2}}.

This article uses the notation below for inverse trigonometric functions:

Function	sin	cos	tan	sec	csc	cot
Inverse	arcsin	arccos	arctan	arcsec	arccsc	arccot

Pythagorean identity

Main article: Pythagorean trigonometric identity

In trigonometry, the basic relationship between the sine and the cosine is known as the Pythagorean identity:

\sin ^{2}\theta +\cos ^{2}\theta =1\!

where $cos 2 θ$ means $(cos(θ)) 2$ and $sin 2 θ$ means $(sin(θ)) 2$ .

This can be viewed as a version of the Pythagorean theorem, and follows from the equation $x 2 + y 2 = 1$ for the unit circle. This equation can be solved for either the sine or the cosine:

{\begin{aligned}\sin \theta &=\pm {\sqrt {1-\cos ^{2}\theta }},\\\cos \theta &=\pm {\sqrt {1-\sin ^{2}\theta }}.\end{aligned}}

where the sign depends on the quadrant of $θ$ .

Related identities

Dividing the Pythagorean identity by either $cos 2 θ$ or $sin 2 θ$ yields two other identities:

1+\tan ^{2}\theta =\sec ^{2}\theta \quad {\text{and}}\quad 1+\cot ^{2}\theta =\csc ^{2}\theta .\!

Using these identities together with the ratio identities, it is possible to express any trigonometric function in terms of any other (up to a plus or minus sign):

Each trigonometric function in terms of the other five.^[3]
in terms of	$\sin \theta \!$	$\cos \theta \!$	$\tan \theta \!$	$\csc \theta \!$	$\sec \theta \!$	$\cot \theta \!$
$\sin \theta =\!$	$\sin \theta \$	$\pm {\sqrt {1-\cos ^{2}\theta }}\!$	$\pm {\frac {\tan \theta }{\sqrt {1+\tan ^{2}\theta }}}\!$	${\frac {1}{\csc \theta }}\!$	$\pm {\frac {\sqrt {\sec ^{2}\theta -1}}{\sec \theta }}\!$	$\pm {\frac {1}{\sqrt {1+\cot ^{2}\theta }}}\!$
$\cos \theta =\!$	$\pm {\sqrt {1-\sin ^{2}\theta }}\!$	$\cos \theta \!$	$\pm {\frac {1}{\sqrt {1+\tan ^{2}\theta }}}\!$	$\pm {\frac {\sqrt {\csc ^{2}\theta -1}}{\csc \theta }}\!$	${\frac {1}{\sec \theta }}\!$	$\pm {\frac {\cot \theta }{\sqrt {1+\cot ^{2}\theta }}}\!$
$\tan \theta =\!$	$\pm {\frac {\sin \theta }{\sqrt {1-\sin ^{2}\theta }}}\!$	$\pm {\frac {\sqrt {1-\cos ^{2}\theta }}{\cos \theta }}\!$	$\tan \theta \!$	$\pm {\frac {1}{\sqrt {\csc ^{2}\theta -1}}}\!$	$\pm {\sqrt {\sec ^{2}\theta -1}}\!$	${\frac {1}{\cot \theta }}\!$
$\csc \theta =\!$	${\frac {1}{\sin \theta }}\!$	$\pm {\frac {1}{\sqrt {1-\cos ^{2}\theta }}}\!$	$\pm {\frac {\sqrt {1+\tan ^{2}\theta }}{\tan \theta }}\!$	$\csc \theta \!$	$\pm {\frac {\sec \theta }{\sqrt {\sec ^{2}\theta -1}}}\!$	$\pm {\sqrt {1+\cot ^{2}\theta }}\!$
$\sec \theta =\!$	$\pm {\frac {1}{\sqrt {1-\sin ^{2}\theta }}}\!$	${\frac {1}{\cos \theta }}\!$	$\pm {\sqrt {1+\tan ^{2}\theta }}\!$	$\pm {\frac {\csc \theta }{\sqrt {\csc ^{2}\theta -1}}}\!$	$\sec \theta \!$	$\pm {\frac {\sqrt {1+\cot ^{2}\theta }}{\cot \theta }}\!$
$\cot \theta =\!$	$\pm {\frac {\sqrt {1-\sin ^{2}\theta }}{\sin \theta }}\!$	$\pm {\frac {\cos \theta }{\sqrt {1-\cos ^{2}\theta }}}\!$	${\frac {1}{\tan \theta }}\!$	$\pm {\sqrt {\csc ^{2}\theta -1}}\!$	$\pm {\frac {1}{\sqrt {\sec ^{2}\theta -1}}}\!$	$\cot \theta \!$

Historical shorthands

All of the trigonometric functions of an angle

θ

can be constructed geometrically in terms of a unit circle centered at O. Many of these terms are no longer in common use.

The versine, coversine, haversine, and exsecant were used in navigation. For example, the haversine formula was used to calculate the distance between two points on a sphere. They are rarely used today.

Name	Abbreviation	Value^[4]
versed sine, versine	$\operatorname {versin} \theta$ $\operatorname {vers} \theta$ $\operatorname {ver} \theta$	$1-\cos \theta$
versed cosine, vercosine	$\operatorname {vercosin} \theta$ $\operatorname {vercos} \theta$ $\operatorname {vcs} \theta$	$1+\cos \theta$
coversed sine, coversine	$\operatorname {coversin} \theta$ $\operatorname {covers} \theta$ $\operatorname {cvs} \theta$	$1-\sin \theta$
coversed cosine, covercosine	$\operatorname {covercosin} \theta$ $\operatorname {covercos} \theta$ $\operatorname {cvc} \theta$	$1+\sin \theta$
half versed sine, haversine	$\operatorname {haversin} \theta$ $\operatorname {hav} \theta$ $\operatorname {sem} \theta$	${\frac {1-\cos \theta }{2}}$
half versed cosine, havercosine	$\operatorname {havercosin} \theta$ $\operatorname {havercos} \theta$ $\operatorname {hvc} \theta$	${\frac {1+\cos \theta }{2}}$
half coversed sine, hacoversine cohaversine	$\operatorname {hacoversin} \theta$ $\operatorname {hacovers} \theta$ $\operatorname {hcv} \theta$	${\frac {1-\sin \theta }{2}}$
half coversed cosine, hacovercosine cohavercosine	$\operatorname {hacovercosin} \theta$ $\operatorname {hacovercos} \theta$ $\operatorname {hcc} \theta$	${\frac {1+\sin \theta }{2}}$
exterior secant, exsecant	$\operatorname {exsec} \theta$ $\operatorname {exs} \theta$	$\sec \theta -1$
exterior cosecant, excosecant	$\operatorname {excosec} \theta$ $\operatorname {excsc} \theta$ $\operatorname {exc} \theta$	$\csc \theta -1$
chord	$\operatorname {crd} \theta$	$2\sin {\frac {\theta }{2}}$

Symmetry, shifts, and periodicity

By examining the unit circle, the following properties of the trigonometric functions can be established.

Symmetry

When the trigonometric functions are reflected from certain angles, the result is often one of the other trigonometric functions. This leads to the following identities:

Reflected in $θ$ = 0^[5]	Reflected in $θ$ = $π$ /4 (co-function identities)^[6]	Reflected in $θ$ = $π$ /2
${\begin{aligned}\sin(-\theta )&=-\sin \theta \\\cos(-\theta )&=+\cos \theta \\\tan(-\theta )&=-\tan \theta \\\csc(-\theta )&=-\csc \theta \\\sec(-\theta )&=+\sec \theta \\\cot(-\theta )&=-\cot \theta \\\end{aligned}}$	${\begin{aligned}\sin({\tfrac {\pi }{2}}-\theta )&=+\cos \theta \\\cos({\tfrac {\pi }{2}}-\theta )&=+\sin \theta \\\tan({\tfrac {\pi }{2}}-\theta )&=+\cot \theta \\\csc({\tfrac {\pi }{2}}-\theta )&=+\sec \theta \\\sec({\tfrac {\pi }{2}}-\theta )&=+\csc \theta \\\cot({\tfrac {\pi }{2}}-\theta )&=+\tan \theta \\\end{aligned}}$	${\begin{aligned}\sin(\pi -\theta )&=+\sin \theta \\\cos(\pi -\theta )&=-\cos \theta \\\tan(\pi -\theta )&=-\tan \theta \\\csc(\pi -\theta )&=+\csc \theta \\\sec(\pi -\theta )&=-\sec \theta \\\cot(\pi -\theta )&=-\cot \theta \\\end{aligned}}$

Note that the sign in front of the trig function does not necessarily indicate the sign of the value. For example, $+cos θ$ does not always mean that $cos θ$ is positive. In particular, if $θ$ = $π$ , then $+cos θ$ = −1.

Shifts and periodicity

By shifting the function round by certain angles, it is often possible to find different trigonometric functions that express particular results more simply. Some examples of this are shown by shifting functions round by $π$ /2, $π$ and 2 $π$ radians. Because the periods of these functions are either $π$ or 2 $π$ , there are cases where the new function is exactly the same as the old function without the shift.

Shift by $π$ /2	Shift by $π$ Period for tan and cot^[7]	Shift by 2 $π$ Period for sin, cos, csc and sec^[8]
${\begin{aligned}\sin(\theta +{\tfrac {\pi }{2}})&=+\cos \theta \\\cos(\theta +{\tfrac {\pi }{2}})&=-\sin \theta \\\tan(\theta +{\tfrac {\pi }{2}})&=-\cot \theta \\\csc(\theta +{\tfrac {\pi }{2}})&=+\sec \theta \\\sec(\theta +{\tfrac {\pi }{2}})&=-\csc \theta \\\cot(\theta +{\tfrac {\pi }{2}})&=-\tan \theta \end{aligned}}$	${\begin{aligned}\sin(\theta +\pi )&=-\sin \theta \\\cos(\theta +\pi )&=-\cos \theta \\\tan(\theta +\pi )&=+\tan \theta \\\csc(\theta +\pi )&=-\csc \theta \\\sec(\theta +\pi )&=-\sec \theta \\\cot(\theta +\pi )&=+\cot \theta \\\end{aligned}}$	${\begin{aligned}\sin(\theta +2\pi )&=+\sin \theta \\\cos(\theta +2\pi )&=+\cos \theta \\\tan(\theta +2\pi )&=+\tan \theta \\\csc(\theta +2\pi )&=+\csc \theta \\\sec(\theta +2\pi )&=+\sec \theta \\\cot(\theta +2\pi )&=+\cot \theta \end{aligned}}$

Angle sum and difference identities

Illustration of angle addition formulae for the sine and cosine. Emphasized segment is of unit length.

These are also known as the addition and subtraction theorems or formulae. The identities can be derived by combining right triangles such as in the adjacent diagram, or by considering the invariance of the length of a chord on a unit circle given a particular central angle. Furthermore, it is even possible to derive the identities using Euler's identity although this would be a more obscure approach given that complex numbers are used.

Illustration of the angle addition formula for the tangent. Emphasized segments are of unit length.

For the angle addition diagram for the sine and cosine, the line in bold with the 1 on it is of length 1. It is the hypotenuse of a right angle triangle with angle $β$ which gives the $sin β$ and $cos β$ . The $cos β$ line is the hypotenuse of a right angle triangle with angle $α$ so it has sides $sin α$ and $cos α$ both multiplied by $cos β$ . This is the same for the $sin β$ line. The original line is also the hypotenuse of a right angle triangle with angle $α + β$ , the opposite side is the $sin(α + β)$ line up from the origin and the adjacent side is the $cos(α + β)$ segment going horizontally from the top left.

Overall the diagram can be used to show the sine and cosine of sum identities

\sin(\alpha +\beta )=\sin \alpha \cos \beta +\cos \alpha \sin \beta

\cos(\alpha +\beta )=\cos \alpha \cos \beta -\sin \alpha \sin \beta

because the opposite sides of the rectangle are equal.

Sine	$\sin(\alpha \pm \beta )=\sin \alpha \cos \beta \pm \cos \alpha \sin \beta \!$ ^[9]^[10]
Cosine	$\cos(\alpha \pm \beta )=\cos \alpha \cos \beta \mp \sin \alpha \sin \beta \,$ ^[10]^[11]
Tangent	$\tan(\alpha \pm \beta )={\frac {\tan \alpha \pm \tan \beta }{1\mp \tan \alpha \tan \beta }}$ ^[10]^[12]
Cotangent	$\cot(\alpha \pm \beta )={\frac {\cot \alpha \cot \beta \mp 1}{\cot \beta \pm \cot \alpha }}$ ^[10]^[13]
Arcsine	$\arcsin x\pm \arcsin y=\arcsin \left(x{\sqrt {1-y^{2}}}\pm y{\sqrt {1-x^{2}}}\right)$ ^[14]
Arccosine	$\arccos x\pm \arccos y=\arccos \left(xy\mp {\sqrt {\left(1-x^{2}\right)\left(1-y^{2}\right)}}\right)$ ^[15]
Arctangent	$\arctan x\pm \arctan y=\arctan \left({\frac {x\pm y}{1\mp xy}}\right)$ ^[16]
atan2	$\operatorname {atan2} (y_{1},x_{1})\pm \operatorname {atan2} (y_{2},x_{2})=\operatorname {atan2} (y_{1}x_{2}\pm y_{2}x_{1},x_{1}x_{2}\mp y_{1}y_{2})$
Arccotangent	$\operatorname {arccot} x\pm \operatorname {arccot} y=\operatorname {arccot} \left({\frac {xy\mp 1}{y\pm x}}\right)$

Matrix form

Sines and cosines of sums of infinitely many terms

\sin \left(\sum _{i=1}^{\infty }\theta _{i}\right)=\sum _{{\text{odd}}\ k\geq 1}(-1)^{\frac {k-1}{2}}\sum _{\begin{smallmatrix}A\subseteq \{\,1,2,3,\dots \,\}\\\left|A\right|=k\end{smallmatrix}}\left(\prod _{i\in A}\sin \theta _{i}\prod _{i\not \in A}\cos \theta _{i}\right)

\cos \left(\sum _{i=1}^{\infty }\theta _{i}\right)=\sum _{{\text{even}}\ k\geq 0}~(-1)^{\frac {k}{2}}~~\sum _{\begin{smallmatrix}A\subseteq \{\,1,2,3,\dots \,\}\\\left|A\right|=k\end{smallmatrix}}\left(\prod _{i\in A}\sin \theta _{i}\prod _{i\not \in A}\cos \theta _{i}\right)

In these two identities an asymmetry appears that is not seen in the case of sums of finitely many terms: in each product, there are only finitely many sine factors and cofinitely many cosine factors.

If only finitely many of the terms $θi$ are nonzero, then only finitely many of the terms on the right side will be nonzero because sine factors will vanish, and in each term, all but finitely many of the cosine factors will be unity.

Tangents of sums

Let $e k$ (for $k$ = 0, 1, 2, 3, ...) be the $k$ th-degree elementary symmetric polynomial in the variables

x_{i}=\tan \theta _{i}\,

for $i$ = 0, 1, 2, 3, ..., i.e.,

{\begin{aligned}e_{0}&=1\\[6pt]e_{1}&=\sum _{i}x_{i}&&=\sum _{i}\tan \theta _{i}\\[6pt]e_{2}&=\sum _{i<j}x_{i}x_{j}&&=\sum _{i<j}\tan \theta _{i}\tan \theta _{j}\\[6pt]e_{3}&=\sum _{i<j<k}x_{i}x_{j}x_{k}&&=\sum _{i<j<k}\tan \theta _{i}\tan \theta _{j}\tan \theta _{k}\\&{}\ \ \vdots &&{}\ \ \vdots \end{aligned}}

Then

\tan \left(\sum _{i}\theta _{i}\right)={\frac {e_{1}-e_{3}+e_{5}-\cdots }{e_{0}-e_{2}+e_{4}-\cdots }}.\!

The number of terms on the right side depends on the number of terms on the left side.

For example:

{\begin{aligned}\tan(\theta _{1}+\theta _{2})&={\frac {e_{1}}{e_{0}-e_{2}}}={\frac {x_{1}+x_{2}}{1\ -\ x_{1}x_{2}}}={\frac {\tan \theta _{1}+\tan \theta _{2}}{1\ -\ \tan \theta _{1}\tan \theta _{2}}},\\[8pt]\tan(\theta _{1}+\theta _{2}+\theta _{3})&={\frac {e_{1}-e_{3}}{e_{0}-e_{2}}}={\frac {(x_{1}+x_{2}+x_{3})\ -\ (x_{1}x_{2}x_{3})}{1\ -\ (x_{1}x_{2}+x_{1}x_{3}+x_{2}x_{3})}},\\[8pt]\tan(\theta _{1}+\theta _{2}+\theta _{3}+\theta _{4})&={\frac {e_{1}-e_{3}}{e_{0}-e_{2}+e_{4}}}\\[8pt]&={\frac {(x_{1}+x_{2}+x_{3}+x_{4})\ -\ (x_{1}x_{2}x_{3}+x_{1}x_{2}x_{4}+x_{1}x_{3}x_{4}+x_{2}x_{3}x_{4})}{1\ -\ (x_{1}x_{2}+x_{1}x_{3}+x_{1}x_{4}+x_{2}x_{3}+x_{2}x_{4}+x_{3}x_{4})\ +\ (x_{1}x_{2}x_{3}x_{4})}},\end{aligned}}

and so on. The case of only finitely many terms can be proved by mathematical induction.^[17]

Secants and cosecants of sums

{\begin{aligned}\sec \left(\sum _{i}\theta _{i}\right)&={\frac {\prod _{i}\sec \theta _{i}}{e_{0}-e_{2}+e_{4}-\cdots }}\\[8pt]\csc \left(\sum _{i}\theta _{i}\right)&={\frac {\prod _{i}\sec \theta _{i}}{e_{1}-e_{3}+e_{5}-\cdots }}\end{aligned}}

where $e k$ is the $k$ th-degree elementary symmetric polynomial in the $n$ variables $x i = tan θ i$ , $i = 1, ..., n$ , and the number of terms in the denominator and the number of factors in the product in the numerator depend on the number of terms in the sum on the left.^[18] The case of only finitely many terms can be proved by mathematical induction on the number of such terms. The convergence of the series in the denominators can be shown by writing the secant identity in the form

e_{0}-e_{2}+e_{4}-\cdots ={\frac {\prod _{i}\sec \theta _{i}}{\sec \left(\sum _{i}\theta _{i}\right)}}

and then observing that the left side converges if the right side converges, and similarly for the cosecant identity.

For example,

{\begin{aligned}\sec(\alpha +\beta +\gamma )&={\frac {\sec \alpha \sec \beta \sec \gamma }{1-\tan \alpha \tan \beta -\tan \alpha \tan \gamma -\tan \beta \tan \gamma }}\\[8pt]\csc(\alpha +\beta +\gamma )&={\frac {\sec \alpha \sec \beta \sec \gamma }{\tan \alpha +\tan \beta +\tan \gamma -\tan \alpha \tan \beta \tan \gamma }}.\end{aligned}}

Multiple-angle formulae

$T n$ is the $n$ th Chebyshev polynomial	$\cos(n\theta )=T_{n}(\cos \theta )\,$ ^[19]
$S n$ is the $n$ th spread polynomial	$\sin ^{2}(n\theta )=S_{n}(\sin ^{2}\theta )\,$
de Moivre's formula, $i$ is the imaginary unit	$\cos(n\theta )+i\sin(n\theta )=(\cos \theta +i\sin \theta )^{n}\,$ ^[20]

Double-angle, triple-angle, and half-angle formulae

Double-angle formulae

\sin(2\theta )=2\cos \theta \sin \theta

\cos(2\theta )=\cos ^{2}\theta -\sin ^{2}\theta =2\cos ^{2}\theta -1=1-2\sin ^{2}\theta ={\frac {1-\tan ^{2}\theta }{1+\tan ^{2}\theta }}

\tan(2\theta )={\frac {2\tan \theta }{1-\tan ^{2}\theta }}

\cot(2\theta )={\frac {\cot ^{2}\theta -1}{2\cot \theta }}

Triple-angle formulae

\sin(3\theta )=-\sin ^{3}\theta +3\cos ^{2}\theta \sin \theta =-4\sin ^{3}\theta +3\sin \theta

\cos(3\theta )=\cos ^{3}\theta -3\sin ^{2}\theta \cos \theta =4\cos ^{3}\theta -3\cos \theta

\tan(3\theta )={\frac {3\tan \theta -\tan ^{3}\theta }{1-3\tan ^{2}\theta }}

\cot(3\theta )={\frac {3\cot \theta -\cot ^{3}\theta }{1-3\cot ^{2}\theta }}

^[19]^[21]

Half-angle formulae

{\begin{aligned}&\sin {\frac {\theta }{2}}=\operatorname {sgn} \left(2\pi -\theta +4\pi \left\lfloor {\frac {\theta }{4\pi }}\right\rfloor \right){\sqrt {\frac {1-\cos \theta }{2}}}\\&\qquad {\text{where }}\operatorname {sgn} x=\pm 1{\text{ according as }}x{\text{ is positive or negative.}}\end{aligned}}

\sin ^{2}{\frac {\theta }{2}}={\frac {1-\cos \theta }{2}}

\cos {\frac {\theta }{2}}=\operatorname{sgn} \left(\pi +\theta +4\pi \left\lfloor {\frac {\pi -\theta }{4\pi }}\right\rfloor \right){\sqrt {{\frac {1+\cos \theta }{2}}}}

\cos ^{2}{\frac {\theta }{2}}={\frac {1+\cos \theta }{2}}

{\begin{aligned}\tan {\frac {\theta }{2}}&=\csc \theta -\cot \theta =\pm \,{\sqrt {1-\cos \theta  \over 1+\cos \theta }}={\frac {\sin \theta }{1+\cos \theta }}\\&={\frac {1-\cos \theta }{\sin \theta }}={\frac {-1\pm {\sqrt {1+\tan ^{2}\theta }}}{\tan \theta }}={\frac {\tan \theta }{1+\sec {\theta }}}\end{aligned}}

\cot {\frac {\theta }{2}}=\csc \theta +\cot \theta =\pm \,{\sqrt {1+\cos \theta \over 1-\cos \theta }}={\frac {\sin \theta }{1-\cos \theta }}={\frac {1+\cos \theta }{\sin \theta }}

^[22]^[23]

Also

\tan {\frac {\eta +\theta }{2}}={\frac {\sin \eta +\sin \theta }{\cos \eta +\cos \theta }}

\tan \left({\frac {\theta }{2}}+{\frac {\pi }{4}}\right)=\sec \theta +\tan \theta

{\sqrt {\frac {1-\sin \theta }{1+\sin \theta }}}={\frac {1-\tan {\frac {\theta }{2}}}{1+\tan {\frac {\theta }{2}}}}

Table

	Sine	Cosine	Tangent	Cotangent
Double-angle formulae^[24]^[25]	${\begin{aligned}\sin(2\theta )&=2\sin \theta \cos \theta \ \\&={\frac {2\tan \theta }{1+\tan ^{2}\theta }}\end{aligned}}$	${\begin{aligned}\cos(2\theta )&=\cos ^{2}\theta -\sin ^{2}\theta \\&=2\cos ^{2}\theta -1\\&=1-2\sin ^{2}\theta \\&={\frac {1-\tan ^{2}\theta }{1+\tan ^{2}\theta }}\end{aligned}}$	$\tan(2\theta )={\frac {2\tan \theta }{1-\tan ^{2}\theta }}$	$\cot(2\theta )={\frac {\cot ^{2}\theta -1}{2\cot \theta }}$
Triple-angle formulae^[19]^[21]	${\begin{aligned}\sin(3\theta )&=-\sin ^{3}\theta +3\cos ^{2}\theta \sin \theta \\&=-4\sin ^{3}\theta +3\sin \theta \end{aligned}}$	${\begin{aligned}\cos(3\theta )&=\cos ^{3}\theta -3\sin ^{2}\theta \cos \theta \\&=4\cos ^{3}\theta -3\cos \theta \end{aligned}}$	$\tan(3\theta )={\frac {3\tan \theta -\tan ^{3}\theta }{1-3\tan ^{2}\theta }}$	$\cot(3\theta )={\frac {3\cot \theta -\cot ^{3}\theta }{1-3\cot ^{2}\theta }}$
Half-angle formulae^[22]^[23]	$\begin{align}&\sin \frac{\theta}{2} = \sgn \left(2 \pi - \theta + 4 \pi \left\lfloor \frac{\theta}{4\pi} \right\rfloor \right) \sqrt{\frac{1 \! - \! \cos \theta}{2}} \\ \\ &\left(\mathrm{or}\,\,\sin^2\frac{\theta}{2}=\frac{1-\cos\theta}{2}\right)\end{align}$	$\begin{align}&\cos \frac{\theta}{2} = \sgn \left(\pi + \theta + 4 \pi \left\lfloor \frac{\pi - \theta}{4\pi} \right\rfloor \right) \sqrt{\frac{1 + \cos\theta}{2}} \\ \\ &\left(\mathrm{or}\,\,\cos^2\frac{\theta}{2}=\frac{1+\cos\theta}{2}\right)\end{align}$	${\begin{aligned}\tan {\frac {\theta }{2}}&=\csc \theta -\cot \theta \\&=\pm \,{\sqrt {1-\cos \theta \over 1+\cos \theta }}\\[8pt]&={\frac {\sin \theta }{1+\cos \theta }}\\[8pt]&={\frac {1-\cos \theta }{\sin \theta }}\\[10pt]\tan {\frac {\eta +\theta }{2}}&={\frac {\sin \eta +\sin \theta }{\cos \eta +\cos \theta }}\\[8pt]\tan \left({\frac {\theta }{2}}+{\frac {\pi }{4}}\right)&=\sec \theta +\tan \theta \\[8pt]{\sqrt {\frac {1-\sin \theta }{1+\sin \theta }}}&={\frac {1-\tan {\frac {\theta }{2}}}{1+\tan {\frac {\theta }{2}}}}\\[8pt]\tan {\frac {\theta }{2}}&={\frac {\tan \theta }{1+{\sqrt {1+\tan ^{2}\theta }}}}\\&{\mbox{for}}\quad \theta \in \left(-{\tfrac {\pi }{2}},{\tfrac {\pi }{2}}\right)\end{aligned}}$	$\begin{align} \cot \frac{\theta}{2} &= \csc \theta + \cot \theta \\ &= \pm\, \sqrt{1 + \cos \theta \over 1 - \cos \theta} \\[8pt] &= \frac{\sin \theta}{1 - \cos \theta} \\[8pt] &= \frac{1 + \cos \theta}{\sin \theta} \end{align}$

Sine, cosine, and tangent of multiple angles

For specific multiples, these follow from the angle addition formulas, while the general formula was given by 16th-century French mathematician François Viète.

{\begin{aligned}\sin(n\theta )&=\sum _{k{\text{ odd}}}(-1)^{\frac {k-1}{2}}{n \choose k}\cos ^{n-k}\theta \sin ^{k}\theta ,\\\cos(n\theta )&=\sum _{k{\text{ even}}}(-1)^{\frac {k}{2}}{n \choose k}\cos ^{n-k}\theta \sin ^{k}\theta \end{aligned}}

In each of these two equations, the first parenthesized term is a binomial coefficient, and the final trigonometric function equals one or minus one or zero so that half the entries in each of the sums are removed. $tan nθ$ can be written in terms of $tan θ$ using the recurrence relation:

\tan \,{\big (}(n{+}1)\theta {\big )}={\frac {\tan(n\theta )+\tan \theta }{1-\tan(n\theta )\,\tan \theta }}.

$cot nθ$ can be written in terms of $cot θ$ using the recurrence relation:

\cot \,{\big (}(n{+}1)\theta {\big )}={\frac {\cot(n\theta )\,\cot \theta -1}{\cot(n\theta )+\cot \theta }}.

Chebyshev method

The Chebyshev method is a recursive algorithm for finding the $n$ th multiple angle formula knowing the $(n - 1)$ th and $(n - 2)$ th formulae.^[26]

$cos(nx)$ can be computed from the cosine of $(n - 1) x$ and $(n - 2) x$ as follows:

\cos(nx)=2\cdot \cos x\cdot \cos {\big (}(n-1)x{\big )}-\cos {\big (}(n-2)x{\big )}\,

Similarly $sin(nx)$ can be computed from the sines of $(n - 1) x$ and $(n - 2) x$

\sin(nx)=2\cdot \cos x\cdot \sin {\big (}(n-1)x{\big )}-\sin {\big (}(n-2)x{\big )}\,

For the tangent, we have:

\tan(nx)={\frac {H+K\tan x}{K-H\tan x}}\,

where $H / K = tan(n - 1) x$ .

Tangent of an average

\tan \left({\frac {\alpha +\beta }{2}}\right)={\frac {\sin \alpha +\sin \beta }{\cos \alpha +\cos \beta }}=-\,{\frac {\cos \alpha -\cos \beta }{\sin \alpha -\sin \beta }}

Setting either $α$ or $β$ to 0 gives the usual tangent half-angle formulae.

Viète's infinite product

\cos {\theta \over 2}\cdot \cos {\theta \over 4}\cdot \cos {\theta \over 8}\cdots =\prod _{n=1}^{\infty }\cos {\theta \over 2^{n}}={\sin \theta \over \theta }=\operatorname {sinc} \,\theta .

(Refer to sinc function.)

Power-reduction formula

Obtained by solving the second and third versions of the cosine double-angle formula.

Sine	Cosine	Other
$\sin ^{2}\theta ={\frac {1-\cos(2\theta )}{2}}\!$	$\cos ^{2}\theta ={\frac {1+\cos(2\theta )}{2}}\!$	$\sin ^{2}\theta \cos ^{2}\theta ={\frac {1-\cos(4\theta )}{8}}\!$
$\sin ^{3}\theta ={\frac {3\sin \theta -\sin(3\theta )}{4}}\!$	$\cos ^{3}\theta ={\frac {3\cos \theta +\cos(3\theta )}{4}}\!$	$\sin ^{3}\theta \cos ^{3}\theta ={\frac {3\sin(2\theta )-\sin(6\theta )}{32}}\!$
$\sin ^{4}\theta ={\frac {3-4\cos(2\theta )+\cos(4\theta )}{8}}\!$	$\cos ^{4}\theta ={\frac {3+4\cos(2\theta )+\cos(4\theta )}{8}}\!$	$\sin ^{4}\theta \cos ^{4}\theta ={\frac {3-4\cos(4\theta )+\cos(8\theta )}{128}}\!$
$\sin ^{5}\theta ={\frac {10\sin \theta -5\sin(3\theta )+\sin(5\theta )}{16}}\!$	$\cos ^{5}\theta ={\frac {10\cos \theta +5\cos(3\theta )+\cos(5\theta )}{16}}\!$	$\sin ^{5}\theta \cos ^{5}\theta ={\frac {10\sin(2\theta )-5\sin(6\theta )+\sin(10\theta )}{512}}\!$

and in general terms of powers of $sin θ$ or $cos θ$ the following is true, and can be deduced using De Moivre's formula, Euler's formula and the binomial theorem .

	Cosine	Sine
${\text{if }}n{\text{ is odd}}$	$\cos ^{n}\theta ={\frac {2}{2^{n}}}\sum _{k=0}^{\frac {n-1}{2}}{\binom {n}{k}}\cos {{\big (}(n-2k)\theta {\big )}}$	$\sin ^{n}\theta ={\frac {2}{2^{n}}}\sum _{k=0}^{\frac {n-1}{2}}(-1)^{({\frac {n-1}{2}}-k)}{\binom {n}{k}}\sin {{\big (}(n-2k)\theta {\big )}}$
${\text{if }}n{\text{ is even}}$	$\cos ^{n}\theta ={\frac {1}{2^{n}}}{\binom {n}{\frac {n}{2}}}+{\frac {2}{2^{n}}}\sum _{k=0}^{{\frac {n}{2}}-1}{\binom {n}{k}}\cos {{\big (}(n-2k)\theta {\big )}}$	$\sin ^{n}\theta ={\frac {1}{2^{n}}}{\binom {n}{\frac {n}{2}}}+{\frac {2}{2^{n}}}\sum _{k=0}^{{\frac {n}{2}}-1}(-1)^{({\frac {n}{2}}-k)}{\binom {n}{k}}\cos {{\big (}(n-2k{\big )}\theta )}$

Product-to-sum and sum-to-product identities

The product-to-sum identities or prosthaphaeresis formulas can be proven by expanding their right-hand sides using the angle addition theorems. See amplitude modulation for an application of the product-to-sum formulae, and beat (acoustics) and phase detector for applications of the sum-to-product formulae.

Product-to-sum^[27]
$2\cos \theta \cos \varphi ={\cos(\theta -\varphi )+\cos(\theta +\varphi )}$
$2\sin \theta \sin \varphi ={\cos(\theta -\varphi )-\cos(\theta +\varphi )}$
$2\sin \theta \cos \varphi ={\sin(\theta +\varphi )+\sin(\theta -\varphi )}$
$2\cos \theta \sin \varphi ={\sin(\theta +\varphi )-\sin(\theta -\varphi )}$
$\tan \theta \tan \varphi ={\frac {\cos(\theta -\varphi )-\cos(\theta +\varphi )}{\cos(\theta -\varphi )+\cos(\theta +\varphi )}}$
${\begin{aligned}\prod _{k=1}^{n}\cos \theta _{k}&={\frac {1}{2^{n}}}\sum _{e\in S}\cos(e_{1}\theta _{1}+\cdots +e_{n}\theta _{n})\\[6pt]&{\text{where }}S=\{1,-1\}^{n}\end{aligned}}$

Sum-to-product^[28]
$\sin \theta \pm \sin \varphi =2\sin \left({\frac {\theta \pm \varphi }{2}}\right)\cos \left({\frac {\theta \mp \varphi }{2}}\right)$
$\cos \theta +\cos \varphi =2\cos \left({\frac {\theta +\varphi }{2}}\right)\cos \left({\frac {\theta -\varphi }{2}}\right)$
$\cos \theta -\cos \varphi =-2\sin \left({\theta +\varphi \over 2}\right)\sin \left({\theta -\varphi \over 2}\right)$

Other related identities

If $x + y + z = π$ (half circle), then
$\sin(2x)+\sin(2y)+\sin(2z)=4\sin x\sin y\sin z.\,$
Triple tangent identity: If $x + y + z = π$ (half circle), then
$\tan x+\tan y+\tan z=\tan x\tan y\tan z.\,$

In particular, the formula holds when $x$ , $y$ , and $z$ are the three angles of any triangle.

(If any of $x, y, z$ is a right angle, one should take both sides to be $\infty$ . This is neither $+\infty$ nor $-\infty$ ; for present purposes it makes sense to add just one point at infinity to the real line, that is approached by $tan θ$ as $tan θ$ either increases through positive values or decreases through negative values. This is a one-point compactification of the real line.)
Triple cotangent identity: If $x + y + z = π / 2$ (right angle or quarter circle), then
$\cot x+\cot y+\cot z=\cot x\cot y\cot z.\,$

Hermite's cotangent identity

Main article: Hermite's cotangent identity

Charles Hermite demonstrated the following identity.^[29] Suppose $a 1, ..., a n$ are complex numbers, no two of which differ by an integer multiple of $π$ . Let

A_{n,k}=\prod _{\begin{smallmatrix}1\leq j\leq n\\j\neq k\end{smallmatrix}}\cot(a_{k}-a_{j})

(in particular, $A 1,1$ , being an empty product, is 1). Then

\cot(z-a_{1})\cdots \cot(z-a_{n})=\cos {\frac {n\pi }{2}}+\sum _{k=1}^{n}A_{n,k}\cot(z-a_{k}).

The simplest non-trivial example is the case $n = 2$ :

\cot(z-a_{1})\cot(z-a_{2})=-1+\cot(a_{1}-a_{2})\cot(z-a_{1})+\cot(a_{2}-a_{1})\cot(z-a_{2}).

Ptolemy's theorem

Main article: Ptolemy's theorem

Ptolemy's theorem can be expressed in the language of modern trigonometry as:

w + x + y + z = π

, then:

{\begin{aligned}\sin(w+x)\sin(x+y)&=\sin(x+y)\sin(y+z)&{\text{(trivial)}}\\&=\sin(y+z)\sin(z+w)&{\text{(trivial)}}\\&=\sin(z+w)\sin(w+x)&{\text{(trivial)}}\\&=\sin w\sin y+\sin x\sin z.&{\text{(significant)}}\end{aligned}}

(The first three equalities are trivial rearrangements; the fourth is the substance of this identity.)

Linear combinations

For some purposes it is important to know that any linear combination of sine waves of the same period or frequency but different phase shifts is also a sine wave with the same period or frequency, but a different phase shift. This is useful in sinusoid data fitting, because the measured or observed data are linearly related to the $a$ and $b$ unknowns of the in-phase and quadrature components basis below, resulting in a simpler Jacobian, compared to that of $c$ and $φ$ .

Sine and cosine

In the case of a non-zero linear combination of a sine and cosine wave^[30] (which is just a sine wave with a phase shift of $π$ /2), we have

a\sin x+b\cos x=c\cdot \sin(x+\varphi )\,

where

c={\sqrt {a^{2}+b^{2}}},\,

and (using the atan2 function)

\varphi =\operatorname {atan2} \left(b,a\right).

Arbitrary phase shift

More generally, for an arbitrary phase shift, we have

a\sin x+b\sin(x+\theta )=c\sin(x+\varphi )\,

where

c={\sqrt {a^{2}+b^{2}+2ab\cos \theta }},\,

and

\varphi =\operatorname {atan} {\frac {b\,\sin \theta }{a+b\cos \theta }}.

More than two sinusoids

The general case reads

\sum _{i}a_{i}\sin(x+\theta _{i})=a\sin(x+\theta ),

where

a^{2}=\sum _{i,j}a_{i}a_{j}\cos(\theta _{i}-\theta _{j})

and

\tan \theta ={\frac {\sum _{i}a_{i}\sin \theta _{i}}{\sum _{i}a_{i}\cos \theta _{i}}}.

Lagrange's trigonometric identities

These identities, named after Joseph Louis Lagrange, are:^[31]^[32]

{\begin{aligned}\sum _{n=1}^{N}\sin(n\theta )&={\frac {1}{2}}\cot {\frac {\theta }{2}}-{\frac {\cos \left(\left(N+{\frac {1}{2}}\right)\theta \right)}{2\sin \left({\frac {\theta }{2}}\right)}}\\\sum _{n=1}^{N}\cos(n\theta )&=-{\frac {1}{2}}+{\frac {\sin \left(\left(N+{\frac {1}{2}}\right)\theta \right)}{2\sin \left({\frac {\theta }{2}}\right)}}\end{aligned}}

A related function is the following function of $x$ , called the Dirichlet kernel.

1+2\cos x+2\cos(2x)+2\cos(3x)+\cdots +2\cos(nx)={\frac {\sin \left(\left(n+{\frac {1}{2}}\right)x\right)}{\sin(x/2)}}.

Other sums of trigonometric functions

Sum of sines and cosines with arguments in arithmetic progression:^[33] if $α \neq 0$ , then

{\begin{aligned}&\sin \varphi +\sin(\varphi +\alpha )+\sin(\varphi +2\alpha )+\cdots \\[8pt]&{}\qquad \qquad \cdots +\sin(\varphi +n\alpha )={\frac {\sin {\frac {(n+1)\alpha }{2}}\cdot \sin(\varphi +{\frac {n\alpha }{2}})}{\sin {\frac {\alpha }{2}}}}\quad {\text{and}}\\[10pt]&\cos \varphi +\cos(\varphi +\alpha )+\cos(\varphi +2\alpha )+\cdots \\[8pt]&{}\qquad \qquad \cdots +\cos(\varphi +n\alpha )={\frac {\sin {\frac {(n+1)\alpha }{2}}\cdot \cos(\varphi +{\frac {n\alpha }{2}})}{\sin {\frac {\alpha }{2}}}}.\end{aligned}}

For any $a$ and $b$ :

a\cos x+b\sin x={\sqrt {a^{2}+b^{2}}}\cos {\big (}x-\operatorname {atan2} \,(b,a){\big )}\;

where $atan2 (y, x)$ is the generalization of $arctan (y / x)$ that covers the entire circular range.

\sec x\pm \tan x=\tan \left({\frac {\pi }{4}}\pm {\frac {x}{2}}\right).

The above identity is sometimes convenient to know when thinking about the Gudermannian function, which relates the circular and hyperbolic trigonometric functions without resorting to complex numbers.

If $x$ , $y$ , and $z$ are the three angles of any triangle, i.e. if $x + y + z = π$ , then

\cot x\cot y+\cot y\cot z+\cot z\cot x=1.\,

Certain linear fractional transformations

If $f (x)$ is given by the linear fractional transformation

f(x)={\frac {(\cos \alpha )x-\sin \alpha }{(\sin \alpha )x+\cos \alpha }},

and similarly

g(x)={\frac {(\cos \beta )x-\sin \beta }{(\sin \beta )x+\cos \beta }},

then

f{\big (}g(x){\big )}=g{\big (}f(x){\big )}={\frac {{\big (}\cos(\alpha +\beta ){\big )}x-\sin(\alpha +\beta )}{{\big (}\sin(\alpha +\beta ){\big )}x+\cos(\alpha +\beta )}}.

More tersely stated, if for all $α$ we let $f α$ be what we called $f$ above, then

f_{\alpha }\circ f_{\beta }=f_{\alpha +\beta }.\,

If $x$ is the slope of a line, then $f (x)$ is the slope of its rotation through an angle of $- α$ .

Inverse trigonometric functions

{\begin{aligned}\arcsin x+\arccos x&={\tfrac {\pi }{2}}\\\arctan x+\operatorname {arccot} x&={\tfrac {\pi }{2}}\\\arctan x+\arctan {\frac {1}{x}}&={\begin{cases}{\tfrac {\pi }{2}},&{\text{if }}x>0\\-{\tfrac {\pi }{2}},&{\text{if }}x<0\end{cases}}\end{aligned}}

Compositions of trig and inverse trig functions

{\begin{aligned}\sin(\arccos x)&={\sqrt {1-x^{2}}}&\tan(\arcsin x)&={\frac {x}{\sqrt {1-x^{2}}}}\\\sin(\arctan x)&={\frac {x}{\sqrt {1+x^{2}}}}&\tan(\arccos x)&={\frac {\sqrt {1-x^{2}}}{x}}\\\cos(\arctan x)&={\frac {1}{\sqrt {1+x^{2}}}}&\cot(\arcsin x)&={\frac {\sqrt {1-x^{2}}}{x}}\\\cos(\arcsin x)&={\sqrt {1-x^{2}}}&\cot(\arccos x)&={\frac {x}{\sqrt {1-x^{2}}}}\end{aligned}}

Relation to the complex exponential function

e^{ix}=\cos x+i\sin x\,

^[34] (Euler's formula),

e^{-ix}=\cos(-x)+i\sin(-x)=\cos x-i\sin x

e^{i\pi }=-1

(Euler's identity),

e^{2\pi i}=1

\cos x={\frac {e^{ix}+e^{-ix}}{2}}

^[35]

\sin x={\frac {e^{ix}-e^{-ix}}{2i}}

^[36]

and hence the corollary:

\tan x={\frac {\sin x}{\cos x}}={\frac {e^{ix}-e^{-ix}}{i({e^{ix}+e^{-ix}})}}

where $i 2 = -1$ .

Infinite product formulae

For applications to special functions, the following infinite product formulae for trigonometric functions are useful:^[37]^[38]

{\begin{aligned}\sin x&=x\prod _{n=1}^{\infty }\left(1-{\frac {x^{2}}{\pi ^{2}n^{2}}}\right)\\\sinh x&=x\prod _{n=1}^{\infty }\left(1+{\frac {x^{2}}{\pi ^{2}n^{2}}}\right)\\{\frac {\sin x}{x}}&=\prod _{n=1}^{\infty }\cos {\frac {x}{2^{n}}}\end{aligned}}\ \,{\begin{aligned}\cos x&=\prod _{n=1}^{\infty }\left(1-{\frac {x^{2}}{\pi ^{2}(n-{\frac {1}{2}})^{2}}}\right)\\\cosh x&=\prod _{n=1}^{\infty }\left(1+{\frac {x^{2}}{\pi ^{2}(n-{\frac {1}{2}})^{2}}}\right)\\|\sin x|&={\frac {1}{2}}\prod _{n=0}^{\infty }{\sqrt[{2^{n+1}}]{\left|\tan \left(2^{n}x\right)\right|}}\end{aligned}}

Identities without variables

The curious identity known as Morrie's law

\cos 20^{\circ }\cdot \cos 40^{\circ }\cdot \cos 80^{\circ }={\frac {1}{8}}

is a special case of an identity that contains one variable:

\prod _{j=0}^{k-1}\cos(2^{j}x)={\frac {\sin(2^{k}x)}{2^{k}\sin x}}.

The same cosine identity in radians is

\cos {\frac {\pi }{9}}\cos {\frac {2\pi }{9}}\cos {\frac {4\pi }{9}}={\frac {1}{8}}.

Similarly:

\sin 20^{\circ }\cdot \sin 40^{\circ }\cdot \sin 80^{\circ }={\frac {\sqrt {3}}{8}}

is a special case of an identity with the case x = 20:

\sin x\cdot \sin(60^{\circ }-x)\cdot \sin(60^{\circ }+x)={\frac {\sin 3x}{4}}.

For the case $x$ = 15:

\sin 15^{\circ }\cdot \sin 45^{\circ }\cdot \sin 75^{\circ }={\frac {\sqrt {2}}{8}},

\sin 15^{\circ }\cdot \sin 75^{\circ }={\frac {1}{4}}.

For the case $x$ = 10:

\sin 10^{\circ }\cdot \sin 50^{\circ }\cdot \sin 70^{\circ }={\frac {1}{8}}.

The same cosine identity is

\cos x\cdot \cos(60^{\circ }-x)\cdot \cos(60^{\circ }+x)={\frac {\cos 3x}{4}}.

Similary:

\cos 10^{\circ }\cdot \cos 50^{\circ }\cdot \cos 70^{\circ }={\frac {\sqrt {3}}{8}}.

\cos 15^{\circ }\cdot \cos 45^{\circ }\cdot \cos 75^{\circ }={\frac {\sqrt {2}}{8}},

\cos 15^{\circ }\cdot \cos 75^{\circ }={\frac {1}{4}}.

Similarly:

\tan 50^{\circ }\cdot \tan 60^{\circ }\cdot \tan 70^{\circ }=\tan 80^{\circ }.

\tan 40^{\circ }\cdot \tan 30^{\circ }\cdot \tan 20^{\circ }=\tan 10^{\circ }.

The following is perhaps not as readily generalized to an identity containing variables (but see explanation below):

\cos 24^{\circ }+\cos 48^{\circ }+\cos 96^{\circ }+\cos 168^{\circ }={\frac {1}{2}}.

Degree measure ceases to be more felicitous than radian measure when we consider this identity with 21 in the denominators:

{\begin{aligned}&\cos {\frac {2\pi }{21}}+\cos \left(2\cdot {\frac {2\pi }{21}}\right)+\cos \left(4\cdot {\frac {2\pi }{21}}\right)\\[10pt]&{}\qquad {}+\cos \left(5\cdot {\frac {2\pi }{21}}\right)+\cos \left(8\cdot {\frac {2\pi }{21}}\right)+\cos \left(10\cdot {\frac {2\pi }{21}}\right)={\frac {1}{2}}.\end{aligned}}

The factors 1, 2, 4, 5, 8, 10 may start to make the pattern clear: they are those integers less than 21/2 that are relatively prime to (or have no prime factors in common with) 21. The last several examples are corollaries of a basic fact about the irreducible cyclotomic polynomials: the cosines are the real parts of the zeroes of those polynomials; the sum of the zeroes is the Möbius function evaluated at (in the very last case above) 21; only half of the zeroes are present above. The two identities preceding this last one arise in the same fashion with 21 replaced by 10 and 15, respectively.

Other cosine identities include:^[39]

2\cos {\frac {\pi }{3}}=1,

2\cos {\frac {\pi }{5}}\times 2\cos {\frac {2\pi }{5}}=1,

2\cos {\frac {\pi }{7}}\times 2\cos {\frac {2\pi }{7}}\times 2\cos {\frac {3\pi }{7}}=1,

and so forth for all odd numbers, and hence

\cos {\frac {\pi }{3}}+\cos {\frac {\pi }{5}}\times \cos {\frac {2\pi }{5}}+\cos {\frac {\pi }{7}}\times \cos {\frac {2\pi }{7}}\times \cos {\frac {3\pi }{7}}+\dots =1.

Many of those curious identities stem from more general facts like the following:^[40]

\prod _{k=1}^{n-1}\sin {\frac {k\pi }{n}}={\frac {n}{2^{n-1}}}

and

\prod _{k=1}^{n-1}\cos {\frac {k\pi }{n}}={\frac {\sin {\frac {\pi n}{2}}}{2^{n-1}}}

Combining these gives us

\prod _{k=1}^{n-1}\tan {\frac {k\pi }{n}}={\frac {n}{\sin {\frac {\pi n}{2}}}}

If $n$ is an odd number ( $n = 2 m + 1$ ) we can make use of the symmetries to get

\prod _{k=1}^{m}\tan {\frac {k\pi }{2m+1}}={\sqrt {2m+1}}

The transfer function of the Butterworth low pass filter can be expressed in terms of polynomial and poles. By setting the frequency as the cutoff frequency, the following identity can be proved:

\prod _{k=1}^{n}\sin {\frac {\left(2k-1\right)\pi }{4n}}=\prod _{k=1}^{n}\cos {\frac {\left(2k-1\right)\pi }{4n}}={\frac {\sqrt {2}}{2^{n}}}

Computing $π$

An efficient way to compute $π$ is based on the following identity without variables, due to Machin:

{\frac {\pi }{4}}=4\arctan {\frac {1}{5}}-\arctan {\frac {1}{239}}

or, alternatively, by using an identity of Leonhard Euler:

{\frac {\pi }{4}}=5\arctan {\frac {1}{7}}+2\arctan {\frac {3}{79}}

or by using Pythagorean triples:

\pi =\arccos {\frac {4}{5}}+\arccos {\frac {5}{13}}+\arccos {\frac {16}{65}}=\arcsin {\frac {3}{5}}+\arcsin {\frac {12}{13}}+\arcsin {\frac {63}{65}}.

A useful mnemonic for certain values of sines and cosines

For certain simple angles, the sines and cosines take the form $\sqrt n / 2$ for $0 \leq n \leq 4$ , which makes them easy to remember.

{\begin{matrix}\sin 0&=&\sin 0^{\circ }&=&{\frac {\sqrt {0}}{2}}&=&\cos 90^{\circ }&=&\cos {\frac {\pi }{2}}\\\sin {\frac {\pi }{6}}&=&\sin 30^{\circ }&=&{\frac {\sqrt {1}}{2}}&=&\cos 60^{\circ }&=&\cos {\frac {\pi }{3}}\\\sin {\frac {\pi }{4}}&=&\sin 45^{\circ }&=&{\frac {\sqrt {2}}{2}}&=&\cos 45^{\circ }&=&\cos {\frac {\pi }{4}}\\\sin {\frac {\pi }{3}}&=&\sin 60^{\circ }&=&{\frac {\sqrt {3}}{2}}&=&\cos 30^{\circ }&=&\cos {\frac {\pi }{6}}\\\sin {\frac {\pi }{2}}&=&\sin 90^{\circ }&=&{\frac {\sqrt {4}}{2}}&=&\cos 0^{\circ }&=&\cos 0\\[6pt]&&&&\uparrow \\&&&&{\text{These}}\\&&&&{\text{radicands}}\\&&&&{\text{are}}\\&&&&0,\,1,\,2,\,3,\,4.\end{matrix}}

Miscellany

With the golden ratio $φ$ :

\cos {\frac {\pi }{5}}=\cos 36^{\circ }={\tfrac {1}{4}}({\sqrt {5}}+1)={\tfrac {1}{2}}\varphi

\sin {\frac {\pi }{10}}=\sin 18^{\circ }={\tfrac {1}{4}}({\sqrt {5}}-1)={\tfrac {1}{2}}\varphi ^{-1}

Also see trigonometric constants expressed in real radicals.

An identity of Euclid

Euclid showed in Book XIII, Proposition 10 of his Elements that the area of the square on the side of a regular pentagon inscribed in a circle is equal to the sum of the areas of the squares on the sides of the regular hexagon and the regular decagon inscribed in the same circle. In the language of modern trigonometry, this says:

\sin ^{2}18^{\circ }+\sin ^{2}30^{\circ }=\sin ^{2}36^{\circ }.\,

Ptolemy used this proposition to compute some angles in his table of chords.

Composition of trigonometric functions

This identity involves a trigonometric function of a trigonometric function:^[41]

\cos(t\sin x)=J_{0}(t)+2\sum _{k=1}^{\infty }J_{2k}(t)\cos(2kx)

\sin(t\sin x)=2\sum _{k=0}^{\infty }J_{2k+1}(t)\sin {\big (}(2k+1)x{\big )}

\cos(t\cos x)=J_{0}(t)+2\sum _{k=1}^{\infty }(-1)^{k}J_{2k}(t)\cos(2kx)

\sin(t\cos x)=2\sum _{k=0}^{\infty }(-1)^{k}J_{2k+1}(t)\cos {\big (}(2k+1)x{\big )}

where $J i$ are Bessel functions.

Calculus

In calculus the relations stated below require angles to be measured in radians; the relations would become more complicated if angles were measured in another unit such as degrees. If the trigonometric functions are defined in terms of geometry, along with the definitions of arc length and area, their derivatives can be found by verifying two limits. The first is:

\lim _{x\rightarrow 0}{\frac {\sin x}{x}}=1,

verified using the unit circle and squeeze theorem. The second limit is:

\lim _{x\rightarrow 0}{\frac {1-\cos x}{x}}=0,

verified using the identity $tan x / 2 = 1 - cos x / sin x$ . Having established these two limits, one can use the limit definition of the derivative and the addition theorems to show that $(sin x)' = cos x$ and $(cos x)' = -sin x$ . If the sine and cosine functions are defined by their Taylor series, then the derivatives can be found by differentiating the power series term-by-term.

{\mathrm {d} \over \mathrm {d} x}\sin x=\cos x

The rest of the trigonometric functions can be differentiated using the above identities and the rules of differentiation:^[42]^[43]^[44]

{\begin{aligned}{\mathrm {d}  \over \mathrm {d} x}\sin x&=\cos x,&{\mathrm {d}  \over \mathrm {d} x}\arcsin x&={1 \over {\sqrt {1-x^{2}}}}\\\\{\mathrm {d}  \over \mathrm {d} x}\cos x&=-\sin x,&{\mathrm {d}  \over \mathrm {d} x}\arccos x&={-1 \over {\sqrt {1-x^{2}}}}\\\\{\mathrm {d}  \over \mathrm {d} x}\tan x&=\sec ^{2}x,&{\mathrm {d}  \over \mathrm {d} x}\arctan x&={1 \over 1+x^{2}}\\\\{\mathrm {d}  \over \mathrm {d} x}\cot x&=-\csc ^{2}x,&{\mathrm {d}  \over \mathrm {d} x}\operatorname {arccot} x&={-1 \over 1+x^{2}}\\\\{\mathrm {d}  \over \mathrm {d} x}\sec x&=\tan x\sec x,&{\mathrm {d}  \over \mathrm {d} x}\operatorname {arcsec} x&={1 \over |x|{\sqrt {x^{2}-1}}}\\\\{\mathrm {d}  \over \mathrm {d} x}\csc x&=-\csc x\cot x,&{\mathrm {d}  \over \mathrm {d} x}\operatorname {arccsc} x&={-1 \over |x|{\sqrt {x^{2}-1}}}\end{aligned}}

The integral identities can be found in List of integrals of trigonometric functions. Some generic forms are listed below.

\int {\frac {\mathrm {d} u}{\sqrt {a^{2}-u^{2}}}}=\sin ^{-1}\left({\frac {u}{a}}\right)+C

\int {\frac {\mathrm {d} u}{a^{2}+u^{2}}}={\frac {1}{a}}\tan ^{-1}\left({\frac {u}{a}}\right)+C

\int {\frac {\mathrm {d} u}{u{\sqrt {u^{2}-a^{2}}}}}={\frac {1}{a}}\sec ^{-1}\left|{\frac {u}{a}}\right|+C

Implications

The fact that the differentiation of trigonometric functions (sine and cosine) results in linear combinations of the same two functions is of fundamental importance to many fields of mathematics, including differential equations and Fourier transforms.

Some differential equations satisfied by the sine function

Let $i = \sqrt -1$ be the imaginary unit and let ∘ denote composition of differential operators. Then for every odd positive integer $n$ ,

{\begin{aligned}\sum _{k=0}^{n}{\binom {n}{k}}&\left({\frac {\mathrm {d} }{\mathrm {d} x}}-\sin x\right)\circ \left({\frac {\mathrm {d} }{\mathrm {d} x}}-\sin x+i\right)\circ \cdots \\&\qquad \cdots \circ \left({\frac {\mathrm {d} }{\mathrm {d} x}}-\sin x+(k-1)i\right)(\sin x)^{n-k}=0.\end{aligned}}

(When $k$ = 0, then the number of differential operators being composed is 0, so the corresponding term in the sum above is just $(sin x) n$ .) This identity was discovered as a by-product of research in medical imaging.^[45]

Exponential definitions

Function	Inverse function^[46]
$\sin \theta ={\frac {e^{i\theta }-e^{-i\theta }}{2i}}\,$	$\arcsin x=-i\ln \left(ix+{\sqrt {1-x^{2}}}\right)\,$
$\cos \theta ={\frac {e^{i\theta }+e^{-i\theta }}{2}}\,$	$\arccos x=i\,\ln \left(x-i\,{\sqrt {1-x^{2}}}\right)\,$
$\tan \theta ={\frac {e^{i\theta }-e^{-i\theta }}{i(e^{i\theta }+e^{-i\theta })}}\,$	$\arctan x={\frac {i}{2}}\ln \left({\frac {i+x}{i-x}}\right)\,$
$\csc \theta ={\frac {2i}{e^{i\theta }-e^{-i\theta }}}\,$	$\operatorname {arccsc} x=-i\ln \left({\frac {i}{x}}+{\sqrt {1-{\frac {1}{x^{2}}}}}\right)\,$
$\sec \theta ={\frac {2}{e^{i\theta }+e^{-i\theta }}}\,$	$\operatorname {arcsec} x=-i\ln \left({\frac {1}{x}}+{\sqrt {1-{\frac {i}{x^{2}}}}}\right)\,$
$\cot \theta ={\frac {i(e^{i\theta }+e^{-i\theta })}{e^{i\theta }-e^{-i\theta }}}\,$	$\operatorname {arccot} x={\frac {i}{2}}\ln \left({\frac {x-i}{x+i}}\right)\,$

$\operatorname {cis} \,\theta =e^{i\theta }\,$	$\operatorname {arccis} \,x={\frac {\ln x}{i}}=-i\ln x=\operatorname {arg} \,x\,$

Miscellaneous

Dirichlet kernel

Main article: Dirichlet kernel

The Dirichlet kernel $D n (x)$ is the function occurring on both sides of the next identity:

1+2\cos x+2\cos(2x)+2\cos(3x)+\cdots +2\cos(nx)={\frac {\sin \left[\left(n+{\frac {1}{2}}\right)x\right\rbrack }{\sin \left({\frac {x}{2}}\right)}}.

The convolution of any integrable function of period 2 $π$ with the Dirichlet kernel coincides with the function's $n$ th-degree Fourier approximation. The same holds for any measure or generalized function.

Tangent half-angle substitution

Main article: Tangent half-angle substitution

If we set

t=\tan {\frac {x}{2}},

then^[47]

\sin x={\frac {2t}{1+t^{2}}};\qquad \cos x={\frac {1-t^{2}}{1+t^{2}}};\qquad e^{ix}={\frac {1+it}{1-it}}

where $e ix = cos x + i sin x$ , sometimes abbreviated to $cis x$ .

When this substitution of $t$ for $tan x / 2$ is used in calculus, it follows that $sin x$ is replaced by $2 t / 1 + t 2$ , $cos x$ is replaced by $1 - t 2 / 1 + t 2$ and the differential $d x$ is replaced by $2 d t / 1 + t 2$ . Thereby one converts rational functions of $sin x$ and $cos x$ to rational functions of $t$ in order to find their antiderivatives.

Notes

↑ Schaumberger, N. (1974). "A Classroom Theorem on Trigonometric Irrationalities". Two-Year College Math. J. 5: 73–76.
↑ Weisstein, Eric W. "Niven's Theorem". MathWorld.
↑ Abramowitz and Stegun, p. 73, 4.3.45
↑ Abramowitz and Stegun, p. 78, 4.3.147
↑ Abramowitz and Stegun, p. 72, 4.3.13–15
↑ The Elementary Identities
↑ Abramowitz and Stegun, p. 72, 4.3.9
↑ Abramowitz and Stegun, p. 72, 4.3.7–8
↑ Abramowitz and Stegun, p. 72, 4.3.16
1 2 3 4 Weisstein, Eric W. "Trigonometric Addition Formulas". MathWorld.
↑ Abramowitz and Stegun, p. 72, 4.3.17
↑ Abramowitz and Stegun, p. 72, 4.3.18
↑ Abramowitz and Stegun, p. 72, 4.3.19
↑ Abramowitz and Stegun, p. 80, 4.4.42
↑ Abramowitz and Stegun, p. 80, 4.4.33
↑ Abramowitz and Stegun, p. 80, 4.4.36
↑ Bronstein, Manuel (1989). "Simplification of real elementary functions". In Gonnet, G. H. Proceedings of the ACM-SIGSAM 1989 International Symposium on Symbolic and Algebraic Computation. ISSAC '89 (Portland US-OR, 1989-07). New York: ACM. pp. 207–211. doi:10.1145/74540.74566. ISBN 0-89791-325-6.
↑ Michael Hardy (August–September 2016). "On Tangents and Secants of Infinite Sums". American Mathematical Monthly. 123 (7): 701–703.
1 2 3 Weisstein, Eric W. "Multiple-Angle Formulas". MathWorld.
↑ Abramowitz and Stegun, p. 74, 4.3.48
1 2 Abramowitz and Stegun, p. 72, 4.3.27–28
1 2 Abramowitz and Stegun, p. 72, 4.3.20–22
1 2 Weisstein, Eric W. "Half-Angle Formulas". MathWorld.
↑ Abramowitz and Stegun, p. 72, 4.3.24–26
↑ Weisstein, Eric W. "Double-Angle Formulas". MathWorld.
↑ Ward, Ken. "Multiple angles recursive formula". Ken Ward's Mathematics Pages.
↑ Abramowitz and Stegun, p. 72, 4.3.31–33
↑ Abramowitz and Stegun, p. 72, 4.3.34–39
↑ Johnson, Warren P. (Apr 2010). "Trigonometric Identities à la Hermite". American Mathematical Monthly. 117 (4): 311–327.
↑ Cazelais, Gilles (18 February 2007). "Linear Combination of Sine and Cosine" (PDF).
↑ Ortiz Muñiz, Eddie (Feb 1953). "A Method for Deriving Various Formulas in Electrostatics and Electromagnetism Using Lagrange's Trigonometric Identities". American Journal of Physics. 21 (2): 140. doi:10.1119/1.1933371.
↑ Jeffrey, Alan; Dai, Hui-hui (2008). "Section 2.4.1.6". Handbook of Mathematical Formulas and Integrals (4th ed.). Academic Press. ISBN 978-0-12-374288-9.
↑ Knapp, Michael P. "Sines and Cosines of Angles in Arithmetic Progression" (PDF).
↑ Abramowitz and Stegun, p. 74, 4.3.47
↑ Abramowitz and Stegun, p. 71, 4.3.2
↑ Abramowitz and Stegun, p. 71, 4.3.1
↑ Abramowitz and Stegun, p. 75, 4.3.89–90
↑ Abramowitz and Stegun, p. 85, 4.5.68–69
↑ Humble, Steve (Nov 2004). "Grandma's identity". Mathematical Gazette. 88: 524–525.
↑ Weisstein, Eric W. "Sine". MathWorld.
↑ Milton Abramowitz and Irene Stegun, Handbook of Mathematical Functions with Formulas, Graphs, and Mathematical Tables, Dover Publications, New York, 1972, formulae 9.1.42–9.1.45
↑ Abramowitz and Stegun, p. 77, 4.3.105–110
↑ Abramowitz and Stegun, p. 82, 4.4.52–57
↑ Finney, Ross (2003). Calculus : Graphical, Numerical, Algebraic. Glenview, Illinois: Prentice Hall. pp. 159–161. ISBN 0-13-063131-0.
↑ Kuchment, Peter; Lvin, Sergey (Aug 2013). "Identities for sin x that Came from Medical Imaging". American Mathematical Monthly. 120: 609–621.
↑ Abramowitz and Stegun, p. 80, 4.4.26–31
↑ Abramowitz and Stegun, p. 72, 4.3.23

References

Abramowitz, Milton; Stegun, Irene A., eds. (1972). Handbook of Mathematical Functions with Formulas, Graphs, and Mathematical Tables. New York: Dover Publications. ISBN 978-0-486-61272-0.

External links

Construction proof for sine and cosine of the sum of two angles
Values of sin and cos, expressed in surds, for integer multiples of 3° and of 5 5/8°, and for the same angles csc and sec and tan

This article is issued from Wikipedia - version of the 11/23/2016. The text is available under the Creative Commons Attribution/Share Alike but additional terms may apply for the media files.

List of trigonometric identities

Notation

Angles

Trigonometric functions

Inverse functions

Pythagorean identity

Related identities

Historical shorthands

Symmetry, shifts, and periodicity

Symmetry

Shifts and periodicity

Angle sum and difference identities

Matrix form

Sines and cosines of sums of infinitely many terms

Tangents of sums

Secants and cosecants of sums

Multiple-angle formulae

Double-angle, triple-angle, and half-angle formulae

Double-angle formulae

Triple-angle formulae

Half-angle formulae

Table

Sine, cosine, and tangent of multiple angles

Chebyshev method

Tangent of an average

Viète's infinite product

Power-reduction formula

Product-to-sum and sum-to-product identities

Other related identities

Hermite's cotangent identity

Ptolemy's theorem

Linear combinations

Sine and cosine

Arbitrary phase shift

More than two sinusoids

Lagrange's trigonometric identities

Other sums of trigonometric functions

Certain linear fractional transformations

Inverse trigonometric functions

Compositions of trig and inverse trig functions

Relation to the complex exponential function

Infinite product formulae

Identities without variables

Computing π

A useful mnemonic for certain values of sines and cosines

Miscellany

An identity of Euclid

Composition of trigonometric functions

Calculus

Implications

Some differential equations satisfied by the sine function

Exponential definitions

Miscellaneous

Dirichlet kernel

Tangent half-angle substitution

See also

Notes

References

External links

Computing $π$