Proofs of trigonometric identities

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Proofs of trigonometric identities are used to show relations between trigonometric functions. This article will list trigonometric identities and prove them.

Contents

Elementary trigonometric identities [edit]

Definitions [edit]

Trigonometric functions specify the relationships between side lengths and interior angles of a right triangle. For example, the sine of angle θ is defined as being the length of the opposite side divided by the length of the hypotenuse.

Referring to the diagram at the right, the six trigonometric functions of θ are:

 \sin \theta = \frac {\mathrm{opposite}}{\mathrm{hypotenuse}} = \frac {a}{h}
 \cos \theta = \frac {\mathrm{adjacent}}{\mathrm{hypotenuse}} = \frac {b}{h}
 \tan \theta = \frac {\mathrm{opposite}}{\mathrm{adjacent}} = \frac {a}{b}
 \cot \theta = \frac {\mathrm{adjacent}}{\mathrm{opposite}} = \frac {b}{a}
 \sec \theta = \frac {\mathrm{hypotenuse}}{\mathrm{adjacent}} = \frac {h}{b}
 \csc \theta = \frac {\mathrm{hypotenuse}}{\mathrm{opposite}} = \frac {h}{a}

Ratio identities [edit]

The following identities are trivial algebraic consequences of these definitions and the division identity.
c is whatever value (not necessarily trigonometric), only to understand the simple demonstrations above. That is because not appear in the graph.

 \frac {a}{b}= \frac {\left(\frac {a}{c}\right)} {\left(\frac {b}{c}\right) }.
 \tan \theta
= \frac{\mathrm{opposite}}{\mathrm{adjacent}}
= \frac { \left( \frac{\mathrm{opposite}}{\mathrm{hypotenuse}} \right) } { \left( \frac{\mathrm{adjacent}}{\mathrm{hypotenuse}}\right) }
= \frac {\sin \theta} {\cos \theta}.
 \cot \theta = \frac {\cos \theta}{\sin \theta}.
 \cot \theta =\frac{\mathrm{adjacent}}{\mathrm{opposite}}
= \frac { \left( \frac{\mathrm{adjacent}}{\mathrm{adjacent}} \right) } { \left( \frac {\mathrm{opposite}}{\mathrm{adjacent}} \right) } = \frac {1}{\tan \theta}.
 \sec \theta = \frac {1}{\cos \theta}
 \csc \theta = \frac {1}{\sin \theta}
 \tan \theta = \frac{\mathrm{opposite}}{\mathrm{adjacent}}
= \frac{\left(\frac{\mathrm{opposite} \times \mathrm{hypotenuse}}{\mathrm{opposite} \times \mathrm{adjacent}} \right) } { \left( \frac {\mathrm{adjacent} \times \mathrm{hypotenuse}} {\mathrm{opposite} \times \mathrm{adjacent} } \right) } 
= \frac{\left( \frac{\mathrm{hypotenuse}}{\mathrm{adjacent}} \right)} { \left( \frac{\mathrm{hypotenuse}}{\mathrm{opposite}} \right)}
= \frac {\sec \theta}{\csc \theta}.
 \cot \theta = \frac {\csc \theta}{\sec \theta}.

Complementary angle identities [edit]

Two angles whose sum is π/2 radians (90 degrees) are complementary. In the diagram, the angles at vertices A and B are complementary, so we can exchange a and b, and change θ to π/2 − θ, obtaining:

 \sin\left(  \pi/2-\theta\right) = \cos \theta
 \cos\left(  \pi/2-\theta\right) = \sin \theta
 \tan\left(  \pi/2-\theta\right) = \cot \theta
 \cot\left(  \pi/2-\theta\right) = \tan \theta
 \sec\left(  \pi/2-\theta\right) = \csc \theta
 \csc\left(  \pi/2-\theta\right) = \sec \theta

Pythagorean identities [edit]

Identity 1:

\sin^2(x) + \cos^2(x) = 1\,

Proof 1:

Refer to the triangle diagram above. Note that a^2+b^2=h^2 by Pythagorean theorem.

\sin^2(x) + \cos^2(x) = \frac{a^2}{h^2} + \frac{b^2}{h^2} = \frac{a^2+b^2}{h^2} = \frac{h^2}{h^2} = 1.\,

The following two results follow from this and the ratio identities. To obtain the first, divide both sides of \sin^2(x) + \cos^2(x) = 1 by \cos^2(x); for the second, divide by \sin^2(x).

\tan^2(x) + 1\ = \sec^2(x)
\sec^2(x) - \tan^2(x) = 1\

Similarly

 1\ + \cot^2(x) = \csc^2(x)
\csc^2(x) - \cot^2(x) = 1\

Proof 2:

Differentiating the left-hand side of the identity yields:

2 \sin x \cdot \cos x - 2 \sin x \cdot \cos x = 0

Integrating this shows that the original identity is equal to a constant, and this constant can be found by plugging in any arbitrary value of x.

Identity 2:

The following accounts for all three reciprocal functions.

 \csc^2(x) + \sec^2(x) - \cot^2(x) = 2\ + \tan^2(x)

Proof 1:

Refer to the triangle diagram above. Note that a^2+b^2=h^2 by Pythagorean theorem.

\csc^2(x) + \sec^2(x) = \frac{h^2}{a^2} + \frac{h^2}{b^2} = \frac{a^2+b^2}{a^2} + \frac{a^2+b^2}{b^2} = 2\ + \frac{b^2}{a^2} + \frac{a^2}{b^2}

Substituting with appropriate functions -

 2\ + \frac{b^2}{a^2} + \frac{a^2}{b^2} = 2\ + \tan^2(x)+ \cot^2(x)

Rearranging gives:

 \csc^2(x) + \sec^2(x) - \cot^2(x) = 2\ + \tan^2(x)

Angle sum identities [edit]

Sine [edit]

Illustration of the sum formula.

Draw the angles α and β. Place P on the line defined by α + β at unit distance from the origin.

Let PQ be a perpendicular from P to the line defined by the angle α. OQP is a right angle.

Let QA be a perpendicular from Q to the x axis, and PB be a perpendicular from P to the x axis. OAQ is a right angle.

Draw QR parallel to the x-axis. Now angle RPQ = α (because RPQ = \tfrac{\pi}{2} - RQP = \tfrac{\pi}{2} - (\tfrac{\pi}{2} - RQO) = RQO = \alpha)

OP = 1\,
PQ = \sin \beta\,
OQ = \cos \beta\,
\frac{AQ}{OQ} = \sin \alpha\,, so AQ = \sin \alpha \cos \beta\,
\frac{PR}{PQ} = \cos \alpha\,, so PR = \cos \alpha \sin \beta\,
\sin (\alpha + \beta) = PB = RB+PR = AQ+PR = \sin \alpha \cos \beta + \cos \alpha \sin \beta\,

By substituting -\beta for \beta and using Symmetry, we also get:

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

Another simple "proof" can be given using Euler's formula known from complex analysis: Euler's formula is:

e^{i\varphi}=\cos \varphi +i \sin \varphi

Although it is more precise to say that Euler's formula entails the trigonometric identities, it follows that for angles \alpha and \beta we have:

e^{i (\alpha + \beta)} = \cos (\alpha +\beta) + i \sin(\alpha +\beta)

Also using the following properties of exponential functions:

e^{i(\alpha + \beta)} = e^{i \alpha} e^{i\beta}= (\cos \alpha +i \sin \alpha) (\cos \beta + i \sin \beta)

Evaluating the product:

e^{i(\alpha + \beta)} = (\cos \alpha \cos \beta - \sin \alpha \sin \beta)+i(\sin \alpha \cos \beta + \sin \beta \cos \alpha)

This will only be equal to the previous expression we got, if the imaginary and real parts are equal respectively. Hence we get:

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

Cosine [edit]

Using the figure above,

OP = 1\,
PQ = \sin \beta\,
OQ = \cos \beta\,
\frac{OA}{OQ} = \cos \alpha\,, so OA = \cos \alpha \cos \beta\,
\frac{RQ}{PQ} = \sin \alpha\,, so RQ = \sin \alpha \sin \beta\,
\cos (\alpha + \beta) = OB = OA-BA = OA-RQ = \cos \alpha \cos \beta\ - \sin \alpha \sin \beta\,

By substituting -\beta for \beta and using Symmetry, we also get:

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

Also, using the complementary angle formulae,

\cos (\alpha + \beta) = \sin\left(  \pi/2-(\alpha + \beta)\right) = \sin\left(  (\pi/2-\alpha) - \beta\right)\,
= \sin\left(  \pi/2-\alpha\right) \cos \beta - \cos\left(  \pi/2-\alpha\right) \sin \beta\,
= \cos \alpha \cos \beta - \sin \alpha \sin \beta\,

Tangent and cotangent [edit]

From the sine and cosine formulae, we get

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

Dividing both numerator and denominator by cos α cos β, we get

\tan (\alpha + \beta) = \frac{\tan \alpha + \tan \beta}{1 - \tan \alpha \tan \beta}\,
\tan (\alpha - \beta) = \frac{\tan \alpha - \tan \beta}{1 + \tan \alpha \tan \beta}\,

Similarly from the sine and cosine formulae, we get

\cot (\alpha + \beta) = \frac{\cos (\alpha + \beta)}{\sin (\alpha + \beta)}\,
= \frac{\cos \alpha \cos \beta - \sin \alpha \sin \beta}{\sin \alpha \cos \beta + \cos \alpha \sin \beta}\,

Then by dividing both numerator and denominator by sin α sin β, we get

\cot (\alpha + \beta) = \frac{\cot \alpha \cot \beta - 1}{\cot \alpha + \cot \beta}\,
\cot (\alpha - \beta) = \frac{\cot \alpha \cot \beta + 1}{\cot \beta - \cot \alpha}\,

Double-angle identities [edit]

From the angle sum identities, we get

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

and

\cos (2 \theta) = \cos^2 \theta - \sin^2 \theta\,

The Pythagorean identities give the two alternative forms for the latter of these:

\cos (2 \theta) = 2 \cos^2 \theta - 1\,
\cos (2 \theta) = 1 - 2 \sin^2 \theta\,

The angle sum identities also give

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

It can also be proved using Euler's formula

 e^{i \varphi}=\cos \varphi +i \sin \varphi

Squaring both sides yields

 e^{i 2\varphi}=(\cos \varphi +i \sin \varphi)^{2}

But replacing the angle with its doubled version, which achieves the same result in the left side of the equation, yields

 e^{i 2\varphi}=\cos 2\varphi +i \sin 2\varphi

It follows that

(\cos \varphi +i \sin \varphi)^{2}=\cos 2\varphi +i \sin 2\varphi.

Expanding the square and simplifying on the left hand side of the equation gives

i(2 \sin \varphi \cos \varphi) + \cos^2 \varphi - \sin^2 \varphi\ = \cos 2\varphi +i \sin 2\varphi.

Because the imaginary and real parts have to be the same, we are left with the original identities

\cos^2 \varphi - \sin^2 \varphi\ = \cos 2\varphi,

and also

2 \sin \varphi \cos \varphi = \sin 2\varphi.

Half-angle identities [edit]

The two identities giving the alternative forms for cos 2θ lead to the following equations:

\cos \frac{\theta}{2} = \pm\, \sqrt\frac{1 + \cos \theta}{2},\,
\sin \frac{\theta}{2} = \pm\, \sqrt\frac{1 - \cos \theta}{2}.\,

The sign of the square root needs to be chosen properly—note that if 2π is added to θ, the quantities inside the square roots are unchanged, but the left-hand-sides of the equations change sign. Therefore the correct sign to use depends on the value of θ.

For the tan function, the equation is:

\tan \frac{\theta}{2} = \pm\, \sqrt\frac{1 - \cos \theta}{1 + \cos \theta}.\,

Then multiplying the numerator and denominator inside the square root by (1 + cos θ) and using Pythagorean identities leads to:

\tan \frac{\theta}{2} = \frac{\sin \theta}{1 + \cos \theta}.\,

Also, if the numerator and denominator are both multiplied by (1 - cos θ), the result is:

\tan \frac{\theta}{2} = \frac{1 - \cos \theta}{\sin \theta}.\,

This also gives:

\tan \frac{\theta}{2} = \csc \theta - \cot \theta.\,

Similar manipulations for the cot function give:

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

Prosthaphaeresis identities [edit]

  • \sin \theta \pm \sin y = 2 \sin \frac{\theta\pm y}2 \cos \frac{\theta\mp y}2
  • \cos \theta + \cos y = 2 \cos \frac{\theta+y}2 \cos \frac{\theta-y}2
  • \cos \theta - \cos y = -2 \sin \frac{\theta+y}2 \sin \frac{\theta-y}2

Inequalities [edit]

Illustration of the sine and tangent inequalities.

The figure at the right shows a sector of a circle with radius 1. The sector is θ/(2π) of the whole circle, so its area is θ/2.

OA = OD = 1\,
AB = \sin \theta\,
CD = \tan \theta\,

The area of triangle OAD is AB/2, or sinθ/2. The area of triangle OCD is CD/2, or tanθ/2.

Since triangle OAD lies completely inside the sector, which in turn lies completely inside triangle OCD, we have

\sin \theta < \theta < \tan \theta\,

This geometric argument applies if 0<θ<π/2. It relies on definitions of arc length and area, which act as assumptions, so it is rather a condition imposed in construction of trigonometric functions than a provable property.[1] For the sine function, we can handle other values. If θ>π/2, then θ>1. But sinθ≤1 (because of the Pythagorean identity), so sinθ<θ. So we have

\frac{\sin \theta}{\theta} < 1\ \ \ \mathrm{if}\ \ \ 0 < \theta\,

For negative values of θ we have, by symmetry of the sine function

\frac{\sin \theta}{\theta} = \frac{\sin (-\theta)}{-\theta} < 1\,

Hence

\frac{\sin \theta}{\theta} < 1\ \ \ \mathrm{if}\ \ \ \theta \ne 0\,
\frac{\tan \theta}{\theta} > 1\ \ \ \mathrm{if}\ \ \ 0 < \theta < \frac{\pi}{2}\,

Identities involving calculus [edit]

Preliminaries [edit]

\lim_{\theta \to 0}{\sin \theta} = 0\,
\lim_{\theta \to 0}{\cos \theta} = 1\,

These can be seen from looking at the diagrams.

Sine and angle ratio identity [edit]

\lim_{\theta \to 0}{\frac{\sin \theta}{\theta}} = 1

Proof: From the previous inequalities, we have, for small angles

\sin \theta < \theta < \tan \theta\,, so
\frac{\sin \theta}{\theta} < 1 < \frac{\tan \theta}{\theta}\,, so
\frac{\sin \theta}{\theta \cos \theta} > 1\,, or
\frac{\sin \theta}{\theta} >  \cos \theta\,, so
\cos \theta < \frac{\sin \theta}{\theta} < 1\,, but
\lim_{\theta \to 0}{\cos \theta} = 1\,, so
\lim_{\theta \to 0}{\frac{\sin \theta}{\theta}} = 1

Cosine and angle ratio identity [edit]

\lim_{\theta \to 0}\frac{1 - \cos \theta}{\theta} = 0\,

Proof:

\frac{1 - \cos \theta}{\theta} = \frac{1 - \cos^2 \theta}{\theta (1 + \cos \theta)}\,
= \frac{\sin^2 \theta}{\theta (1 + \cos \theta)}\,
= \frac{\sin \theta}{\theta} \times \sin \theta \times \frac{1}{1 + \cos \theta}.\,

The limits of those three quantities are 1, 0, and 1/2, so the resultant limit is zero.

Cosine and square of angle ratio identity [edit]

 \lim_{\theta \to 0}\frac{1 - \cos \theta}{\theta^2}  = \frac{1}{2}

Proof:

As in the preceding proof,

\frac{1 - \cos \theta}{\theta^2} = \frac{\sin \theta}{\theta} \times \frac{\sin \theta}{\theta} \times \frac{1}{1 + \cos \theta}.\,

The limits of those three quantities are 1, 1, and 1/2, so the resultant limit is 1/2.

Proof of Compositions of trig and inverse trig functions [edit]

All these functions follow from the Pythagorean trigonometric identity. We can prove for instance the function

\sin[\arctan(x)]=\frac{x}{\sqrt{1+x^2}}

Proof:

We start from

\sin^2\theta+\cos^2\theta=1

Then we divide this equation by \cos^2\theta

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

Then use the substitution \theta=arctan(x), also use the Pythagorean trigonometric identity:

1-\sin^2[\arctan(x)]=\frac{1}{\tan^2[\arctan(x)]+1}

Then we use the identity \tan[\arctan(x)]\equiv x

\sin[\arctan(x)]=\frac{x}{\sqrt{x^2+1}}

See also [edit]

References [edit]

  • E. T. Whittaker and G. N. Watson. A course of modern analysis, Cambridge University Press, 1952
  1. ^ Richman, Fred (March 1993). . "A Circular Argument". The College Mathematics Journal 24 (2): 160–162. Retrieved 3 November 2012.