Proofs of trigonometric identities

There are several equivalent ways for defining trigonometric functions, and the proofs of the trigonometric identities between them depend on the chosen definition. The oldest and most elementary definitions are based on the geometry of right triangles. The proofs given in this article use these definitions, and thus apply to non-negative angles not greater than a right angle. For greater and negative angles, see Trigonometric functions.

Other definitions, and therefore other proofs are based on the Taylor series of sine and cosine, or on the differential equation $$f''+f=0$$ to which they are solutions.

Definitions


The six trigonometric functions are defined for every real number, except, for some of them, for angles that differ from 0 by a multiple of the right angle (90°). Referring to the diagram at the right, the six trigonometric functions of θ are, for angles smaller than the right angle:


 * $$ \sin \theta = \frac {\mathrm{opposite}}{\mathrm{hypotenuse}} = \frac {a}{h}$$


 * $$ \cos \theta = \frac {\mathrm{adjacent}}{\mathrm{hypotenuse}} = \frac {b}{h}$$


 * $$ \tan \theta = \frac {\mathrm{opposite}}{\mathrm{adjacent}} = \frac {a}{b}$$


 * $$ \cot \theta = \frac {\mathrm{adjacent}}{\mathrm{opposite}} = \frac {b}{a}$$


 * $$ \sec \theta = \frac {\mathrm{hypotenuse}}{\mathrm{adjacent}} = \frac {h}{b}$$


 * $$ \csc \theta = \frac {\mathrm{hypotenuse}}{\mathrm{opposite}} = \frac {h}{a}$$

Ratio identities
In the case of angles smaller than a right angle, the following identities are direct consequences of above definitions through the division identity
 * $$ \frac {a}{b}= \frac {\left(\frac {a}{h}\right)} {\left(\frac {b}{h}\right) }.$$

They remain valid for angles greater than 90° and for negative angles.


 * $$ \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{\mathrm{adjacent}}{\mathrm{opposite}}

= \frac { \left( \frac{\mathrm{adjacent}}{\mathrm{adjacent}} \right) } { \left( \frac {\mathrm{opposite}}{\mathrm{adjacent}} \right) } = \frac {1}{\tan \theta} = \frac {\cos \theta}{\sin \theta} $$


 * $$ \sec \theta = \frac {1}{\cos \theta} = \frac{\mathrm{hypotenuse}}{\mathrm{adjacent}} $$
 * $$ \csc \theta = \frac {1}{\sin \theta} = \frac{\mathrm{hypotenuse}}{\mathrm{opposite}} $$


 * $$ \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} $$ Or
 * $$ \tan \theta = \frac{\sin \theta}{\cos \theta}

= \frac{\left( \frac{1}{\csc \theta} \right) }{\left( \frac{1}{\sec \theta} \right) } = \frac{\left( \frac{\csc \theta \sec \theta}{\csc \theta} \right) }{\left( \frac{\csc \theta \sec \theta}{\sec \theta} \right) } = \frac{\sec \theta}{\csc \theta} $$
 * $$ \cot \theta = \frac {\csc \theta}{\sec \theta}$$

Complementary angle identities
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
Identity 1:


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

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


 * $$\tan^2\theta + 1\ = \sec^2\theta $$
 * $$\sec^2\theta - \tan^2\theta = 1 $$

Similarly


 * $$1\ + \cot^2\theta = \csc^2\theta $$
 * $$\csc^2\theta - \cot^2\theta = 1$$

Identity 2:

The following accounts for all three reciprocal functions.


 * $$ \csc^2\theta + \sec^2\theta - \cot^2\theta = 2\ + \tan^2\theta $$

Proof 2:

Refer to the triangle diagram above. Note that $$a^2+b^2=h^2$$ by Pythagorean theorem.
 * $$\csc^2\theta + \sec^2\theta = \frac{h^2}{a^2} + \frac{h^2}{b^2} = \frac{a^2+b^2}{a^2} + \frac{a^2+b^2}{b^2} = 2\ + \frac{b^2}{a^2} + \frac{a^2}{b^2}$$

Substituting with appropriate functions -


 * $$ 2\ + \frac{b^2}{a^2} + \frac{a^2}{b^2} = 2\ + \tan^2\theta+ \cot^2\theta $$

Rearranging gives:


 * $$ \csc^2\theta + \sec^2\theta - \cot^2\theta = 2\ + \tan^2\theta $$

Sine


Draw a horizontal line (the x-axis); mark an origin O. Draw a line from O at an angle $$\alpha$$ above the horizontal line and a second line at an angle $$\beta$$ above that; the angle between the second line and the x-axis is $$\alpha + \beta$$.

Place P on the line defined by $$\alpha + \beta$$ at a unit distance from the origin.

Let PQ be a line perpendicular to line OQ defined by angle $$\alpha$$, drawn from point Q on this line to point P. $$\therefore$$ OQP is a right angle.

Let QA be a perpendicular from point A on the x-axis to Q and PB be a perpendicular from point B on the x-axis to P. $$\therefore$$ OAQ and OBP are right angles.

Draw R on PB so that QR is parallel to the x-axis.

Now angle $$RPQ = \alpha$$ (because $$OQA = \frac{\pi}{2} - \alpha$$, making $$RQO = \alpha, RQP = \frac{\pi}{2}-\alpha$$, and finally $$RPQ = \alpha$$)
 * $$RPQ = \tfrac{\pi}{2} - RQP = \tfrac{\pi}{2} - (\tfrac{\pi}{2} - RQO) = RQO = \alpha$$
 * $$OP = 1$$
 * $$PQ = \sin \beta$$
 * $$OQ = \cos \beta$$
 * $$\frac{AQ}{OQ} = \sin \alpha$$, 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 the reflection identities of even and odd functions, we also get:
 * $$\sin (\alpha - \beta) = \sin \alpha \cos (-\beta) + \cos \alpha \sin (-\beta)$$
 * $$\sin (\alpha - \beta) = \sin \alpha \cos \beta - \cos \alpha \sin \beta$$

Cosine
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 the reflection identities of even and odd functions, 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,



\begin{align} \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 \\ \end{align} $$

Tangent and cotangent
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 $$ \cos \alpha \cos \beta $$, we get
 * $$\tan (\alpha + \beta) = \frac{\tan \alpha + \tan \beta}{1 - \tan \alpha \tan \beta}$$

Subtracting $$ \beta $$ from $$ \alpha $$, using $$\tan (- \beta) = -\tan \beta $$,
 * $$\tan (\alpha - \beta) = \frac{\tan \alpha + \tan (-\beta)}{1 - \tan \alpha \tan (-\beta)} = \frac{\tan \alpha - \tan \beta}{1 + \tan \alpha \tan \beta}$$

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 $$ \sin \alpha \sin \beta $$, we get
 * $$\cot (\alpha + \beta) = \frac{\cot \alpha \cot \beta - 1}{\cot \alpha + \cot \beta}$$

Or, using $$ \cot \theta = \frac{1}{\tan \theta} $$,
 * $$\cot (\alpha + \beta) = \frac{1 - \tan \alpha \tan \beta}{\tan \alpha + \tan \beta}

= \frac{\frac{1}{\tan \alpha \tan \beta} - 1}{\frac{1}{\tan \alpha} + \frac{1}{\tan \beta}} = \frac{\cot \alpha \cot \beta - 1}{\cot \alpha + \cot \beta} $$

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

Double-angle identities
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
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 2$\pi$ 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:


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

Miscellaneous – the triple tangent identity
If $$\psi + \theta + \phi = \pi = $$ half circle (for example, $$\psi$$, $$\theta$$ and $$\phi$$ are the angles of a triangle),
 * $$\tan(\psi) + \tan(\theta) + \tan(\phi) = \tan(\psi)\tan(\theta)\tan(\phi).$$

Proof:

\begin{align} \psi & = \pi - \theta - \phi \\ \tan(\psi) & = \tan(\pi - \theta - \phi) \\ & = - \tan(\theta + \phi) \\ & = \frac{- \tan\theta - \tan\phi}{1 - \tan\theta \tan\phi} \\ & = \frac{\tan\theta + \tan\phi}{\tan\theta \tan\phi - 1} \\ (\tan\theta \tan\phi - 1) \tan\psi & = \tan\theta + \tan\phi \\ \tan\psi \tan\theta \tan\phi - \tan\psi & = \tan\theta + \tan\phi \\ \tan\psi \tan\theta \tan\phi & = \tan\psi + \tan\theta + \tan\phi \\ \end{align} $$

Miscellaneous – the triple cotangent identity
If $$\psi + \theta + \phi = \tfrac{\pi}{2} = $$ quarter circle,
 * $$ \cot(\psi) + \cot(\theta) + \cot(\phi) = \cot(\psi)\cot(\theta)\cot(\phi)$$.

Proof:

Replace each of $$\psi $$, $$\theta $$, and $$\phi $$ with their complementary angles, so cotangents turn into tangents and vice versa.

Given
 * $$\psi + \theta + \phi = \tfrac{\pi}{2}$$
 * $$\therefore (\tfrac{\pi}{2}-\psi) + (\tfrac{\pi}{2}-\theta) + (\tfrac{\pi}{2}-\phi) = \tfrac{3\pi}{2} - (\psi+\theta+\phi) = \tfrac{3\pi}{2} - \tfrac{\pi}{2} = \pi $$

so the result follows from the triple tangent identity.

Sum to product identities

 * $$\sin \theta \pm \sin \phi = 2 \sin \left ( \frac{\theta\pm \phi}2 \right ) \cos \left ( \frac{\theta\mp \phi}2 \right )$$
 * $$\cos \theta + \cos \phi = 2 \cos \left ( \frac{\theta+\phi}2 \right ) \cos \left ( \frac{\theta-\phi}2 \right ) $$
 * $$\cos \theta - \cos \phi = -2 \sin \left ( \frac{\theta+\phi}2 \right ) \sin \left ( \frac{\theta-\phi}2 \right ) $$

Proof of sine identities
First, start with the sum-angle identities:
 * $$\sin (\alpha + \beta) = \sin \alpha \cos \beta + \cos \alpha \sin \beta$$
 * $$\sin (\alpha - \beta) = \sin \alpha \cos \beta - \cos \alpha \sin \beta$$

By adding these together,
 * $$\sin (\alpha + \beta) + \sin (\alpha - \beta) = \sin \alpha \cos \beta + \cos \alpha \sin \beta + \sin \alpha \cos \beta - \cos \alpha \sin \beta

= 2 \sin \alpha \cos \beta $$

Similarly, by subtracting the two sum-angle identities,
 * $$\sin (\alpha + \beta) - \sin (\alpha - \beta) = \sin \alpha \cos \beta + \cos \alpha \sin \beta - \sin \alpha \cos \beta + \cos \alpha \sin \beta

= 2 \cos \alpha \sin \beta $$

Let $$\alpha + \beta = \theta$$ and $$\alpha - \beta = \phi$$,
 * $$\therefore \alpha = \frac{\theta + \phi}2 $$ and $$\beta = \frac{\theta - \phi}2 $$

Substitute $$\theta$$ and $$\phi$$
 * $$\sin \theta + \sin \phi = 2 \sin \left( \frac{\theta + \phi}2 \right) \cos \left( \frac{\theta - \phi}2 \right) $$
 * $$\sin \theta - \sin \phi = 2 \cos \left( \frac{\theta + \phi}2 \right) \sin \left( \frac{\theta - \phi}2 \right) = 2 \sin \left( \frac{\theta - \phi}2 \right) \cos \left( \frac{\theta + \phi}2 \right) $$

Therefore,
 * $$\sin \theta \pm \sin \phi = 2 \sin \left( \frac{\theta\pm \phi}2 \right) \cos \left( \frac{\theta\mp \phi}2 \right) $$

Proof of cosine identities
Similarly for cosine, start with the sum-angle identities:
 * $$\cos (\alpha + \beta) = \cos \alpha \cos \beta\ - \sin \alpha \sin \beta$$
 * $$\cos (\alpha - \beta) = \cos \alpha \cos \beta + \sin \alpha \sin \beta$$

Again, by adding and subtracting
 * $$\cos (\alpha + \beta) + \cos (\alpha - \beta) = \cos \alpha \cos \beta\ - \sin \alpha \sin \beta + \cos \alpha \cos \beta + \sin \alpha \sin \beta = 2\cos \alpha \cos \beta$$
 * $$\cos (\alpha + \beta) - \cos (\alpha - \beta) = \cos \alpha \cos \beta\ - \sin \alpha \sin \beta - \cos \alpha \cos \beta - \sin \alpha \sin \beta

= -2 \sin \alpha \sin \beta$$

Substitute $$\theta$$ and $$\phi$$ as before,
 * $$\cos \theta + \cos \phi = 2 \cos \left( \frac{\theta+\phi}2 \right) \cos \left( \frac{\theta-\phi}2 \right) $$
 * $$\cos \theta - \cos \phi = -2 \sin \left( \frac{\theta+\phi}2 \right) \sin \left( \frac{\theta-\phi}2 \right) $$

Inequalities


The figure at the right shows a sector of a circle with radius 1. The sector is $θ/(2\pi)$ of the whole circle, so its area is $θ/2$. We assume here that $θ < \pi/2$.


 * $$OA = OD = 1$$
 * $$AB = \sin \theta$$
 * $$CD = \tan \theta$$

The area of triangle $OAD$ is $AB/2$, or $sin(θ)/2$. The area of triangle $OCD$ is $CD/2$, or $tan(θ)/2$.

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 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. For the sine function, we can handle other values. If $θ > \pi/2$, then $θ > 1$. But $sin θ ≤ 1$ (because of the Pythagorean identity), so $sin θ < θ$. So we have


 * $$\frac{\sin \theta}{\theta} < 1\ \ \ \mathrm{if}\ \ \ 0 < \theta.$$

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


 * $$\frac{\sin \theta}{\theta} = \frac{\sin (-\theta)}{-\theta} < 1.$$

Hence


 * $$\frac{\sin \theta}{\theta} < 1\quad \text{if }\quad \theta \ne 0,$$

and
 * $$\frac{\tan \theta}{\theta} > 1\quad \text{if }\quad  0 < \theta < \frac{\pi}{2}.$$

Preliminaries

 * $$\lim_{\theta \to 0}{\sin \theta} = 0$$
 * $$\lim_{\theta \to 0}{\cos \theta} = 1$$

Sine and angle ratio identity

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

In other words, the function sine is differentiable at 0, and its derivative is 1.

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


 * $$\sin \theta < \theta < \tan \theta$$,

Therefore,
 * $$\frac{\sin \theta}{\theta} < 1 < \frac{\tan \theta}{\theta}$$,

Consider the right-hand inequality. Since
 * $$\tan \theta = \frac{\sin \theta}{\cos \theta} $$
 * $$\therefore 1 < \frac{\sin \theta}{\theta \cos \theta} $$

Multiply through by $$\cos \theta $$
 * $$\cos \theta < \frac{\sin \theta}{\theta} $$

Combining with the left-hand inequality:
 * $$\cos \theta < \frac{\sin \theta}{\theta} < 1 $$

Taking $$\cos \theta $$ to the limit as $$ \theta \to 0 $$
 * $$\lim_{\theta \to 0}{\cos \theta} = 1$$

Therefore,
 * $$\lim_{\theta \to 0}{\frac{\sin \theta}{\theta}} = 1$$

Cosine and angle ratio identity

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

Proof:



\begin{align} \frac{1 - \cos \theta}{\theta} & = \frac{1 - \cos^2 \theta}{\theta (1 + \cos \theta)}\\ & = \frac{\sin^2 \theta}{\theta (1 + \cos \theta)}\\ & = \left( \frac{\sin \theta}{\theta} \right) \times \sin \theta \times \left( \frac{1}{1 + \cos \theta} \right)\\ \end{align} $$

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

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

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
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
 * $$\sin^2\theta+\cos^2\theta=1$$ (I)

Then we divide this equation (I) by $$\cos^2\theta$$


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

Then use the substitution $$\theta=\arctan(x)$$:


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

Then we use the identity $$\tan[\arctan(x)]\equiv x$$
 * $$\sin[\arctan(x)]=\frac{x}{\sqrt{x^2+1}}$$ (III)

And initial Pythagorean trigonometric identity proofed...

Similarly if we divide this equation (I) by $$\sin^2\theta$$
 * $$\sin^2\theta=\frac{\frac{1}{1}}{1+\frac{1}{\tan^2\theta}}$$ (II)
 * $$\sin^2\theta=\frac{\tan^2\theta}{\tan^2\theta+1}$$

Then use the substitution $$\theta=\arctan(x)$$:
 * $$\sin^2[\arctan(x)]=\frac{\tan^2[\arctan(x)]}{\tan^2[\arctan(x)]+1}$$

Then we use the identity $$\tan[\arctan(x)]\equiv x$$
 * $$\sin[\arctan(x)]=\frac{x}{\sqrt{x^2+1}}$$ (III)

And initial Pythagorean trigonometric identity proofed...


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


 * $$y=\frac{x}{\sqrt{x^2+1}}$$


 * $$y^2=\frac{x^2}{x^2+1}$$ (IV)

Let we guess that we have to prove:


 * $$x=\frac{y}{\sqrt{1-y^2}}$$


 * $$x^2=\frac{y^2}{1-y^2}$$ (V)

Replacing (V) into (IV) :


 * $$y^2=\frac{\frac{y^2}{(1-y^2)}}{\frac{y^2}{(1-y^2)}+1}$$


 * $$y^2=\frac{\frac{y^2}{(1-y^2)}}{\frac{1}{(1-y^2)}}$$

So it's true: $$y^2=y^2$$ and guessing statement was true: $$x=\frac{y}{\sqrt{1-y^2}}$$


 * $$[\arctan(x)]=[\arcsin(\frac{x}{\sqrt{x^2+1}})]=[\arcsin(y)]=[\arctan(\frac{y}{\sqrt{1-y^2}})]$$

Now y can be written as x ; and we have [arcsin] expressed through [arctan]...


 * $$[\arcsin(x)]=[\arctan(\frac{x}{\sqrt{1-x^2}})]$$

Similarly if we seek :$$[\arccos(x)]$$...


 * $$\cos[\arccos(x)]=x$$


 * $$\cos(\frac{\pi}{2}-(\frac{\pi}{2}-[\arccos(x)]))=x$$


 * $$\sin(\frac{\pi}{2}-[\arccos(x)])=x$$


 * $$\frac{\pi}{2}-[\arccos(x)]=[\arcsin(x)]$$


 * $$[\arccos(x)]=\frac{\pi}{2}-[\arcsin(x)]$$

From :$$[\arcsin(x)]$$...


 * $$[\arccos(x)]=\frac{\pi}{2}-[\arctan(\frac{x}{\sqrt{1-x^2}})]$$


 * $$[\arccos(x)]=\frac{\pi}{2}-[\arccot(\frac{\sqrt{1-x^2}}{x})]$$

And finally we have [arccos] expressed through [arctan]...


 * $$[\arccos(x)]=[\arctan(\frac{\sqrt{1-x^2}}{x})]$$