Trigonometric Functions

Basis
Last updated: Tags: Elementary Function

Prerequisites

Angles, oscillations, and rotations all involve the same pair of functions — sine and cosine. At the basis level these are most cleanly defined as specific power series, in direct parallel to how exp\exp was defined in Exponential Functions. This approach avoids any appeal to geometry and gives you precise formulas for derivatives, identities, and even the definition of π\pi — all from first principles.

Power series definitions

Recall from Exponential Functions that exp(x)=k=0xk/k!\exp(x) = \sum_{k=0}^{\infty} x^k/k! converges absolutely for every xRx \in \mathbb{R}. Define two new functions by splitting this series into its even-indexed and odd-indexed terms, each with alternating signs:

cosx    k=0(1)kx2k(2k)!=1x22!+x44!x66!+(1)\cos x \;\coloneqq\; \sum_{k=0}^{\infty} \frac{(-1)^k\,x^{2k}}{(2k)!} = 1 - \frac{x^2}{2!} + \frac{x^4}{4!} - \frac{x^6}{6!} + \cdots \tag{1} sinx    k=0(1)kx2k+1(2k+1)!=xx33!+x55!x77!+(2)\sin x \;\coloneqq\; \sum_{k=0}^{\infty} \frac{(-1)^k\,x^{2k+1}}{(2k+1)!} = x - \frac{x^3}{3!} + \frac{x^5}{5!} - \frac{x^7}{7!} + \cdots \tag{2}

Both series converge absolutely for all xRx \in \mathbb{R}: the ratio test gives a ratio x2 ⁣/((2k+1)(2k+2))0|x|^2\!/\bigl((2k+1)(2k+2)\bigr) \to 0 as kk \to \infty, so convergence is absolute and uniform on every bounded interval. Uniform convergence justifies differentiating the series term-by-term.

At x=0x = 0: the constant term of the cosine series is 11 and all other terms vanish, giving cos(0)=1\cos(0) = 1. The sine series starts with xx, so sin(0)=0\sin(0) = 0.

Motivation: Euler’s formula

Why these particular series? Substitute ixix (where i2=1i^2 = -1) formally into the exponential series:

exp(ix)=k=0(ix)kk!.\exp(ix) = \sum_{k=0}^{\infty} \frac{(ix)^k}{k!}.

Separating even and odd powers, and using i2m=(1)mi^{2m} = (-1)^m and i2m+1=i(1)mi^{2m+1} = i(-1)^m, the real part is exactly the cosine series (1)(1) and the imaginary part is ii times the sine series (2)(2). This yields Euler’s formula:

exp(ix)=cosx+isinx.(3)\exp(ix) = \cos x + i\sin x. \tag{3}

At the basis level, treat (3)(3) as a motivating insight rather than a fully rigorous statement (a complete treatment requires extending exp\exp to the complex numbers). The formula makes the connection between exponentials and trigonometry vivid and will let you derive the addition formulas below in a single line.

The special case x=πx = \pi gives Euler’s identity exp(iπ)+1=0\exp(i\pi) + 1 = 0, once π\pi is defined — which you will do shortly.

Derivatives

Differentiate the series (1)(1) and (2)(2) term-by-term:

ddxcosx=k=1(1)k2kx2k1(2k)!=j=0(1)jx2j+1(2j+1)!=sinx,\frac{d}{dx}\cos x = \sum_{k=1}^{\infty} \frac{(-1)^k \cdot 2k \cdot x^{2k-1}}{(2k)!} = -\sum_{j=0}^{\infty} \frac{(-1)^j\,x^{2j+1}}{(2j+1)!} = -\sin x, ddxsinx=k=0(1)k(2k+1)x2k(2k+1)!=k=0(1)kx2k(2k)!=cosx.\frac{d}{dx}\sin x = \sum_{k=0}^{\infty} \frac{(-1)^k(2k+1)x^{2k}}{(2k+1)!} = \sum_{k=0}^{\infty} \frac{(-1)^k\,x^{2k}}{(2k)!} = \cos x.

In summary:

(cosx)=sinx,(sinx)=cosx.(4)(\cos x)' = -\sin x, \qquad (\sin x)' = \cos x. \tag{4}

Applying (4)(4) twice: (cosx)=cosx(\cos x)'' = -\cos x and (sinx)=sinx(\sin x)'' = -\sin x. Both functions therefore satisfy the simple harmonic oscillator equation y+y=0y'' + y = 0.

The Pythagorean identity

Theorem. For all xRx \in \mathbb{R}:

cos2x+sin2x=1.(5)\cos^2 x + \sin^2 x = 1. \tag{5}

Proof. Let f(x)cos2x+sin2xf(x) \coloneqq \cos^2 x + \sin^2 x. Differentiate using (4)(4):

f(x)=2cosx(sinx)+2sinxcosx=0.f'(x) = 2\cos x \cdot (-\sin x) + 2\sin x \cdot \cos x = 0.

So ff is constant on R\mathbb{R}. Evaluating at x=0x = 0:

f(0)=cos2(0)+sin2(0)=12+02=1.f(0) = \cos^2(0) + \sin^2(0) = 1^2 + 0^2 = 1.

Therefore f(x)=1f(x) = 1 for all xx. \square

The Pythagorean identity (5)(5) is the source of almost every trigonometric manipulation you will encounter. One immediate consequence: cosx1|\cos x| \leq 1 and sinx1|\sin x| \leq 1 for all xx.

Addition formulas

Theorem. For all x,yRx, y \in \mathbb{R}:

cos(x+y)=cosxcosysinxsiny,(6)\cos(x + y) = \cos x \cos y - \sin x \sin y, \tag{6} sin(x+y)=sinxcosy+cosxsiny.(7)\sin(x + y) = \sin x \cos y + \cos x \sin y. \tag{7}

Proof using Euler’s formula. Multiply the two complex exponentials:

exp(i(x+y))=exp(ix)exp(iy)=(cosx+isinx)(cosy+isiny).\exp(i(x + y)) = \exp(ix)\exp(iy) = (\cos x + i\sin x)(\cos y + i\sin y).

Expanding the right side:

=(cosxcosysinxsiny)+i(sinxcosy+cosxsiny).= (\cos x\cos y - \sin x\sin y) + i(\sin x\cos y + \cos x\sin y).

The left side equals cos(x+y)+isin(x+y)\cos(x+y) + i\sin(x+y) by (3)(3). Equating real and imaginary parts gives (6)(6) and (7)(7). \square

Setting y=xy = x in (6)(6) gives the double-angle formula cos(2x)=cos2xsin2x\cos(2x) = \cos^2 x - \sin^2 x. Combined with the Pythagorean identity (5)(5), this also gives cos(2x)=2cos2x1=12sin2x\cos(2x) = 2\cos^2 x - 1 = 1 - 2\sin^2 x.

Defining π\pi

The cosine series (1)(1) gives cos(0)=1>0\cos(0) = 1 > 0. You can show that cos(2)<0\cos(2) < 0 by examining the alternating partial sums: grouping consecutive pairs shows every partial sum from the second term onward is negative when x=2x = 2, and a careful estimate gives cos(2)<13\cos(2) < -\tfrac{1}{3}.

Since cos\cos is continuous (its series converges uniformly), the Intermediate Value Theorem guarantees at least one zero of cos\cos in the interval (0,2)(0, 2).

Definition. π\boldsymbol{\pi} is defined as twice the smallest positive zero of cos\cos:

π    2min{x>0cosx=0}.(8)\pi \;\coloneqq\; 2\cdot\min\{\,x > 0 \mid \cos x = 0\,\}. \tag{8}

From this definition, cos(π/2)=0\cos(\pi/2) = 0. Applying the Pythagorean identity (5)(5) at x=π/2x = \pi/2 forces sin2(π/2)=1\sin^2(\pi/2) = 1. Because sin\sin is positive on (0,π/2)(0,\,\pi/2) — its derivative there equals cos>0\cos > 0, and sin(0)=0\sin(0) = 0 — you get sin(π/2)=1\sin(\pi/2) = 1.

Using the addition formulas (6)(6) and (7)(7) with y=π/2y = \pi/2:

cos ⁣(x+π2)=sinx,sin ⁣(x+π2)=cosx.\cos\!\left(x + \frac{\pi}{2}\right) = -\sin x, \qquad \sin\!\left(x + \frac{\pi}{2}\right) = \cos x.

Applying this shift twice gives cos(x+π)=cosx\cos(x + \pi) = -\cos x and sin(x+π)=sinx\sin(x + \pi) = -\sin x, and one more application gives periodicity.

Periodicity

Theorem. For all xRx \in \mathbb{R}:

cos(x+2π)=cosx,sin(x+2π)=sinx.(9)\cos(x + 2\pi) = \cos x, \qquad \sin(x + 2\pi) = \sin x. \tag{9}

Proof. Apply cos(x+π)=cosx\cos(x + \pi) = -\cos x twice:

cos(x+2π)=cos((x+π)+π)=cos(x+π)=(cosx)=cosx,\cos(x + 2\pi) = \cos\bigl((x+\pi)+\pi\bigr) = -\cos(x+\pi) = -(-\cos x) = \cos x,

and similarly for sin\sin. \square

In fact 2π2\pi is the minimal period of both functions, though proving this requires confirming that cos\cos has no positive zeros smaller than π/2\pi/2.

Values at special angles

The definitions and identities you have developed so far pin down the values at the standard angles:

xxcosx\cos xsinx\sin x
001100
π/6\pi/63/2\sqrt{3}/21/21/2
π/4\pi/41/21/\sqrt{2}1/21/\sqrt{2}
π/3\pi/31/21/23/2\sqrt{3}/2
π/2\pi/20011
π\pi1-100

For π/4\pi/4: the addition formula with x=y=π/4x = y = \pi/4 and cos(π/2)=0\cos(\pi/2) = 0 gives cos2(π/4)=sin2(π/4)\cos^2(\pi/4) = \sin^2(\pi/4); combined with (5)(5), both equal 1/21/\sqrt{2}.

For π/3\pi/3: the double-angle formula gives cos(2π/3)=2cos2(π/3)1\cos(2\pi/3) = 2\cos^2(\pi/3) - 1. Because cos(2π/3)=cos(ππ/3)=cos(π/3)\cos(2\pi/3) = \cos(\pi - \pi/3) = -\cos(\pi/3) (a consequence of cos(x+π)=cosx\cos(x+\pi) = -\cos x), solving cos(π/3)=2cos2(π/3)1-\cos(\pi/3) = 2\cos^2(\pi/3) - 1 yields cos(π/3)=1/2\cos(\pi/3) = 1/2 and then sin(π/3)=3/2\sin(\pi/3) = \sqrt{3}/2 from (5)(5).

Other trigonometric functions

Four more functions are defined as ratios and reciprocals of sine and cosine.

Tangent:

tanx    sinxcosx,cosx0.\tan x \;\coloneqq\; \frac{\sin x}{\cos x}, \qquad \cos x \neq 0.

The domain of tan\tan is R{π/2+kπkZ}\mathbb{R} \setminus \{\pi/2 + k\pi \mid k \in \mathbb{Z}\} and its minimal period is π\pi.

Cotangent:

cotx    cosxsinx,sinx0.\cot x \;\coloneqq\; \frac{\cos x}{\sin x}, \qquad \sin x \neq 0.

Secant and cosecant are the reciprocals:

secx    1cosx,cscx    1sinx.\sec x \;\coloneqq\; \frac{1}{\cos x}, \qquad \csc x \;\coloneqq\; \frac{1}{\sin x}.

Derivatives of tan\tan and cot\cot

Apply the quotient rule, then use the Pythagorean identity (5)(5):

(tanx)=cosxcosxsinx(sinx)cos2x=cos2x+sin2xcos2x=1cos2x=sec2x.(10)(\tan x)' = \frac{\cos x \cdot \cos x - \sin x \cdot (-\sin x)}{\cos^2 x} = \frac{\cos^2 x + \sin^2 x}{\cos^2 x} = \frac{1}{\cos^2 x} = \sec^2 x. \tag{10} (cotx)=sinxsinxcosxcosxsin2x=cos2x+sin2xsin2x=1sin2x=csc2x.(11)(\cot x)' = \frac{-\sin x \cdot \sin x - \cos x \cdot \cos x}{\sin^2 x} = -\frac{\cos^2 x + \sin^2 x}{\sin^2 x} = -\frac{1}{\sin^2 x} = -\csc^2 x. \tag{11}

The inverse trigonometric functions — arcsin\arcsin, arccos\arccos, arctan\arctan — are defined and studied in Inverse Trigonometric Functions.

Summary

  • Cosine and sine are defined by the absolutely convergent power series (1)(1) and (2)(2); at x=0x = 0, cos(0)=1\cos(0) = 1 and sin(0)=0\sin(0) = 0.
  • Euler’s formula exp(ix)=cosx+isinx\exp(ix) = \cos x + i\sin x arises by separating real and imaginary parts of the exponential series after substituting ixix.
  • Derivatives: (cosx)=sinx(\cos x)' = -\sin x and (sinx)=cosx(\sin x)' = \cos x; both functions satisfy y+y=0y'' + y = 0.
  • Pythagorean identity: cos2x+sin2x=1\cos^2 x + \sin^2 x = 1, proved by showing the derivative of the left side is 00 and evaluating at x=0x = 0.
  • Addition formulas (6)(6) and (7)(7) are derived by expanding exp(ix)exp(iy)=exp(i(x+y))\exp(ix)\exp(iy) = \exp(i(x+y)).
  • π\pi is defined as twice the smallest positive zero of cos\cos; its existence follows from the Intermediate Value Theorem applied to the continuous function cos\cos.
  • Periodicity: cos\cos and sin\sin each have period 2π2\pi.
  • Key values: cos(π/2)=0\cos(\pi/2) = 0, sin(π/2)=1\sin(\pi/2) = 1, cos(π)=1\cos(\pi) = -1, sin(π)=0\sin(\pi) = 0, cos(π/4)=sin(π/4)=1/2\cos(\pi/4) = \sin(\pi/4) = 1/\sqrt{2}, cos(π/3)=1/2\cos(\pi/3) = 1/2, sin(π/3)=3/2\sin(\pi/3) = \sqrt{3}/2.
  • tanx=sinx/cosx\tan x = \sin x/\cos x with (tanx)=sec2x(\tan x)' = \sec^2 x; cotx=cosx/sinx\cot x = \cos x/\sin x with (cotx)=csc2x(\cot x)' = -\csc^2 x.