TheoremBase

Sketch: the quotient rule and the Pythagorean identity give tan' = 1/cos² > 0, hence continuity and strict increase; tan is unbounded above near π/2 and, being odd, unbounded below, so its image, an interval, is all of ℝ; the values follow from sin 0 = 0, cos 0 = 1 and sin(π/4) = cos(π/4).

Proof

Routine arithmetic and routine facts about functions are used without comment (Routine Facts, Continued: Typed Arithmetic, Maps and Predicativity); results stated for Derivative of a Real Function on an Interval are read for Derivative of a Real Function on an Interval by The Earlier and the New Versions of the Definitions of the Derivative on an Interval and of the Riemann Integral Agree (ii) and The Earlier and the New Versions of the Definitions of the Derivative on an Interval and of the Riemann Integral Agree (iii).

Write I=(−π/2,π/2)I=(-\pi/2,\pi/2). Since π>0\pi>0 by Quarter-Turn Identities and Periodicity of Sine and Cosine (i), II is an interval containing the two distinct points 00 and π/4\pi/4, so derivatives of maps I→RI\to\mathbb{R} are defined. Moreover

cos⁡x>0(x∈I)\cos x>0\qquad(x\in I)

by The Cosine Is Positive on (−π/2,π/2)(-\pi/2,\pi/2) (i); this is what makes tan⁡x=sin⁡x/cos⁡x\tan x=\sin x/\cos x meaningful on II, and it will be used repeatedly below.

The derivative. By Continuity, Derivatives and Power Series of Sine and Cosine (ii), sin⁡\sin and cos⁡\cos are differentiable on R\mathbb{R}, with sin⁡′=cos⁡\sin'=\cos and cos⁡′=−sin⁡\cos'=-\sin. Their restrictions sin⁡∣I\sin|_{I} and cos⁡∣I\cos|_{I} to the subinterval II are therefore differentiable at every x∈Ix\in I, relative to II, with the same derivatives cos⁡x\cos x and −sin⁡x-\sin x, by Restriction Stability of Continuity and of the Derivative (ii). On II the tangent is the quotient sin⁡∣I/cos⁡∣I\sin|_{I}/\cos|_{I}, and its denominator has no zero on II. The quotient rule Derivatives of Constants, the Identity, Sums, Scalar Multiples, Products, Reciprocals, Quotients and Powers (viii), applied with numerator sin⁡∣I\sin|_{I} and denominator cos⁡∣I\cos|_{I}, shows that tan⁡\tan is differentiable at every x∈Ix\in I, with

tan⁡′(x)=cos⁡x⋅cos⁡x−sin⁡x⋅(−sin⁡x)cos⁡2x=cos⁡2x+sin⁡2xcos⁡2x.\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}.

The numerator equals 11 by the Pythagorean identity The Pythagorean Identity for Sine and Cosine (i), which gives tan⁡′(x)=1/cos⁡2x\tan'(x)=1/\cos^{2}x; splitting the fraction instead gives

tan⁡′(x)=1+sin⁡2xcos⁡2x=1+tan⁡2x.\tan'(x)=1+\frac{\sin^{2}x}{\cos^{2}x}=1+\tan^{2}x .

Thus tan⁡\tan is differentiable on II, and its derivative takes the values claimed in (i).

Continuity and strict increase. Being differentiable at every point of II, tan⁡\tan is continuous at every point of II by The Increment Form of the Derivative, and Differentiability Implies Continuity (ii), that is, continuous on II. Its derivative 1/cos⁡2x1/\cos^{2}x is positive at every x∈Ix\in I. Hence The Sign and Size of the Derivative: Monotonicity, Constancy and Lipschitz Bounds (ii), applied to the continuous map tan⁡\tan on the interval II, gives tan⁡x<tan⁡y\tan x<\tan y for all x,y∈Ix,y\in I with x<yx<y: tan⁡\tan is strictly increasing on II. This proves (ii).

Unbounded above. We show that for every M>0M>0 there is x∈Ix\in I with tan⁡x>M\tan x>M. Near π/2\pi/2 the denominator cos⁡x\cos x is small and positive while the numerator sin⁡x\sin x is close to 11, and we make this precise. The functions cos⁡\cos and sin⁡\sin are continuous at π/2\pi/2, by Continuity, Derivatives and Power Series of Sine and Cosine (i), and

cos⁡π2=0,sin⁡π2=1\cos\frac{\pi}{2}=0,\qquad \sin\frac{\pi}{2}=1

by Quarter-Turn Identities and Periodicity of Sine and Cosine (ii). Let M>0M>0 be given. Choose first, by continuity of cos⁡\cos at π/2\pi/2, a δ1>0\delta_{1}>0 with ∣cos⁡t∣<1/(2M)|\cos t|<1/(2M) for every t∈Rt\in\mathbb{R} with ∣t−π/2∣<δ1|t-\pi/2|<\delta_{1}; then choose, by continuity of sin⁡\sin at π/2\pi/2, a δ2>0\delta_{2}>0 with ∣sin⁡t−1∣<1/2|\sin t-1|<1/2, and so sin⁡t>1/2\sin t>1/2, for every t∈Rt\in\mathbb{R} with ∣t−π/2∣<δ2|t-\pi/2|<\delta_{2}; and put δ=min⁡{δ1,δ2,π/2}\delta=\min\{\delta_{1},\delta_{2},\pi/2\}. The point x=π/2−δ/2x=\pi/2-\delta/2 satisfies π/4≤x<π/2\pi/4\le x<\pi/2, so it lies in (0,π/2)⊆I(0,\pi/2)\subseteq I, and ∣x−π/2∣=δ/2|x-\pi/2|=\delta/2 is less than both δ1\delta_{1} and δ2\delta_{2}. Since x∈Ix\in I, the cosine is positive there, so 0<cos⁡x<1/(2M)0<\cos x<1/(2M) and sin⁡x>1/2\sin x>1/2, and therefore

tan⁡x=sin⁡xcos⁡x>1/21/(2M)=M.\tan x=\frac{\sin x}{\cos x}>\frac{1/2}{1/(2M)}=M .

Unbounded below. The interval II is symmetric about 00: for x∈Ix\in I also −x∈I-x\in I. By Values at Zero, Parity and Double-Angle Identities for Sine and Cosine (ii), sin⁡(−x)=−sin⁡x\sin(-x)=-\sin x and cos⁡(−x)=cos⁡x\cos(-x)=\cos x, so

tan⁡(−x)=−sin⁡xcos⁡x=−tan⁡x(x∈I).\tan(-x)=\frac{-\sin x}{\cos x}=-\tan x\qquad(x\in I).

Given M>0M>0, take x∈Ix\in I with tan⁡x>M\tan x>M as in the previous paragraph; then −x∈I-x\in I and tan⁡(−x)<−M\tan(-x)<-M.

Bijectivity. Being strictly increasing, tan⁡\tan is injective: if x≠yx\neq y in II, say x<yx<y, then tan⁡x<tan⁡y\tan x<\tan y. Since tan⁡\tan is continuous on the interval II, its image J=tan⁡(I)J=\tan(I) is an interval, by Intermediate Value Theorem on a Closed Real Interval, and Continuous Images of Intervals (ii). Now let y∈Ry\in\mathbb{R} and put M=∣y∣+1>0M=|y|+1>0. The two previous paragraphs give points x1,x2∈Ix_{1},x_{2}\in I with

tan⁡x1<−M<y<M<tan⁡x2,\tan x_{1}<-M<y<M<\tan x_{2},

so yy lies between two elements of JJ, and y∈Jy\in J because JJ is an interval. Hence tan⁡\tan maps II onto R\mathbb{R}; being also injective, it is a bijection of II onto R\mathbb{R}, which is (iii).

Special values. By Values at Zero, Parity and Double-Angle Identities for Sine and Cosine (i), sin⁡0=0\sin 0=0 and cos⁡0=1\cos 0=1, so tan⁡0=0/1=0\tan 0=0/1=0. For π/4\pi/4, apply the quarter-turn identity Quarter-Turn Identities and Periodicity of Sine and Cosine (iii) at the point −π/4-\pi/4, and then Values at Zero, Parity and Double-Angle Identities for Sine and Cosine (ii):

sin⁡π4=sin⁡(−π4+π2)=cos⁡(−π4)=cos⁡π4.\sin\frac{\pi}{4}=\sin\Bigl(-\frac{\pi}{4}+\frac{\pi}{2}\Bigr)=\cos\Bigl(-\frac{\pi}{4}\Bigr)=\cos\frac{\pi}{4}.

Since π/4∈I\pi/4\in I, cos⁡(π/4)>0\cos(\pi/4)>0, so we may divide and obtain tan⁡(π/4)=1\tan(\pi/4)=1. This proves (iv).

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