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Chapter 5 · Continuity and Differentiability

Exercise 5.4 · Q2: Differentiate esin⁡−1xe^{\sin^{-1}x}

Exercise 5.4Chain rule with eˣ and sin⁻¹x · Section 5.4
The question

Differentiate the following w.r.t. xx⁠:

esin⁡−1xe^{\sin^{-1} x}
Exam answer

Let y=esin⁡−1xy = e^{\sin^{-1}x}⁠. By the chain rule,

dydx=esin⁡−1x⋅ddx(sin⁡−1x)\frac{dy}{dx} = e^{\sin^{-1}x}\cdot\frac{d}{dx}(\sin^{-1}x)

∴ dydx=esin⁡−1x1−x2\therefore\ \dfrac{dy}{dx} = \dfrac{e^{\sin^{-1}x}}{\sqrt{1 - x^2}} (−1<x<1)(-1 < x < 1)⁠.

Want the reason behind every step, the basics and the checks?

The one idea this problem is built on

This is ee raised to the power sin⁡−1x\sin^{-1}x⁠: an exponential of an inverse sine. The chain rule multiplies the derivative of the outer function (ete^t⁠, which is its own derivative) by the derivative of the inner function (sin⁡−1x\sin^{-1}x⁠, whose derivative is 11−x2\frac{1}{\sqrt{1-x^2}}⁠). The care is all in the domain: sin⁡−1x\sin^{-1}x accepts only −1≤x≤1-1 \le x \le 1⁠, and its derivative exists only for −1<x<1-1 < x < 1⁠.

Given, to find, and the plan
Given
y=esin⁡−1xy = e^{\sin^{-1}x}⁠.
To find
dydx\dfrac{dy}{dx}⁠, and the values of xx where it is valid.
Plan
(1) Find the domain from the inner function sin⁡−1\sin^{-1}⁠. (2) Name inner t=sin⁡−1xt = \sin^{-1}x and outer y=ety = e^t⁠; differentiate each. (3) Multiply (chain rule). (4) Examine the end points x=±1x = \pm 1⁠.

Basics you need

1Inverse sine

sin⁡−1x\sin^{-1}x is defined only for −1≤x≤1-1 \le x \le 1⁠, and its value (the principal value) lies in [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right] (Chapter 2). Lesson: derivatives of inverse trig functions

2Derivative of sin⁡−1x\sin^{-1}x

ddxsin⁡−1x=11−x2\dfrac{d}{dx}\sin^{-1}x = \dfrac{1}{\sqrt{1-x^2}} for −1<x<1-1 < x < 1 only (Example 24 and the table after it, Section 5.3.3). Basics: derivative rules

3Theorem 5 (1)

ddtet=et\dfrac{d}{dt}e^t = e^t for every real tt⁠. Basics: exponentials and logarithms

4Chain rule

If y=f(t)y = f(t) and t=g(x)t = g(x)⁠, then dydx=dydt⋅dtdx\dfrac{dy}{dx} = \dfrac{dy}{dt}\cdot\dfrac{dt}{dx}⁠, provided both derivatives exist (Theorem 4). Basics: composite functions

Solution

  1. Where is the function defined?

    The inner function sin⁡−1x\sin^{-1}x needs −1≤x≤1-1 \le x \le 1⁠. Its value tt then lies in [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right]⁠, and ete^t is defined for every real tt⁠. So the domain of yy is the closed interval

    −1≤x≤1.-1 \le x \le 1.

    Since sin⁡−1x\sin^{-1}x increases with xx and ete^t increases with tt⁠, yy runs from e−π/2≈0.2079e^{-\pi/2} \approx 0.2079 at x=−1x = -1 up to eπ/2≈4.8105e^{\pi/2} \approx 4.8105 at x=1x = 1⁠.

    The exponential accepts any input, so it adds no restriction; the whole restriction comes from the inner function. Knowing the domain is closed matters in Step 4: the end points belong to the domain, so we must say what happens to the derivative there.
    Domain [−1,1][-1, 1] and principal range [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right] of sin⁡−1\sin^{-1}⁠, Chapter 2. Lesson: derivatives of inverse trig functions
  2. Name the inner and outer functions, and differentiate each

    Inner: t=sin⁡−1xt = \sin^{-1}x⁠. Outer: y=ety = e^t⁠.

    dtdx=11−x2,−1<x<1,dydt=et,all real t.\begin{aligned} \frac{dt}{dx} &= \frac{1}{\sqrt{1-x^2}}, \quad -1 < x < 1, \\ \frac{dy}{dt} &= e^t, \quad \text{all real } t. \end{aligned}
    To compute esin⁡−1xe^{\sin^{-1}x} you first find the angle sin⁡−1x\sin^{-1}x⁠, then raise ee to it: the job done first is the inner function. The inner derivative comes from Example 24; it needs 1−x2>01 - x^2 > 0⁠, which excludes the end points x=±1x = \pm1⁠.
    Derivative of sin⁡−1x\sin^{-1}x⁠: Example 24 and the table after it, Section 5.3.3. Derivative of ete^t⁠: Theorem 5 (1), Section 5.4. Lesson: exponential and logarithmic functions
  3. Multiply (chain rule)

    For −1<x<1-1 < x < 1⁠, both link derivatives exist, so

    dydx=dydt⋅dtdx=et⋅11−x2=esin⁡−1x1−x2.\begin{aligned} \frac{dy}{dx} &= \frac{dy}{dt}\cdot\frac{dt}{dx} = e^t\cdot\frac{1}{\sqrt{1-x^2}} \\ &= \frac{e^{\sin^{-1}x}}{\sqrt{1-x^2}}. \end{aligned}
    The outer derivative ete^t must be written back in terms of xx⁠: with t=sin⁡−1xt = \sin^{-1}x it is esin⁡−1xe^{\sin^{-1}x}⁠, the original function itself. So the derivative is "the function, divided by 1−x2\sqrt{1-x^2}". Both factors are positive, so the slope is positive everywhere on (−1,1)(-1, 1)⁠, and the graph rises (Chapter 6, Section 6.3 turns "positive derivative" into "increasing function").
    Chain rule, Theorem 4, Section 5.3.1. Lesson: the chain rule
    x y −1 −0.5 0.5 1 2 3 4 (0, 1) slope 1 at x = 0 slope → ∞ as x → 1⁻ slope → ∞ as x → −1⁺
    y=esin⁡−1xy = e^{\sin^{-1}x} on [−1,1][-1, 1]⁠. At x=0x = 0 the slope is e01=1\frac{e^0}{\sqrt{1}} = 1 (gold tangent). Towards either end the slope grows without bound and the curve meets the end points with a vertical tangent.
  4. What happens at the end points x=±1x = \pm 1⁠?

    At x=±1x = \pm1 the formula has denominator 1−1=0\sqrt{1 - 1} = 0⁠, so it gives no value there. A formula failing is not yet a proof that no derivative exists, so we test the difference quotient itself. At an end point only one side is available: from the left at x=1x = 1⁠, from the right at x=−1x = -1⁠.

    At x=1x = 1⁠, write the nearby point as x=cos⁡φx = \cos\varphi with 0<φ<π20 < \varphi < \frac{\pi}{2}⁠. Then sin⁡−1x=π2−φ\sin^{-1}x = \frac{\pi}{2} - \varphi⁠, the step is h=1−cos⁡φ>0h = 1 - \cos\varphi > 0⁠, and h→0+h \to 0^+ exactly when φ→0+\varphi \to 0^+⁠. The left-hand difference quotient is

    f(1)−f(1−h)h=eπ/2−eπ/2−φ1−cos⁡φ=eπ/2(1−e−φ)1−cos⁡φ.\begin{aligned} \frac{f(1) - f(1-h)}{h} &= \frac{e^{\pi/2} - e^{\pi/2-\varphi}}{1 - \cos\varphi} \\ &= \frac{e^{\pi/2}\left(1 - e^{-\varphi}\right)}{1 - \cos\varphi}. \end{aligned}

    Two inequalities bound it from below:

    • bottom: 1−cos⁡φ=2sin⁡2φ2≤φ221 - \cos\varphi = 2\sin^2\frac{\varphi}{2} \le \frac{\varphi^2}{2}⁠, because sin⁡t<t\sin t < t for 0<t<π20 < t < \frac{\pi}{2}⁠;
    • top: eφ≥1+φe^{\varphi} \ge 1 + \varphi⁠, so e−φ≤11+φe^{-\varphi} \le \frac{1}{1+\varphi} and 1−e−φ≥φ1+φ1 - e^{-\varphi} \ge \frac{\varphi}{1+\varphi}⁠.
    f(1)−f(1−h)h≥2eπ/2φ(1+φ),\frac{f(1) - f(1-h)}{h} \ge \frac{2e^{\pi/2}}{\varphi(1+\varphi)},

    which grows without bound as φ→0+\varphi \to 0^+⁠. At x=−1x = -1⁠, write x=−cos⁡φx = -\cos\varphi⁠: then sin⁡−1x=−π2+φ\sin^{-1}x = -\frac{\pi}{2} + \varphi⁠, and the same two inequalities give

    f(−1+h)−f(−1)h=e−π/2(eφ−1)1−cos⁡φ≥2e−π/2φ,\begin{aligned} \frac{f(-1+h) - f(-1)}{h} &= \frac{e^{-\pi/2}\left(e^{\varphi} - 1\right)}{1 - \cos\varphi} \\ &\ge \frac{2e^{-\pi/2}}{\varphi}, \end{aligned}

    which also grows without bound. So the function is defined at ±1\pm1 but is not differentiable there.

    A derivative must be a finite limit of the difference quotient (Section 5.3); at an end point of the domain the book takes the one-sided limit from inside. Here both one-sided quotients exceed any number you name once φ\varphi is small enough, so no finite limit exists. Writing the nearby point as cos⁡φ\cos\varphi turns sin⁡−1x\sin^{-1}x into the simple angle π2−φ\frac{\pi}{2} - \varphi⁠, which is why it is the convenient substitution. The two inequalities are used here, not proved: sin⁡t<t\sin t < t comes from Class XI, and es≥1+se^{s} \ge 1 + s is proved with Chapter 6 (see the table at the end).
    Differentiable at a point means the difference quotient has a finite limit (Section 5.3). Lesson: differentiability
Result ddx esin⁡−1x=esin⁡−1x1−x2,−1<x<1.\begin{aligned} &\frac{d}{dx}\,e^{\sin^{-1}x} \\ &\quad= \frac{e^{\sin^{-1}x}}{\sqrt{1-x^2}}, \qquad -1 < x < 1. \end{aligned}

The function is defined on [−1,1][-1, 1]⁠, but at x=±1x = \pm1 it has no derivative. (Textbook answer: esin⁡−1x1−x2\dfrac{e^{\sin^{-1}x}}{\sqrt{1-x^2}}⁠, x∈(−1,1)x \in (-1, 1)⁠. The same.)

Check it with numbers

Take x=0.5x = 0.5⁠. Then sin⁡−10.5=π6≈0.5235988\sin^{-1}0.5 = \frac{\pi}{6} \approx 0.5235988⁠, so eπ/6≈1.6880918e^{\pi/6} \approx 1.6880918⁠, and 1−0.25=0.75\sqrt{1 - 0.25} = \sqrt{0.75}⁠, which is about 0.86602540.8660254⁠. The formula gives

1.68809180.8660254≈1.9492405.\frac{1.6880918}{0.8660254} \approx 1.9492405.

A difference quotient of esin⁡−1xe^{\sin^{-1}x} with h=0.0001h = 0.0001 on each side of 0.50.5 gives 1.949241.94924⁠. They agree.

Common mistakes
  1. Stopping at esin⁡−1xe^{\sin^{-1}x}⁠. The exponential is its own derivative only when its exponent is plain xx⁠; here the chain rule adds the factor 11−x2\frac{1}{\sqrt{1-x^2}}⁠.
  2. Mixing up the inverse-trig derivatives. 11+x2\frac{1}{1+x^2} is the derivative of tan⁡−1x\tan^{-1}x⁠; for sin⁡−1x\sin^{-1}x it is 11−x2\frac{1}{\sqrt{1-x^2}}⁠, with a square root and a minus sign.
  3. Claiming the derivative on [−1,1][-1, 1]⁠. The function exists at ±1\pm1⁠, but its derivative does not.
What to take away
  1. ddxeg(x)=eg(x) g′(x)\dfrac{d}{dx}e^{g(x)} = e^{g(x)}\,g'(x)⁠: the exponential reproduces itself and the chain rule appends the derivative of the exponent.
  2. The derivative of a composite exists only where every link is differentiable; the end points of sin⁡−1\sin^{-1} are typical places where a function exists but has no derivative.

Every fact used, and where it comes from

FactUsed inSource
sin⁡−1\sin^{-1}⁠: domain [−1,1][-1, 1]⁠, principal range [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right]Step 1Chapter 2 (inverse trigonometric functions)
ddxsin⁡−1x=11−x2\frac{d}{dx}\sin^{-1}x = \frac{1}{\sqrt{1-x^2}}⁠, −1<x<1-1 < x < 1Step 2Example 24 and the table after it, Section 5.3.3 (Lesson: derivatives of inverse trig functions)
ddtet=et\frac{d}{dt}e^t = e^tStep 2Theorem 5 (1), Section 5.4
Chain ruleStep 3Theorem 4, Section 5.3.1
Differentiable means a finite limit of the difference quotientStep 4Definition of differentiability, Section 5.3
1−cos⁡φ=2sin⁡2φ21 - \cos\varphi = 2\sin^2\frac{\varphi}{2}Step 4Double-angle formula (Class XI trigonometry)
sin⁡t<t\sin t < t for 0<t<π20 < t < \frac{\pi}{2}Step 4Class XI, Limits and Derivatives (the inequality used to prove sin⁡xx→1\frac{\sin x}{x} \to 1⁠)
es≥1+se^{s} \ge 1 + s for s≥0s \ge 0Step 4Not proved in Chapter 5. It follows from Theorem 1 of Section 6.3 (Chapter 6): g(s)=es−1−sg(s) = e^s - 1 - s has g′(s)=es−1>0g'(s) = e^s - 1 > 0 for s>0s > 0⁠, so gg is increasing on [0,∞)[0, \infty) and g(s)≥g(0)=0g(s) \ge g(0) = 0
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