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Chapter 5 · Continuity and Differentiability

Miscellaneous · Q13: y=sin⁡−1x+sin⁡−11−x2y=\sin^{-1}x+\sin^{-1}\sqrt{1-x^2} is constant on (0,1)(0,1)

Miscellaneous ExerciseDerivatives of inverse trigonometric functions · Miscellaneous Exercise
The question

Find dydx\dfrac{dy}{dx}⁠, if y=sin⁡−1x+sin⁡−11−x2y = \sin^{-1} x + \sin^{-1}\sqrt{1 - x^2}⁠, 0<x<10 < x < 1⁠.

Exam answer

Put x=sin⁡θx = \sin\theta⁠, θ=sin⁡−1x\theta = \sin^{-1}x⁠. As 0<x<10 \lt x \lt 1⁠, 0<θ<π20 \lt \theta \lt \frac{\pi}{2}⁠, so cos⁡θ>0\cos\theta \gt 0⁠.

1−x2=1−sin⁡2θ=cos⁡θ=sin⁡(π2−θ)\begin{aligned} \sqrt{1 - x^2} &= \sqrt{1 - \sin^2\theta} = \cos\theta \\ &= \sin\Big(\frac{\pi}{2} - \theta\Big) \end{aligned}

Since π2−θ∈(0,π2)\frac{\pi}{2} - \theta \in \big(0, \frac{\pi}{2}\big)⁠,

y=θ+sin⁡−1(sin⁡(π2−θ))=θ+π2−θ=π2\begin{aligned} y &= \theta + \sin^{-1}\Big(\sin\Big(\frac{\pi}{2} - \theta\Big)\Big) \\ &= \theta + \frac{\pi}{2} - \theta = \frac{\pi}{2} \end{aligned}

∴ dydx=0\therefore\ \dfrac{dy}{dx} = 0 (0<x<1)(0 \lt x \lt 1)

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

The one idea this problem is built on

If x=sin⁡θx = \sin\theta with θ\theta between 0 and π2\frac{\pi}{2}⁠, then 1−x2=cos⁡θ\sqrt{1-x^2} = \cos\theta⁠, which is the sine of the complementary angle π2−θ\frac{\pi}{2} - \theta⁠. The two inverse sines are the two acute angles of one right triangle, so they always add up to π2\frac{\pi}{2}⁠. A function that is constant has derivative 0.

Given, to find, and the plan
Given
y=sin⁡−1x+sin⁡−11−x2y = \sin^{-1} x + \sin^{-1}\sqrt{1 - x^2} for 0<x<10 < x < 1⁠.
To find
dydx\dfrac{dy}{dx}⁠.
Plan
(1) Check that yy is defined. (2) Put x=sin⁡θx = \sin\theta and check that this is legitimate. (3) Show the second term equals π2−θ\frac{\pi}{2} - \theta⁠, checking the principal range. (4) Conclude y=π2y = \frac{\pi}{2}⁠, so dydx=0\frac{dy}{dx} = 0⁠. (5) Confirm by differentiating term by term with the chain rule.

Basics you need

1Principal value of sin⁡−1\sin^{-1}

sin⁡−1u\sin^{-1} u is defined for −1≤u≤1-1 \le u \le 1 and its value always lies in [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right]⁠. So sin⁡−1(sin⁡ϕ)=ϕ\sin^{-1}(\sin\phi) = \phi only when ϕ\phi is in that interval (Chapter 2, Sections 2.2 and 2.3). Basics: trigonometric identities

2Complementary angles

cos⁡θ=sin⁡(π2−θ)\cos\theta = \sin\left(\frac{\pi}{2} - \theta\right) for every θ\theta (Class XI).

3Square roots

u2=∣u∣\sqrt{u^2} = |u|⁠, not uu⁠. So cos⁡2θ=cos⁡θ\sqrt{\cos^2\theta} = \cos\theta only when cos⁡θ≥0\cos\theta \ge 0⁠.

4Derivative of sin⁡−1\sin^{-1} and the chain rule

ddxsin⁡−1x=11−x2\frac{d}{dx}\sin^{-1}x = \frac{1}{\sqrt{1-x^2}} for −1<x<1-1 < x < 1 (Example 24, Section 5.3.3). For a composite, multiply the outer derivative by the inner one (Theorem 4). Lesson: derivatives of inverse trig functions

Solution

  1. Check that yy is defined on 0<x<10 < x < 1

    For 0<x<10 < x < 1 we have 0<x2<10 < x^2 < 1⁠, so 0<1−x2<10 < 1 - x^2 < 1 and 0<1−x2<10 < \sqrt{1-x^2} < 1⁠. Both inputs, xx and 1−x2\sqrt{1-x^2}⁠, lie in [−1,1][-1, 1]⁠, so both inverse sines exist.

    sin⁡−1\sin^{-1} only accepts inputs between −1-1 and 1. Before differentiating anything we make sure the function we are differentiating actually exists on the stated interval.
    Domain of sin⁡−1\sin^{-1} is [−1,1][-1, 1] (Chapter 2, Section 2.2; Basic 1).
  2. Substitute x=sin⁡θx = \sin\theta⁠, with θ=sin⁡−1x\theta = \sin^{-1}x

    Let θ=sin⁡−1x\theta = \sin^{-1} x⁠. Since 0<x<10 < x < 1⁠, the angle θ\theta lies in (0,π2)\left(0, \frac{\pi}{2}\right) (the sine is positive and less than 1 there, and sin⁡−1\sin^{-1} takes values in [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right]⁠). Then x=sin⁡θx = \sin\theta and the first term is simply

    sin⁡−1x=θ.\sin^{-1} x = \theta.
    Defining θ\theta as sin⁡−1x\sin^{-1} x (rather than just writing "put x=sin⁡θx = \sin\theta") makes the substitution automatically legitimate: every xx in (0,1)(0,1) gives exactly one such θ\theta⁠, and we know precisely which interval it is in. That interval is what the next step needs.
    sin⁡(sin⁡−1x)=x\sin(\sin^{-1}x) = x for x∈[−1,1]x \in [-1,1] (Chapter 2, Section 2.3). Basics: trigonometric identities
  3. Rewrite 1−x2\sqrt{1-x^2} as sin⁡(π2−θ)\sin\left(\frac{\pi}{2} - \theta\right)

    1−x2=1−sin⁡2θ=cos⁡2θ=∣cos⁡θ∣=cos⁡θ=sin⁡(π2−θ).\begin{aligned} \sqrt{1 - x^2} &= \sqrt{1 - \sin^2\theta} \\ &= \sqrt{\cos^2\theta} = |\cos\theta| \\ &= \cos\theta \\ &= \sin\left(\tfrac{\pi}{2} - \theta\right). \end{aligned}
    The step ∣cos⁡θ∣=cos⁡θ|\cos\theta| = \cos\theta needs cos⁡θ≥0\cos\theta \ge 0⁠. That holds because θ∈(0,π2)\theta \in \left(0, \frac{\pi}{2}\right)⁠, where cosine is positive. The last line is the complementary-angle identity (Basic 2).
    sin⁡2θ+cos⁡2θ=1\sin^2\theta + \cos^2\theta = 1⁠; u2=∣u∣\sqrt{u^2} = |u| (Basic 3). Basics: trigonometric identities
  4. Undo the sine, checking the principal range

    Since 0<θ<π20 < \theta < \frac{\pi}{2}⁠, the angle π2−θ\frac{\pi}{2} - \theta also lies in (0,π2)\left(0, \frac{\pi}{2}\right)⁠, which is inside the principal range [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right]⁠. Therefore

    sin⁡−11−x2=sin⁡−1(sin⁡(π2−θ))=π2−θ.\sin^{-1}\sqrt{1 - x^2} = \sin^{-1}\left(\sin\left(\tfrac{\pi}{2} - \theta\right)\right) = \tfrac{\pi}{2} - \theta.
    sin⁡−1(sin⁡ϕ)=ϕ\sin^{-1}(\sin\phi) = \phi is true only for ϕ\phi in [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right]⁠. We have just checked that ϕ=π2−θ\phi = \frac{\pi}{2} - \theta is there, so the inverse really does undo the sine. (If ϕ\phi were outside that interval, sin⁡−1(sin⁡ϕ)\sin^{-1}(\sin\phi) would be some other angle with the same sine.)
    Principal value branch of sin⁡−1\sin^{-1} (Chapter 2, Section 2.2) and sin⁡−1(sin⁡ϕ)=ϕ\sin^{-1}(\sin\phi) = \phi for ϕ∈[−π2,π2]\phi \in \left[-\frac{\pi}{2}, \frac{\pi}{2}\right] (Chapter 2, Section 2.3). Lesson: derivatives of inverse trig functions
  5. Add: yy is the constant π2\frac{\pi}{2}⁠, so dydx=0\frac{dy}{dx} = 0

    y=θ+(π2−θ)=π2for every x∈(0,1).y = \theta + \left(\tfrac{\pi}{2} - \theta\right) = \frac{\pi}{2} \quad \text{for every } x \in (0,1).

    A constant function has derivative 0, so

    dydx=0,0<x<1.\frac{dy}{dx} = 0, \qquad 0 < x < 1.
    θ π/2 − θ 1 √(1 − x²) = cos θ x = sin θ (here x = 0.6)
    A right triangle with hypotenuse 1 (equal scales, drawn for x=0.6x = 0.6⁠). The side opposite θ\theta is x=sin⁡θx = \sin\theta⁠, the base is 1−x2=cos⁡θ\sqrt{1-x^2} = \cos\theta⁠. The base is also the side opposite the other acute angle π2−θ\frac{\pi}{2} - \theta⁠. So sin⁡−1x\sin^{-1}x and sin⁡−11−x2\sin^{-1}\sqrt{1-x^2} are the two acute angles, and they add up to π2\frac{\pi}{2}⁠.
    The θ\theta's cancel, leaving no xx at all: the value of yy does not change as xx moves through (0,1)(0,1)⁠. The triangle shows why: the two acute angles of a right triangle always add up to a right angle.
    The derivative of a constant function is 0 (Class XI, Limits and Derivatives). Basics: derivative rules
  6. Confirm with the chain rule

    Differentiate the second term with outer function sin⁡−1u\sin^{-1}u and inner function u=1−x2u = \sqrt{1-x^2}⁠:

    dudx=121−x2⋅(−2x)=−x1−x2.\frac{du}{dx} = \frac{1}{2\sqrt{1-x^2}}\cdot(-2x) = \frac{-x}{\sqrt{1-x^2}}.

    The outer derivative is 11−u2\frac{1}{\sqrt{1-u^2}}⁠, and 1−u2=1−(1−x2)=x21 - u^2 = 1 - (1 - x^2) = x^2⁠, so 1−u2=x2=∣x∣=x\sqrt{1-u^2} = \sqrt{x^2} = |x| = x (because x>0x > 0⁠). Hence

    ddxsin⁡−11−x2=1x⋅−x1−x2=−11−x2,\begin{aligned} \frac{d}{dx}\sin^{-1}\sqrt{1-x^2} &= \frac{1}{x}\cdot\frac{-x}{\sqrt{1-x^2}} \\ &= \frac{-1}{\sqrt{1-x^2}}, \end{aligned} dydx=11−x2−11−x2=0. ✓\frac{dy}{dx} = \frac{1}{\sqrt{1-x^2}} - \frac{1}{\sqrt{1-x^2}} = 0. \ ✓
    This is a fully independent route, and it shows exactly where x>0x > 0 is used: x2=x\sqrt{x^2} = x⁠. The derivative formula for sin⁡−1u\sin^{-1}u needs −1<u<1-1 < u < 1⁠, which holds since 0<u<10 < u < 1 (Step 1).
    ddxsin⁡−1x=11−x2\frac{d}{dx}\sin^{-1}x = \frac{1}{\sqrt{1-x^2}} (Example 24); chain rule (Theorem 4, Section 5.3.1); ddxv=12v⋅dvdx\frac{d}{dx}\sqrt{v} = \frac{1}{2\sqrt v}\cdot\frac{dv}{dx}⁠. Lesson: chain rule
  7. Why the interval 0<x<10 < x < 1 matters

    For −1<x<0-1 < x < 0 the same steps break at two places. Then θ∈(−π2,0)\theta \in \left(-\frac{\pi}{2}, 0\right)⁠, so π2−θ\frac{\pi}{2} - \theta lies in (π2,π)\left(\frac{\pi}{2}, \pi\right)⁠, outside the principal range; and in Step 6 x2=−x\sqrt{x^2} = -x⁠. Redoing Step 6 with ∣x∣=−x|x| = -x gives dydx=21−x2\frac{dy}{dx} = \frac{2}{\sqrt{1-x^2}} there, and indeed y=π2+2sin⁡−1xy = \frac{\pi}{2} + 2\sin^{-1}x for −1≤x≤0-1 \le x \le 0⁠.

    So the answer 0 is a property of the stated interval, not of the formula everywhere. For example at x=−0.6x = -0.6⁠, y=sin⁡−1(−0.6)+sin⁡−1(0.8)y = \sin^{-1}(-0.6) + \sin^{-1}(0.8)⁠, which is ≈0.2837941\approx 0.2837941⁠, not π2\frac{\pi}{2}⁠. This is the same lesson as in Chapter 2: check that every angle lies in the principal range before cancelling sin⁡−1\sin^{-1} against sin⁡\sin⁠.
    For π2−θ∈(π2,π)\frac{\pi}{2} - \theta \in \left(\frac{\pi}{2}, \pi\right)⁠: sin⁡−1(sin⁡(π2−θ))=π2+θ\sin^{-1}\left(\sin\left(\frac{\pi}{2} - \theta\right)\right) = \frac{\pi}{2} + \theta⁠, since sin⁡(π−ϕ)=sin⁡ϕ\sin(\pi - \phi) = \sin\phi⁠.
Result

For 0<x<10 < x < 1⁠, y=sin⁡−1x+sin⁡−11−x2=π2y = \sin^{-1}x + \sin^{-1}\sqrt{1-x^2} = \dfrac{\pi}{2} is constant, so

dydx=0.\frac{dy}{dx} = 0.

(Textbook answer: 0.)

Check it with numbers

At x=0.6x = 0.6⁠: 1−0.36=0.8\sqrt{1 - 0.36} = 0.8⁠, and sin⁡−10.6≈0.6435011\sin^{-1}0.6 \approx 0.6435011⁠, sin⁡−10.8≈0.9272952\sin^{-1}0.8 \approx 0.9272952⁠. Their sum is 1.5707963≈π21.5707963 \approx \frac{\pi}{2}⁠. ✓ The same sum appears at every xx in (0,1)(0,1)⁠, so the graph of yy is a horizontal line there, with slope 0.

Term by term at x=0.6x = 0.6⁠: 11−0.36=1.25\frac{1}{\sqrt{1-0.36}} = 1.25 and −11−0.36=−1.25\frac{-1}{\sqrt{1-0.36}} = -1.25⁠; total 0. ✓

Common mistakes
  1. Writing 1−x2=cos⁡θ\sqrt{1 - x^2} = \cos\theta without checking the sign. cos⁡2θ=∣cos⁡θ∣\sqrt{\cos^2\theta} = |\cos\theta|⁠; it equals cos⁡θ\cos\theta here only because θ\theta is acute.
  2. Cancelling sin⁡−1\sin^{-1} and sin⁡\sin blindly. sin⁡−1(sin⁡ϕ)=ϕ\sin^{-1}(\sin\phi) = \phi needs ϕ∈[−π2,π2]\phi \in \left[-\frac{\pi}{2}, \frac{\pi}{2}\right]⁠.
  3. Writing x2=x\sqrt{x^2} = x in the chain-rule route without saying x>0x > 0⁠. For negative xx this gives the wrong derivative (Step 7).
What to take away
  1. sin⁡−1x+sin⁡−11−x2=π2\sin^{-1}x + \sin^{-1}\sqrt{1-x^2} = \frac{\pi}{2} for 0≤x≤10 \le x \le 1⁠: the two acute angles of a right triangle with hypotenuse 1.
  2. When an expression simplifies to a constant, its derivative is 0; simplifying first is often far quicker than differentiating.
  3. Every substitution in an inverse-trig problem comes with two checks: is the substitution allowed on the interval, and is the final angle in the principal range?

Every fact used, and where it comes from

FactUsed inSource
Domain [−1,1][-1,1] and principal range [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right] of sin⁡−1\sin^{-1}Steps 1, 2, 4Chapter 2, Section 2.2
sin⁡(sin⁡−1x)=x\sin(\sin^{-1}x) = x⁠; sin⁡−1(sin⁡ϕ)=ϕ\sin^{-1}(\sin\phi) = \phi on the principal rangeSteps 2, 4Chapter 2, Section 2.3
sin⁡2θ+cos⁡2θ=1\sin^2\theta + \cos^2\theta = 1⁠, cos⁡θ=sin⁡(π2−θ)\cos\theta = \sin\left(\frac{\pi}{2} - \theta\right)⁠, u2=∣u∣\sqrt{u^2} = |u|Step 3Class XI, Trigonometric Functions
Derivative of a constant is 0Step 5Class XI, Limits and Derivatives
ddxsin⁡−1x=11−x2\frac{d}{dx}\sin^{-1}x = \frac{1}{\sqrt{1-x^2}}⁠, −1<x<1-1 < x < 1Steps 6, 7Example 24, Section 5.3.3 (Lesson: derivatives of inverse trig functions)
Chain ruleStep 6Theorem 4, Section 5.3.1 (Lesson: chain rule)
AnswerResultAnswers, Miscellaneous Exercise on Chapter 5, Q13
Numerical values, figure coordinatesCheck, figureRecomputed in the site's verification script
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