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Chapter 7 · Integrals

Exercise 7.8 · Q9: ∫01dx1−x2\int_0^1\frac{dx}{\sqrt{1 - x^2}}

Exercise 7.8Fundamental theorem of calculus · Section 7.8
The question

Evaluate the definite integral

∫01dx1−x2.\int_0^1\frac{dx}{\sqrt{1 - x^2}}.
Exam answer

Let I=∫01dx1−x2I = \displaystyle\int_0^1\frac{dx}{\sqrt{1 - x^2}}⁠.

Using ∫dx1−x2=sin⁡−1x+C,\displaystyle\int\frac{dx}{\sqrt{1 - x^2}} = \sin^{-1}x + C,

I=[sin⁡−1x]01=sin⁡−11−sin⁡−10=π2−0\begin{aligned} I &= \Big[\sin^{-1}x\Big]_0^1 \\ &= \sin^{-1}1 - \sin^{-1}0 \\ &= \frac{\pi}{2} - 0 \end{aligned}

∴ I=π2\therefore\ I = \dfrac{\pi}{2}⁠.

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

The one idea this problem is built on

The antiderivative of 11−x2\frac{1}{\sqrt{1 - x^2}} is sin⁡−1x\sin^{-1}x (standard formula (viii), Section 7.2), so the expected answer is sin⁡−11−sin⁡−10=π2\sin^{-1}1 - \sin^{-1}0 = \frac{\pi}{2}⁠. There is one point to settle first, which the exercise does not raise: at x=1x = 1 the denominator is 0, so the integrand is not defined there, and Theorem 2 needs ff continuous on the whole closed interval. The standard way round it is to integrate up to b<1b < 1⁠, where everything is fine, and then let bb tend to 1. The answer is still π2\frac{\pi}{2}⁠.

Given, to find, and the plan
Given
f(x)=11−x2f(x) = \frac{1}{\sqrt{1 - x^2}}⁠, defined for −1<x<1-1 < x < 1⁠; the interval is [0,1][0, 1]⁠.
To find
The value of ∫01f(x) dx\int_0^1 f(x)\,dx⁠.
Plan
(1) Find where ff is defined and continuous: on [0,1)[0, 1)⁠, not at 1. (2) Antiderivative sin⁡−1x\sin^{-1}x⁠, checked by differentiating. (3) Theorem 2 on [0,b][0, b] for b<1b < 1⁠. (4) Let b→1−b \to 1^-⁠. (5) Confirm by x=sin⁡θx = \sin\theta and numerically.

Basics you need

1Second fundamental theorem

∫abf(x) dx=F(b)−F(a)\int_a^b f(x)\,dx = F(b) - F(a) when ff is continuous on the closed interval [a,b][a, b] and F′=fF' = f (Theorem 2, Section 7.8.3; Remark (iv) insists on continuity on all of [a,b][a, b]⁠). Lesson: definite integrals and the fundamental theorem

2The sin⁡−1\sin^{-1} formula

ddxsin⁡−1x=11−x2\frac{d}{dx}\sin^{-1}x = \frac{1}{\sqrt{1 - x^2}} for −1<x<1-1 < x < 1⁠, so ∫dx1−x2=sin⁡−1x+C\int\frac{dx}{\sqrt{1 - x^2}} = \sin^{-1}x + C (standard formula (viii), Section 7.2). Lesson: integrals of particular functions

3Principal values

sin⁡−1x\sin^{-1}x takes values in [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right] with sin⁡−10=0\sin^{-1}0 = 0⁠, sin⁡−11=π2\sin^{-1}1 = \frac{\pi}{2} (Chapter 2). It is continuous on [−1,1][-1, 1] (stated without proof in Chapter 5, Section 5.3.3). Basics: trigonometric values

4Area meaning

For f≥0f \ge 0⁠, ∫abf\int_a^b f is the area under the graph (Section 7.8.1). Basics: area as a sum of thin strips

Solution

  1. Where is the integrand defined and continuous?

    1−x2\sqrt{1 - x^2} is real when 1−x2≥01 - x^2 \ge 0⁠, and the fraction needs 1−x2≠0\sqrt{1 - x^2} \ne 0⁠. Together: 1−x2>01 - x^2 > 0⁠, that is −1<x<1-1 < x < 1⁠. So on our interval:

    • for 0≤x<10 \le x < 1⁠, f(x)f(x) is defined and continuous (a quotient of continuous functions with non-zero denominator);
    • at x=1x = 1⁠, the denominator is 0=0\sqrt{0} = 0⁠: f(1)f(1) is not defined, and f(x)→∞f(x) \to \infty as x→1−x \to 1^-⁠.
    Remark (iv) after Theorem 2 says the integrand must be well defined and continuous on the whole of [a,b][a, b]⁠. That fails at the single point x=1x = 1⁠, so we cannot quote Theorem 2 on [0,1][0, 1] directly. We can quote it on [0,b][0, b] for any bb with 0<b<10 < b < 1⁠, because there ff is continuous.
    Quotient of continuous functions: Chapter 5, Theorem 1, Section 5.2.1. Lesson: the fundamental theorem
  2. Antiderivative, and check it

    By standard formula (viii),

    ∫dx1−x2=sin⁡−1x+C,F(x)=sin⁡−1x.\int\frac{dx}{\sqrt{1 - x^2}} = \sin^{-1}x + C, \qquad F(x) = \sin^{-1}x.

    Check: for −1<x<1-1 < x < 1⁠, F′(x)=ddxsin⁡−1x=11−x2=f(x)F'(x) = \frac{d}{dx}\sin^{-1}x = \frac{1}{\sqrt{1 - x^2}} = f(x)⁠.

    This is the derivative of sin⁡−1x\sin^{-1}x from Chapter 5 read backwards. It holds on the open interval (−1,1)(-1, 1)⁠, which contains [0,b][0, b] for every b<1b < 1⁠.
    Standard formula (viii), Section 7.2; ddxsin⁡−1x\frac{d}{dx}\sin^{-1}x is in Chapter 5, Section 5.3.3. Basics: integration undoes differentiation
  3. Theorem 2 on [0,b][0, b]⁠, with 0<b<10 < b < 1

    ∫0bdx1−x2=sin⁡−1b−sin⁡−10=sin⁡−1b.\int_0^b\frac{dx}{\sqrt{1 - x^2}} = \sin^{-1}b - \sin^{-1}0 = \sin^{-1}b.
    On [0,b][0, b] the integrand is continuous and F′=fF' = f⁠, so all the conditions of Theorem 2 hold. sin⁡−10=0\sin^{-1}0 = 0 because sin⁡0=0\sin 0 = 0 and 0 lies in the principal range [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right]⁠.
    Theorem 2, Section 7.8.3. Lesson: the fundamental theorem
  4. Let bb tend to 1

    sin⁡−1\sin^{-1} is continuous on [−1,1][-1, 1]⁠, so as b→1−b \to 1^-⁠,

    ∫01dx1−x2=lim⁡b→1−sin⁡−1b=sin⁡−11=π2≈1.5707963.\begin{aligned}\int_0^1\frac{dx}{\sqrt{1 - x^2}} &= \lim_{b \to 1^-}\sin^{-1}b = \sin^{-1}1 \\ &= \frac{\pi}{2} \approx 1.5707963.\end{aligned}
    The value of the integral over [0,1][0, 1] is defined as this limit (an "improper integral"; the idea goes beyond this book, but the computation is just a limit). sin⁡−11=π2\sin^{-1}1 = \frac{\pi}{2} because sin⁡π2=1\sin\frac{\pi}{2} = 1 and π2\frac{\pi}{2} is in the principal range. The answer key gives only the value π2\frac{\pi}{2}⁠, which is what the usual one-line evaluation [sin⁡−1x]01\big[\sin^{-1}x\big]_0^1 produces. That shortcut gives the same number as the limit because the antiderivative sin⁡−1x\sin^{-1}x is continuous on the closed interval [0,1][0, 1]⁠, even though the integrand is not.
    Principal value branch of sin⁡−1\sin^{-1}⁠: Chapter 2; its continuity: Chapter 5, Section 5.3.3 (stated without proof). Basics: trigonometric values
  5. Confirm with x=sin⁡θx = \sin\theta

    For 0≤θ<π20 \le \theta < \frac{\pi}{2}⁠, put x=sin⁡θx = \sin\theta⁠: then dx=cos⁡θ dθdx = \cos\theta\,d\theta⁠, and 1−sin⁡2θ=cos⁡θ\sqrt{1 - \sin^2\theta} = \cos\theta because cos⁡θ>0\cos\theta > 0 for these θ\theta⁠. So

    dx1−x2=cos⁡θ dθcos⁡θ=dθ.\frac{dx}{\sqrt{1 - x^2}} = \frac{\cos\theta\,d\theta}{\cos\theta} = d\theta.

    On [0,b][0, b] with b<1b < 1 the new limits are θ=0\theta = 0 and θ=sin⁡−1b\theta = \sin^{-1}b⁠, so the integral is ∫0sin⁡−1bdθ=sin⁡−1b\int_0^{\sin^{-1}b}d\theta = \sin^{-1}b⁠, as in Step 3. As b→1−b \to 1^-⁠, the upper limit sin⁡−1b\sin^{-1}b rises to π2\frac{\pi}{2}⁠, and the value tends to π2\frac{\pi}{2}⁠.

    0.5 1 1 2 4 6 x y y = 1/√(1 − x²) x = 1 (not defined) area π/2 ≈ 1.571
    y=11−x2y = \frac{1}{\sqrt{1 - x^2}} starts at height 1 and shoots up without bound as x→1x \to 1 (the dashed line x=1x = 1⁠, where it is undefined). The shaded region is unbounded, yet its area is finite: π2≈1.571\frac{\pi}{2} \approx 1.571⁠. The picture is cut off at height 6.
    The substitution turns the integrand into the constant 1 in θ\theta⁠, so the integral is simply the length of the θ\theta-interval. It is legitimate because x=sin⁡θx = \sin\theta is increasing on [0,π2]\left[0, \frac{\pi}{2}\right]⁠, so θ=sin⁡−1x\theta = \sin^{-1}x runs exactly once over [0,π2)\left[0, \frac{\pi}{2}\right)⁠, and cos⁡θ\cos\theta is positive there, so cos⁡2θ=cos⁡θ\sqrt{\cos^2\theta} = \cos\theta with no sign change.
    Substitution in definite integrals, Section 7.9; 1−sin⁡2θ=∣cos⁡θ∣\sqrt{1 - \sin^2\theta} = |\cos\theta|⁠. Lesson: integration by substitution
Result ∫01dx1−x2=π2≈1.5707963,\int_0^1\frac{dx}{\sqrt{1 - x^2}} = \frac{\pi}{2} \approx 1.5707963,

understood as lim⁡b→1−∫0b\lim_{b \to 1^-}\int_0^b⁠, since the integrand is undefined at x=1x = 1⁠. (Textbook answer: π2\frac{\pi}{2}⁠, the same.)

Check it with numbers

Numerical integration (thin strips, no antiderivative used) up to b<1b < 1⁠:

bbSum of thin stripssin⁡−1b\sin^{-1}b
0.91.11976951.11976951.11976951.1197695
0.991.42925691.42925691.42925691.4292569
0.99991.55665411.55665411.55665411.5566541

The values creep up towards π2≈1.5707963\frac{\pi}{2} \approx 1.5707963⁠; a numerical integrator designed for end-point singularities gives 1.57079631.5707963 on the whole of [0,1][0, 1]⁠.

Common mistakes
  1. Ignoring the bad end point. f(1)f(1) does not exist. Theorem 2 needs continuity on the closed interval, so the limit step is what makes the answer legitimate.
  2. Writing sin⁡−11=90\sin^{-1}1 = 90⁠. Integrals use radians: sin⁡−11=π2\sin^{-1}1 = \frac{\pi}{2}⁠.
  3. Thinking an unbounded region must have infinite area. Here the graph rises so steeply that the strips near x=1x = 1 are very thin, and the total stays finite.
What to take away
  1. ∫dx1−x2=sin⁡−1x+C\int\frac{dx}{\sqrt{1 - x^2}} = \sin^{-1}x + C on −1<x<1-1 < x < 1⁠.
  2. Always test the end points: if the integrand is undefined there, integrate to a nearby point and take a limit.
  3. If the antiderivative is continuous at the bad end point, the limit is just its value there.

Every fact used, and where it comes from

FactUsed inSource
Theorem 2 and the continuity requirementSteps 1, 3Theorem 2 and Remark (iv), Section 7.8.3 (Lesson)
∫dx1−x2=sin⁡−1x+C\int\frac{dx}{\sqrt{1 - x^2}} = \sin^{-1}x + CStep 2Standard formula (viii), Section 7.2 (Lesson)
ddxsin⁡−1x=11−x2\frac{d}{dx}\sin^{-1}x = \frac{1}{\sqrt{1 - x^2}}Step 2Chapter 5, Section 5.3.3
Principal range of sin⁡−1\sin^{-1}Steps 3, 4Chapter 2 (Basics)
sin⁡−1\sin^{-1} is continuous on [−1,1][-1, 1]Step 4Chapter 5, Section 5.3.3 (stated without proof)
Integral up to a bad end point as a limitStep 4Beyond the book (improper integral)
Substitution x=sin⁡θx = \sin\thetaStep 5Section 7.9 (Lesson)
Definite integral as areaStep 5Section 7.8.1 (Basics)
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