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Chapter 9 · Differential Equations

Miscellaneous · Q4: General solution of dydx+1−y21−x2=0\frac{dy}{dx} + \sqrt{\frac{1 - y^2}{1 - x^2}} = 0

Miscellaneous ExerciseVariables separable · Section 9.4.1
The question

4. Find the general solution of the differential equation dydx+1−y21−x2=0\dfrac{dy}{dx} + \sqrt{\dfrac{1 - y^2}{1 - x^2}} = 0⁠.

Exam answer

Here −1<x<1-1 < x < 1⁠. For −1<y<1-1 < y < 1⁠, the equation is

dydx=−1−y21−x2\frac{dy}{dx} = -\frac{\sqrt{1 - y^2}}{\sqrt{1 - x^2}}

The variables are separable. Separating them,

dy1−y2=−dx1−x2\frac{dy}{\sqrt{1 - y^2}} = -\frac{dx}{\sqrt{1 - x^2}}

Integrating both sides,

∫dy1−y2=−∫dx1−x2⇒ sin⁡−1y=−sin⁡−1x+C\begin{aligned} &\int\frac{dy}{\sqrt{1 - y^2}} = -\int\frac{dx}{\sqrt{1 - x^2}} \\ &\Rightarrow\ \sin^{-1}y = -\sin^{-1}x + C \end{aligned}

∴\therefore sin⁡−1x+sin⁡−1y=C\sin^{-1}x + \sin^{-1}y = C is the general solution.

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

The one idea this problem is built on

The right side splits into a factor in yy times a factor in xx⁠: 1−y21−x2=1−y2⋅11−x2\sqrt{\frac{1 - y^2}{1 - x^2}} = \sqrt{1 - y^2}\cdot\frac{1}{\sqrt{1 - x^2}}⁠. So the variables separate, and each side is the standard integral ∫du1−u2=sin⁡−1u\int\frac{du}{\sqrt{1 - u^2}} = \sin^{-1}u⁠. One constant on one side gives the general solution.

Given, to find, and the plan
Given
dydx+1−y21−x2=0\frac{dy}{dx} + \sqrt{\frac{1 - y^2}{1 - x^2}} = 0⁠, a first order equation.
To find
Its general solution.
Plan
(1) Find where the equation makes sense and split the root. (2) Separate the variables. (3) Integrate, with one constant. (4) Write the general solution and its domain. (5) Note the constant solutions set aside. (6) Check by differentiating back.

Basics you need

1Variables separable

If dydx=h(y) g(x)\frac{dy}{dx} = h(y)\,g(x) with h(y)≠0h(y) \ne 0⁠, then dyh(y)=g(x) dx\frac{dy}{h(y)} = g(x)\,dx⁠, and integrating both sides gives the general solution (Section 9.4.1, equations (2) to (4)). Lesson: variables separable

2The standard integral ∫du1−u2\int\frac{du}{\sqrt{1 - u^2}}

∫du1−u2=sin⁡−1u+C\int\frac{du}{\sqrt{1 - u^2}} = \sin^{-1}u + C for −1<u<1-1 < u < 1 (Section 7.2, formula (viii)). Basics: every method ends with an integral

3Roots of a quotient

For p≥0p \ge 0 and q>0q > 0⁠, pq=pq\sqrt{\frac{p}{q}} = \frac{\sqrt p}{\sqrt q}⁠. Basics: dy = y′ dx

4One constant for a first order equation

A general solution of a first order equation carries one arbitrary constant (chapter Summary). Basics: order n gives n constants

Solution

  1. Where the equation makes sense; split the root

    The denominator 1−x21 - x^2 must be positive (it is under a root and below a fraction line), so −1<x<1-1 < x < 1⁠. Then the quotient under the root is ≥0\ge 0 only if 1−y2≥01 - y^2 \ge 0⁠, that is −1≤y≤1-1 \le y \le 1⁠. With 1−y2≥01 - y^2 \ge 0 and 1−x2>01 - x^2 > 0⁠,

    dydx=−1−y21−x2=−1−y21−x2.\frac{dy}{dx} = -\sqrt{\frac{1 - y^2}{1 - x^2}} = -\frac{\sqrt{1 - y^2}}{\sqrt{1 - x^2}}.
    The form dydx=h(y) g(x)\frac{dy}{dx} = h(y)\,g(x) needs the root split into a yy-part and an xx-part. That split is valid exactly because the top is not negative and the bottom is positive.
    p/q=p/q\sqrt{p/q} = \sqrt p/\sqrt q for p≥0p \ge 0⁠, q>0q > 0⁠. Basics: dy = y′ dx
  2. Separate the variables

    For −1<y<1-1 < y < 1⁠, 1−y2≠0\sqrt{1 - y^2} \ne 0⁠, and we may divide by it:

    dy1−y2=−dx1−x2.\frac{dy}{\sqrt{1 - y^2}} = -\frac{dx}{\sqrt{1 - x^2}}.
    Now the left side has only yy and the right side only xx⁠. This is the book's form (3) of Section 9.4.1 with h(y)=1−y2h(y) = \sqrt{1 - y^2} and g(x)=−11−x2g(x) = -\frac{1}{\sqrt{1 - x^2}}⁠. The two values y=±1y = \pm 1⁠, where we cannot divide, are looked at in Step 5.
    Section 9.4.1: separating the variables. Lesson: variables separable
  3. Integrate, with one constant

    ∫dy1−y2=−∫dx1−x2sin⁡−1y=−sin⁡−1x+C,\begin{aligned} \int\frac{dy}{\sqrt{1 - y^2}} &= -\int\frac{dx}{\sqrt{1 - x^2}} \\ \sin^{-1}y &= -\sin^{-1}x + C, \end{aligned}

    where CC is an arbitrary constant.

    Both integrals are the same standard form. Each side would bring its own constant, but their difference is one arbitrary number, so one CC on the right is enough.
    Section 7.2, formula (viii); Section 9.4.1, equation (4). Basics: every method ends with an integral
  4. The general solution, and where it lives

    sin⁡−1x+sin⁡−1y=C,\sin^{-1}x + \sin^{-1}y = C,

    for −1<x<1-1 < x < 1 and −1<y<1-1 < y < 1⁠. Since each inverse sine lies in (−π2,π2)\left(-\frac{\pi}{2}, \frac{\pi}{2}\right) here, only constants with −π<C<π-\pi < C < \pi give curves. Solved for yy⁠: y=sin⁡(C−sin⁡−1x)y = \sin(C - \sin^{-1}x)⁠, for the xx with C−sin⁡−1xC - \sin^{-1}x in (−π2,π2)\left(-\frac{\pi}{2}, \frac{\pi}{2}\right)⁠.

    Moving sin⁡−1x\sin^{-1}x to the left gives the symmetric form of the answer key. The range of sin⁡−1\sin^{-1} is [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right] (Chapter 2), which is why CC is limited and why the explicit form holds only on part of (−1,1)(-1, 1)⁠.
    Principal value branch of sin⁡−1\sin^{-1} (Chapter 2, Section 2.2). Lesson: Examples 4 to 9
  5. The constant solutions y=1y = 1 and y=−1y = -1

    In Step 2 we divided by 1−y2\sqrt{1 - y^2}⁠, which is 0 when y=±1y = \pm 1⁠. The constant functions y=1y = 1 and y=−1y = -1 have dydx=0\frac{dy}{dx} = 0 and make the root 01−x2=0\sqrt{\frac{0}{1 - x^2}} = 0⁠, so they also satisfy the equation on −1<x<1-1 < x < 1⁠. No value of CC gives them: y=1y = 1 would need sin⁡−1x=C−π2\sin^{-1}x = C - \frac{\pi}{2} for every xx⁠.

    Dividing by an expression can lose the solutions on which it vanishes, so we test them directly. These two lines lie outside the family; the question asks for the general solution, which is the family of Step 4. The answer key gives the family only.
    Section 9.4.1: separating needs h(y)≠0h(y) \ne 0⁠, so y=±1y = \pm 1 are tested directly; chapter Summary: one arbitrary constant in the general solution. Lesson: general and particular solutions
  6. Check by substituting back

    Differentiate sin⁡−1x+sin⁡−1y=C\sin^{-1}x + \sin^{-1}y = C with respect to xx⁠:

    11−x2+11−y2dydx=0,dydx=−1−y21−x2=−1−y21−x2,\begin{aligned} \frac{1}{\sqrt{1 - x^2}} + \frac{1}{\sqrt{1 - y^2}}\frac{dy}{dx} &= 0, \\ \frac{dy}{dx} = -\frac{\sqrt{1 - y^2}}{\sqrt{1 - x^2}} &= -\sqrt{\frac{1 - y^2}{1 - x^2}}, \end{aligned}

    which is the given equation, for every CC⁠.

    Getting the equation back proves the answer. The minus sign comes out right because both roots are positive; on the curve, 1−y2=cos⁡(sin⁡−1y)≥0\sqrt{1 - y^2} = \cos(\sin^{-1}y) \ge 0 since sin⁡−1y\sin^{-1}y lies in [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right]⁠.
    ddxsin⁡−1x=11−x2\frac{d}{dx}\sin^{-1}x = \frac{1}{\sqrt{1 - x^2}} (Chapter 5, Section 5.3.3). Basics: y′ and y″
Result

The general solution is sin⁡−1x+sin⁡−1y=C\sin^{-1}x + \sin^{-1}y = C⁠, for −1<x<1-1 < x < 1 and −1<y<1-1 < y < 1⁠. (The constant functions y=±1y = \pm 1 also satisfy the equation; no value of CC gives them.) (Textbook answer: sin⁡−1y+sin⁡−1x=C\sin^{-1}y + \sin^{-1}x = C⁠.)

Check it with numbers

Take C=π2C = \frac{\pi}{2}⁠. Then y=sin⁡(π2−sin⁡−1x)y = \sin\left(\frac{\pi}{2} - \sin^{-1}x\right)⁠, which is cos⁡(sin⁡−1x)=1−x2\cos(\sin^{-1}x) = \sqrt{1 - x^2}⁠, for 0≤x<10 \le x < 1⁠. At x=0.6x = 0.6⁠: y=0.8y = 0.8⁠, and sin⁡−10.6≈0.643501\sin^{-1}0.6 \approx 0.643501⁠, sin⁡−10.8≈0.927295\sin^{-1}0.8 \approx 0.927295⁠, whose sum 1.5707961.570796 is π2\frac{\pi}{2}⁠.

The equation gives the slope −1−0.641−0.36=−0.360.64=−0.75-\sqrt{\frac{1 - 0.64}{1 - 0.36}} = -\sqrt{\frac{0.36}{0.64}} = -0.75⁠. The curve itself: y(0.601)≈0.7992490225y(0.601) \approx 0.7992490225 and y(0.599)≈0.8007490244y(0.599) \approx 0.8007490244⁠. Their difference is

0.7992490225−0.8007490244=−0.0015000019,\begin{aligned} &0.7992490225 - 0.8007490244 \\ &= -0.0015000019, \end{aligned}

and −0.0015000019÷0.002≈−0.75000-0.0015000019 \div 0.002 \approx -0.75000⁠, the slope the equation gives.

Common mistakes
  1. Losing the minus sign when separating: the xx-side is −dx1−x2-\frac{dx}{\sqrt{1 - x^2}}⁠, so the answer is a sum sin⁡−1x+sin⁡−1y\sin^{-1}x + \sin^{-1}y⁠, not a difference.
  2. Writing cos⁡−1\cos^{-1} for ∫du1−u2\int\frac{du}{\sqrt{1 - u^2}}⁠. Either is possible, −cos⁡−1u-\cos^{-1}u and sin⁡−1u\sin^{-1}u differ by a constant, but mixing them on one line hides the constant; keep sin⁡−1\sin^{-1} as the book does.
  3. Two constants, one on each side. One arbitrary constant is enough for a first order equation.
  4. Ignoring the domain. The equation lives only on −1<x<1-1 < x < 1 and −1≤y≤1-1 \le y \le 1⁠.
What to take away
  1. A root of a quotient of an xx-part and a yy-part separates once the root is split.
  2. ∫du1−u2=sin⁡−1u\int\frac{du}{\sqrt{1 - u^2}} = \sin^{-1}u⁠: the answer is a relation between inverse sines.
  3. After dividing by a yy-expression, test the values where it is 0; here y=±1y = \pm 1 are extra solutions outside the family.

Every fact used, and where it comes from

FactUsed inSource
p/q=p/q\sqrt{p/q} = \sqrt p/\sqrt q for p≥0p \ge 0⁠, q>0q > 0Step 1Algebra of square roots (Basics)
Separating the variables; integrate both sidesSteps 2, 3Section 9.4.1, equations (2) to (4) (Lesson)
∫du1−u2=sin⁡−1u+C\int\frac{du}{\sqrt{1 - u^2}} = \sin^{-1}u + CStep 3Section 7.2, formula (viii) (Basics)
Range of sin⁡−1\sin^{-1} is [−π2,π2]\left[-\frac{\pi}{2}, \frac{\pi}{2}\right]Steps 4, 6Chapter 2, Section 2.2
One arbitrary constant for a first order equationSteps 3, 5Chapter Summary (Basics)
Separating needs h(y)≠0h(y) \ne 0⁠; the values where h(y)=0h(y) = 0 are tested directlySteps 2, 5Section 9.4.1, equation (3) (Lesson)
ddxsin⁡−1x=11−x2\frac{d}{dx}\sin^{-1}x = \frac{1}{\sqrt{1 - x^2}}Step 6Chapter 5, Section 5.3.3 (Basics)
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