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Exercise 9.3 · Q2

Q.Solve the following differential equation: dydx=4−y2\frac{dy}{dx} = \sqrt{4 - y^2} (−2<y<2-2 < y < 2)

Mizoram MbseTextbookSubjective· 3mImportance★★★★★
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This is a first-order separable ODE. We separate variables, integrate using the standard form ∫dya2−y2=sin⁡−1ya+C\int \frac{dy}{\sqrt{a^2 - y^2}} = \sin^{-1}\frac{y}{a} + C, and obtain the general solution y=2sin⁡(x+C)y = 2\sin(x + C).

The key idea here is Separation of Variables. When a differential equation can be written in the form dydx=f(x)g(y)\frac{dy}{dx} = f(x)g(y), we can rearrange it so that all yy terms (including dydy) are on one side and all xx terms (including dxdx) are on the other. Then we integrate both sides. This works because we are essentially treating dydy and dxdx as differentials that can be moved algebraically — a standard technique in first-order ODEs.

Our equation is dydx=4−y2\frac{dy}{dx} = \sqrt{4 - y^2}. Notice the right-hand side depends only on yy, not on xx. That makes it a special case of separable: f(x)=1f(x) = 1 and g(y)=4−y2g(y) = \sqrt{4 - y^2}.

Watch out

A common mistake is to forget the domain restriction −2<y<2-2 < y < 2. The square root 4−y2\sqrt{4 - y^2} is real only when ∣y∣≤2|y| \leq 2, and the derivative is undefined at y=±2y = \pm 2 (the denominator in the separated form would be zero). So we work strictly inside the open interval.

Let’s solve it step by step.

  1. Separate the variables. Multiply both sides by dxdx and divide by 4−y2\sqrt{4 - y^2}:

dy4−y2=dx\frac{dy}{\sqrt{4 - y^2}} = dx

The left side is now purely in yy, the right side purely in xx.

  1. Integrate both sides.

∫dy4−y2=∫dx\int \frac{dy}{\sqrt{4 - y^2}} = \int dx

The right-hand integral is straightforward: ∫dx=x+C\int dx = x + C, where CC is an arbitrary constant.

  1. Evaluate the left-hand integral. This is a standard form. Recall:

∫dya2−y2=sin⁡−1ya+C\int \frac{dy}{\sqrt{a^2 - y^2}} = \sin^{-1}\frac{y}{a} + C

Here a=2a = 2 (since 4=224 = 2^2). So:

∫dy4−y2=sin⁡−1y2+C1\int \frac{dy}{\sqrt{4 - y^2}} = \sin^{-1}\frac{y}{2} + C_1

We can absorb C1C_1 into the constant from the other side.

∫dya2−y2=sin⁡−1ya+C\int \frac{dy}{\sqrt{a^2 - y^2}} = \sin^{-1}\frac{y}{a} + C

  1. Combine the results. Equating the two integrals (and merging constants):

sin⁡−1y2=x+C\sin^{-1}\frac{y}{2} = x + C

where CC is an arbitrary constant.

  1. Solve for yy explicitly. Take the sine of both sides:

y2=sin⁡(x+C)\frac{y}{2} = \sin(x + C)

Multiply by 2:

y=2sin⁡(x+C)y = 2\sin(x + C)

This is the general solution. The constant CC is determined by an initial condition if one is given. The domain restriction −2<y<2-2 < y < 2 is automatically satisfied for all real xx because ∣sin⁡(x+C)∣≤1|\sin(x+C)| \leq 1, so ∣y∣≤2|y| \leq 2, and equality only at isolated points (where the derivative would be zero, but the original ODE still holds in the limit).

Tip

You could also write the solution as y=2sin⁡(x+C)y = 2\sin(x + C) or, equivalently, y=2sin⁡(x+C)y = 2\sin(x + C) with CC any real number. If an initial condition like y(0)=0y(0) = 0 were given, you’d find C=0C = 0, giving y=2sin⁡xy = 2\sin x.

✓Final answer

The general solution is y=2sin⁡(x+C)y = 2\sin(x + C), where CC is an arbitrary constant.

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