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Miscellaneous Exercise · Q13

Q.The general solution of the differential equation y dx−x dyy=0\frac{y\, dx - x\, dy}{y} = 0 is (A) xy=Cxy = C (B) x=Cy2x = Cy^2 (C) y=Cxy = Cx (D) y=Cx2y = Cx^2

Yanam CbseNCERTSubjective· 1mImportance★★★★★
Appeared in past exams:GUJCET 2024· Set 13· 1mreworded
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The equation y dx−x dyy=0\frac{y\, dx - x\, dy}{y} = 0 simplifies to dx−xydy=0dx - \frac{x}{y}dy = 0, which is a first-order linear ODE in x(y)x(y). Using the integrating factor 1y\frac{1}{y}, we get xy=C\frac{x}{y} = C, so the general solution is x=Cyx = Cy, i.e., y=Cxy = Cx — option (C).

The key here is to see what the equation is really saying. You have y dx−x dyy=0\frac{y\, dx - x\, dy}{y} = 0. Before diving into any method, simplify: dividing term-by-term gives dx−xy dy=0dx - \frac{x}{y}\, dy = 0. That’s a differential equation where xx is a function of yy (or vice versa). It’s not in the standard dy/dxdy/dx form, but that’s fine — we can treat yy as the independent variable.

  1. Rewrite in standard linear form From dx−xy dy=0dx - \frac{x}{y}\, dy = 0, bring the dydy term to the other side:

dxdy−xy=0\frac{dx}{dy} - \frac{x}{y} = 0

This is a first-order linear ODE in x(y)x(y): dxdy+P(y)x=Q(y)\frac{dx}{dy} + P(y)x = Q(y) with P(y)=−1yP(y) = -\frac{1}{y} and Q(y)=0Q(y) = 0.

  1. Why the Integrating Factor works The idea: if we multiply the whole equation by some function μ(y)\mu(y), the left side becomes the derivative of μ(y)⋅x\mu(y) \cdot x with respect to yy. That turns the problem into a simple integration. The formula for the integrating factor is μ(y)=e∫P(y) dy\mu(y) = e^{\int P(y)\, dy}. Here P(y)=−1/yP(y) = -1/y, so

∫P(y) dy=∫−1y dy=−log⁡∣y∣=log⁡∣y∣−1\int P(y)\, dy = \int -\frac{1}{y}\, dy = -\log|y| = \log|y|^{-1}

Hence

μ(y)=elog⁡∣y∣−1=1∣y∣\mu(y) = e^{\log|y|^{-1}} = \frac{1}{|y|}

Since we usually work with a positive integrating factor, we take μ(y)=1y\mu(y) = \frac{1}{y} (assuming y≠0y \neq 0; the constant sign can be absorbed later).

  1. Multiply and simplify Multiply the ODE dxdy−xy=0\frac{dx}{dy} - \frac{x}{y} = 0 by 1y\frac{1}{y}:

1ydxdy−xy2=0\frac{1}{y}\frac{dx}{dy} - \frac{x}{y^2} = 0

Notice that the left side is exactly ddy(xy)\frac{d}{dy}\left(\frac{x}{y}\right) — check by differentiating:

ddy(xy)=1ydxdy−xy2\frac{d}{dy}\left(\frac{x}{y}\right) = \frac{1}{y}\frac{dx}{dy} - \frac{x}{y^2}

So the equation becomes

ddy(xy)=0\frac{d}{dy}\left(\frac{x}{y}\right) = 0

  1. Integrate Integrating both sides with respect to yy:

xy=C\frac{x}{y} = C

where CC is an arbitrary constant. Multiply through by yy:

x=Cyx = C y …

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