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Exercise 9.4 · Q10

Q.(1+exy)dx+exy(1−xy)dy=0\left(1+e^{\frac{x}{y}}\right) dx + e^{\frac{x}{y}} \left(1-\frac{x}{y}\right) dy = 0

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This is a homogeneous differential equation in xx and yy. Substituting x=vyx = vy and separating variables leads to the general solution x+yex/y=Cx + y e^{x/y} = C. The problem asks for the general solution (no initial condition is given in the text), so the answer is x+yex/y=Cx + y e^{x/y} = C.

The given equation is:

(1+exy)dx+exy(1−xy)dy=0\left(1+e^{\frac{x}{y}}\right) dx + e^{\frac{x}{y}} \left(1-\frac{x}{y}\right) dy = 0

We can rewrite it as:

dxdy=−exy(1−xy)1+exy\frac{dx}{dy} = - \frac{e^{\frac{x}{y}} \left(1-\frac{x}{y}\right)}{1+e^{\frac{x}{y}}}

The right-hand side is a function of xy\frac{x}{y} alone. This is the hallmark of a homogeneous differential equation (in the sense that the function f(x,y)f(x,y) is homogeneous of degree zero). When you see an equation where every term has the same total degree in xx and yy, or where the ratio x/yx/y appears naturally, the substitution x=vyx = vy (or y=uxy = ux) is the standard path.

Why does this work? Because if x=vyx = vy, then dxdy=v+ydvdy\frac{dx}{dy} = v + y\frac{dv}{dy}. The original equation, which is messy in xx and yy, becomes a separable equation in vv and yy. That is the entire point: turn a complicated coupled pair into something you can integrate.

Let’s do it step by step.

  1. Substitute x=vyx = vy.

    Then dxdy=v+ydvdy\frac{dx}{dy} = v + y\frac{dv}{dy}. Also, xy=v\frac{x}{y} = v.

    The equation becomes:

v+ydvdy=−ev(1−v)1+evv + y\frac{dv}{dy} = - \frac{e^{v}(1-v)}{1+e^{v}}

  1. Isolate the derivative term. Bring vv to the right:

ydvdy=−ev(1−v)1+ev−vy\frac{dv}{dy} = - \frac{e^{v}(1-v)}{1+e^{v}} - v

Combine the right-hand side into a single fraction:

ydvdy=−ev(1−v)+v(1+ev)1+evy\frac{dv}{dy} = - \frac{e^{v}(1-v) + v(1+e^{v})}{1+e^{v}}

Simplify the numerator:

ev(1−v)+v(1+ev)=ev−vev+v+vev=ev+ve^{v}(1-v) + v(1+e^{v}) = e^{v} - v e^{v} + v + v e^{v} = e^{v} + v

So we have:

ydvdy=−ev+v1+evy\frac{dv}{dy} = - \frac{e^{v} + v}{1+e^{v}}

  1. Separate variables. Multiply both sides by dydy and divide by the vv-expression:

1+evev+v dv=−dyy\frac{1+e^{v}}{e^{v} + v} \, dv = - \frac{dy}{y}

Tip

Notice that the numerator 1+ev1+e^{v} is exactly the derivative of ev+ve^{v} + v with respect to vv. That is, ddv(ev+v)=ev+1\frac{d}{dv}(e^{v} + v) = e^{v} + 1. This is a perfect setup for a logarithmic integration.

  1. Integrate both sides. …

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