We use parametric differentiation to express dxdy and dx2d2y in terms of t, then substitute into the given differential equation. The key is that dxdy=msintsinmt and dx2d2y=sin3tmcosmtsint−msinmtcost, which simplifies to satisfy the equation identically.
When a curve is given parametrically — here x=cost, y=cosmt — we cannot directly write y as a function of x in a simple closed form. But we can still find derivatives using the chain rule: dxdy=dx/dtdy/dt, provided dx/dt=0. For the second derivative, we differentiate dxdy with respect to t and then divide by dx/dt again. This is the standard parametric second derivative formula.
The problem asks us to prove a differential equation involving y, dy/dx, and d2y/dx2, with coefficients in x. So we will compute these derivatives in terms of t, then replace x and y with their parametric forms, and simplify to zero.
Let's go step by step.
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First derivatives with respect to t
Given x=cost, so dtdx=−sint.
Given y=cosmt, so dtdy=−msinmt.
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First derivative dxdy
Using the parametric formula:
dxdy=dx/dtdy/dt=−sint−msinmt=msintsinmt.
Notice the negatives cancel neatly. This is valid wherever sint=0, i.e., t=nπ.
- Second derivative dx2d2y
We differentiate dxdy with respect to t, then divide by dx/dt:
dx2d2y=dtd(dxdy)/dtdx.
First compute dtd(msintsinmt):
dtd(msintsinmt)=m⋅sin2t(mcosmt)sint−sinmt(cost)
using the quotient rule. So:
dtd(dxdy)=m⋅sin2tmcosmtsint−sinmtcost.
Now divide by dtdx=−sint:
dx2d2y=sin2tm(mcosmtsint−sinmtcost)⋅−sint1=−sin3tm(mcosmtsint−sinmtcost).
- Substitute into the left-hand side of the given equation
We need to verify:
(1−x2)dx2d2y−xdxdy+m2y=0.
Substitute x=cost, y=cosmt, and the derivatives we found.
First, 1−x2=1−cos2t=sin2t.
So the first term becomes:
(1−x2)dx2d2y=sin2t⋅(−sin3tm(mcosmtsint−sinmtcost))=−sintm(mcosmtsint−sinmtcost).
Simplify the numerator:
=−sintm2cosmtsint−msinmtcost=−m2cosmt+msintsinmtcost. …