dθdx=−asinθ,dθdy=bcosθ,dxdy=−asinθbcosθ=−abcotθ.
Differentiate again:
dθd(dxdy)=abcsc2θ,dx2d2y=−asinθabcsc2θ=−a2bcsc3θ=−a2sin3θb.
Now compute y⋅y′′: with y=bsinθ,
yy′′=bsinθ⋅(−a2sin3θb)=−a2sin2θb2=−a2b2csc2θ.
And (y′)2=a2b2cot2θ. Adding:
yy′′+(y′)2=a2b2(cot2θ−csc2θ)=a2b2(−1)=−a2b2.
(using csc2θ−cot2θ=1). So
ydx2d2y+(dxdy)2+a2b2=0.
Multiplying through by a2 gives the equivalent, fully-cleared form …