Obtain the singular solution of the differential equation
(dxdy)2(xy)2cot2α−2(dxdy)(xy)+(xy)2csc2α=1.
Also find the complete primitive of the given differential equation. Give the geometrical interpretations of the complete primitive and singular solution.
Technique
Treat as quadratic in p; singular solution =p-discriminant B2−4AC=0. For the complete primitive, the substitution X=x2,Y=y2 linearises it to Y=Xϕ(P) (Lagrange form), which integrates to X(P+1)2=c2; eliminate P to get the circle family.
Solution
Write p=dxdy and v=xy. The equation is a quadratic in p:
Av2cot2αp2B−2vp+C(v2csc2α−1)=0.
Step 1 — Singular solution from the p-discriminant
The singular solution (envelope) satisfies B2−4AC=0:
4v2−4v2cot2α(v2csc2α−1)=0.
Divide by 4v2 (the case v=0 gives y=0, a trivial line):
1−cot2α(v2csc2α−1)=0⟹1+cot2α=v2cot2αcsc2α.
Since 1+cot2α=csc2α, this reduces to csc2α=v2cot2αcsc2α, i.e. v2cot2α=1, so v=±tanα. Restoring v=y/x:
y=±xtanα(singular solution).
Step 2 — Reduce to a solvable form (substitution X=x2,Y=y2)
Multiply the equation by x2 and use py=21(y2)′ in the new variables. Put X=x2,Y=y2 and P=dXdY=2xdx2ydy=xyp=vp, so vp=P and v2p2=P2, while v2=Y/X. The x2× equation
p2y2cot2α−2pxy+y2csc2α=x2
becomes (divide by x2 and substitute):
P2cot2α−2P+XYcsc2α−1=0.
Solve for Y:
Y=Xsin2α(1+2P−P2cot2α)≡Xϕ(P).
Step 3 — Lagrange-type integration
This has the form Y=Xϕ(P) with P=dY/dX. Differentiate w.r.t. X:
P=ϕ(P)+Xϕ′(P)dXdP⟹(P−ϕ(P))=Xϕ′(P)dXdP.
Now
P−ϕ(P)=cos2α(P+1)(P−tan2α),ϕ′(P)=2sin2α−2Pcos2α.
Separate:
XdX=P−ϕ(P)ϕ′(P)dP.
The integral of the right side is (sympy below):
∫cos2α(P+1)(P−tan2α)2sin2α−2Pcos2αdP=−2ln(P+1).
Hence lnX=−2ln(P+1)+const, i.e.
X(P+1)2=c2(constant c2).
Step 4 — Eliminate the parameter P
From X(P+1)2=c2 and X=x2: (P+1)=c/x, so P=xc−1. Substitute into Y=Xϕ(P) (algebra carried out symbolically):