← 2019 Paper 1

UPSC 2019 Maths Optional Paper 1 Q8a — Step-by-Step Solution

15 marks · Section B

Clairaut's equation · ODEs · asked 5× in 14 yrs · Read the full method →

Question

Obtain the singular solution of the differential equation

(dydx)2(yx)2cot⁡2α−2(dydx)(yx)+(yx)2csc⁡2α=1.\left(\frac{dy}{dx}\right)^2\left(\frac{y}{x}\right)^2\cot^2\alpha-2\left(\frac{dy}{dx}\right)\left(\frac{y}{x}\right)+\left(\frac{y}{x}\right)^2\csc^2\alpha=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 pp; singular solution == pp-discriminant B2−4AC=0B^2-4AC=0. For the complete primitive, the substitution X=x2,Y=y2X=x^2,Y=y^2 linearises it to Y=Xϕ(P)Y=X\phi(P) (Lagrange form), which integrates to X(P+1)2=c2X(P+1)^2=c^2; eliminate PP to get the circle family.

Solution

Write p=dydxp=\dfrac{dy}{dx} and v=yxv=\dfrac yx. The equation is a quadratic in pp:

v2cot⁡2α⏟A p2−2v⏟B p+(v2csc⁡2α−1)⏟C=0.\underbrace{v^2\cot^2\alpha}_{A}\,p^2\underbrace{-2v}_{B}\,p+\underbrace{(v^2\csc^2\alpha-1)}_{C}=0.

Step 1 — Singular solution from the pp-discriminant

The singular solution (envelope) satisfies B2−4AC=0B^2-4AC=0:

4v2−4 v2cot⁡2α (v2csc⁡2α−1)=0.4v^2-4\,v^2\cot^2\alpha\,(v^2\csc^2\alpha-1)=0.

Divide by 4v24v^2 (the case v=0v=0 gives y=0y=0, a trivial line):

1−cot⁡2α (v2csc⁡2α−1)=0 ⟹ 1+cot⁡2α=v2cot⁡2αcsc⁡2α.1-\cot^2\alpha\,(v^2\csc^2\alpha-1)=0\ \Longrightarrow\ 1+\cot^2\alpha=v^2\cot^2\alpha\csc^2\alpha.

Since 1+cot⁡2α=csc⁡2α1+\cot^2\alpha=\csc^2\alpha, this reduces to csc⁡2α=v2cot⁡2αcsc⁡2α\csc^2\alpha=v^2\cot^2\alpha\csc^2\alpha, i.e. v2cot⁡2α=1v^2\cot^2\alpha=1, so v=±tan⁡αv=\pm\tan\alpha. Restoring v=y/xv=y/x:

  y=±xtan⁡α(singular solution).  \boxed{\;y=\pm x\tan\alpha\quad(\text{singular solution}).\;}

Step 2 — Reduce to a solvable form (substitution X=x2, Y=y2X=x^2,\ Y=y^2)

Multiply the equation by x2x^2 and use py=12(y2)′py=\tfrac12(y^2)' in the new variables. Put X=x2, Y=y2X=x^2,\ Y=y^2 and P=dYdX=2y dy2x dx=yx p=vpP=\dfrac{dY}{dX}=\dfrac{2y\,dy}{2x\,dx}=\dfrac yx\,p=vp, so vp=Pvp=P and v2p2=P2v^2p^2=P^2, while v2=Y/Xv^2=Y/X. The x2×x^2\times equation

p2y2cot⁡2α−2pxy+y2csc⁡2α=x2p^2y^2\cot^2\alpha-2pxy+y^2\csc^2\alpha=x^2

becomes (divide by x2x^2 and substitute):

P2cot⁡2α−2P+YXcsc⁡2α−1=0.P^2\cot^2\alpha-2P+\frac YX\csc^2\alpha-1=0.

Solve for YY:

Y=Xsin⁡2α(1+2P−P2cot⁡2α)≡X ϕ(P).Y=X\sin^2\alpha\big(1+2P-P^2\cot^2\alpha\big)\equiv X\,\phi(P).

Step 3 — Lagrange-type integration

This has the form Y=X ϕ(P)Y=X\,\phi(P) with P=dY/dXP=dY/dX. Differentiate w.r.t. XX:

P=ϕ(P)+X ϕ′(P)dPdX ⟹ (P−ϕ(P))=X ϕ′(P)dPdX.P=\phi(P)+X\,\phi'(P)\frac{dP}{dX}\ \Longrightarrow\ \big(P-\phi(P)\big)=X\,\phi'(P)\frac{dP}{dX}.

Now

P−ϕ(P)=cos⁡2α (P+1)(P−tan⁡2α),ϕ′(P)=2sin⁡2α−2Pcos⁡2α.P-\phi(P)=\cos^2\alpha\,(P+1)(P-\tan^2\alpha),\qquad \phi'(P)=2\sin^2\alpha-2P\cos^2\alpha.

Separate:

dXX=ϕ′(P)P−ϕ(P) dP.\frac{dX}{X}=\frac{\phi'(P)}{P-\phi(P)}\,dP.

The integral of the right side is (sympy below):

∫2sin⁡2α−2Pcos⁡2αcos⁡2α(P+1)(P−tan⁡2α) dP=−2ln⁡(P+1).\int\frac{2\sin^2\alpha-2P\cos^2\alpha}{\cos^2\alpha(P+1)(P-\tan^2\alpha)}\,dP=-2\ln(P+1).

Hence ln⁡X=−2ln⁡(P+1)+const\ln X=-2\ln(P+1)+\text{const}, i.e.

X(P+1)2=c2(constant c2).X(P+1)^2=c^2\quad(\text{constant }c^2).

Step 4 — Eliminate the parameter PP

From X(P+1)2=c2X(P+1)^2=c^2 and X=x2X=x^2: (P+1)=c/x(P+1)=c/x, so P=cx−1P=\dfrac cx-1. Substitute into Y=Xϕ(P)Y=X\phi(P) (algebra carried out symbolically):

y2=Y=2cx−x2−c2cos⁡2α.y^2=Y=2cx-x^2-c^2\cos^2\alpha.

Rearrange, writing b=cb=c:

x2−2bx+y2+b2cos⁡2α=0 ⟹ (x−b)2+y2=b2(1−cos⁡2α)=b2sin⁡2α.x^2-2bx+y^2+b^2\cos^2\alpha=0\ \Longrightarrow\ (x-b)^2+y^2=b^2(1-\cos^2\alpha)=b^2\sin^2\alpha.

Answer

  (x−b)2+y2=b2sin⁡2α(complete primitive, parameter b).  \boxed{\;(x-b)^2+y^2=b^2\sin^2\alpha\quad(\text{complete primitive, parameter }b).\;}
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