← 2023 Paper 1

UPSC 2023 Maths Optional Paper 1 Q7a-ii — Step-by-Step Solution

10 marks · Section B

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

Question

Reduce the equation x2p2+y(2x+y)p+y2=0x^2 p^2+y(2x+y)p+y^2=0 to Clairaut’s form by the substitution y=uy=u and xy=vxy=v. Hence solve the equation and show that y+4x=0y+4x=0 is a singular solution of the differential equation.

Technique

Substitution y=u, xy=vy=u,\,xy=v converts the original equation to Clairaut’s form. The general solution is the one-parameter family with P=cP=c; singular solution from differentiating the Clairaut form w.r.t. PP to get the envelope.

Solution

Here p=dy/dxp=dy/dx.

Step 1 — Substitute u=y, v=xyu=y,\,v=xy

Compute du/dvdu/dv. With u,vu,v as functions of xx: dudx=p,dvdx=y+xdydx=u+vup.\dfrac{du}{dx}=p,\quad\dfrac{dv}{dx}=y+x\dfrac{dy}{dx}=u+\dfrac{v}{u}p. (Using x=v/ux=v/u.)

So dudv=pu+(v/u)p=upu2+vp\dfrac{du}{dv}=\dfrac{p}{u+(v/u)p}=\dfrac{up}{u^2+vp}.

Let P=du/dvP=du/dv. Then up=Pu2+Pvp⇒p(u−Pv)=Pu2⇒p=Pu2u−Pv.up=Pu^2+Pvp\Rightarrow p(u-Pv)=Pu^2\Rightarrow p=\dfrac{Pu^2}{u-Pv}.

Step 2 — Substitute into the original equation

Original: x2p2+y(2x+y)p+y2=0x^2p^2+y(2x+y)p+y^2=0. With x=v/u, y=ux=v/u,\,y=u:

(vu)2[Pu2u−Pv]2+u(2vu+u)⋅Pu2u−Pv+u2=0.\Bigl(\frac{v}{u}\Bigr)^2\Bigl[\frac{Pu^2}{u-Pv}\Bigr]^2+u\Bigl(\frac{2v}{u}+u\Bigr)\cdot\frac{Pu^2}{u-Pv}+u^2=0.

Multiply by (u−Pv)2/u2(u-Pv)^2/u^2:

v2P2u2u2⋅(u−Pv)2(u−Pv)2⋅…\frac{v^2 P^2 u^2}{u^2}\cdot\frac{(u-Pv)^2}{(u-Pv)^2}\cdot\ldots

Let me simplify more carefully. The first term: v2u2⋅P2u4(u−Pv)2=v2P2u2(u−Pv)2.\dfrac{v^2}{u^2}\cdot\dfrac{P^2 u^4}{(u-Pv)^2}=\dfrac{v^2 P^2 u^2}{(u-Pv)^2}.

Second term: u(2v/u+u)⋅Pu2u−Pv=(2v+u2)⋅Pu2u−Pvu(2v/u+u)\cdot\dfrac{Pu^2}{u-Pv}=(2v+u^2)\cdot\dfrac{Pu^2}{u-Pv}.

Third term: u2u^2.

Multiply all three terms by (u−Pv)2/u2(u-Pv)^2/u^2:

First → v2P2v^2 P^2. Second → (2v+u2)P(u−Pv)(2v+u^2)P(u-Pv). Third → (u−Pv)2(u-Pv)^2.

Sum:

v2P2+(2v+u2)P(u−Pv)+(u−Pv)2=0.v^2 P^2+(2v+u^2)P(u-Pv)+(u-Pv)^2=0.

Expand: (2v+u2)P(u−Pv)=2vPu−2v2P2+u3P−u2P2v.(2v+u^2)P(u-Pv)=2vPu-2v^2P^2+u^3P-u^2P^2v. (u−Pv)2=u2−2uPv+P2v2.(u-Pv)^2=u^2-2uPv+P^2v^2.

Sum: v2P2+2vPu−2v2P2+u3P−u2P2v+u2−2uPv+P2v2v^2P^2+2vPu-2v^2P^2+u^3P-u^2P^2v+u^2-2uPv+P^2v^2 Combine P2P^2-terms: v2−2v2+v2=0v^2-2v^2+v^2=0 (cancel) but −u2P2v-u^2P^2v remains. Combine PP-terms: 2vPu+u3P−2uPv=u3P2vPu+u^3P-2uPv=u^3P (the 2vPu2vPu and −2uPv-2uPv cancel). Constant term: u2u^2.

So the equation reduces to:

−u2vP2+u3P+u2=0.-u^2 v P^2+u^3 P+u^2=0.

Divide by u2u^2:

−vP2+uP+1=0⇒vP2−uP−1=0.-vP^2+uP+1=0\Rightarrow vP^2-uP-1=0.

Solve for uu:

  u=vP−1P.  \boxed{\;u=vP-\frac{1}{P}.\;}

This is Clairaut’s form u=vP+f(P)u=vP+f(P) with f(P)=−1/Pf(P)=-1/P.

Step 3 — General solution

Clairaut’s general solution: P=cP=c (constant), so u=vc−1/cu=vc-1/c, i.e., y=cv−1/c=c(xy)−1/cy=cv-1/c=c(xy)-1/c.

Rearrange: y(1−cx)=−1/c⇒y=1c(cx−1)y(1-cx)=-1/c\Rightarrow y=\dfrac{1}{c(cx-1)}, equivalently

c2xy−cy−1=0.c^2 xy-cy-1=0.

(Family of curves parameterised by cc.)

Step 4 — Singular solution

Differentiate u=vP−1/Pu=vP-1/P w.r.t. PP (treating u,vu,v as functions of PP in the singular envelope):

0=v+1P2⇒v=−1P2.0=v+\frac{1}{P^2}\Rightarrow v=-\frac{1}{P^2}.

Combined with u=vP−1/P=−1/P−1/P=−2/Pu=vP-1/P=-1/P-1/P=-2/P, eliminate PP: P=−2/uP=-2/u, so v=−1/P2=−u2/4v=-1/P^2=-u^2/4.

In original variables: xy=v=−u2/4=−y2/4⇒4xy+y2=0⇒y(4x+y)=0xy=v=-u^2/4=-y^2/4\Rightarrow 4xy+y^2=0\Rightarrow y(4x+y)=0.

The trivial solution y=0y=0 is included; the non-trivial singular solution is y+4x=0y+4x=0, i.e., y=−4xy=-4x.

Answer

  Singular solution: y+4x=0.  \boxed{\;\text{Singular solution: }y+4x=0.\;}
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