← 2021 Paper 1

UPSC 2021 Maths Optional Paper 1 Q8a-ii — Step-by-Step Solution

10 marks · Section B

Method of variation of parameters · ODEs · asked 12× in 14 yrs · Read the full method →

Question

Find general solution of x2y′′−2x(1+x)y′+2(1+x)y=0x^2 y''-2x(1+x)y'+2(1+x)y=0. Hence solve x2y′′−2x(1+x)y′+2(1+x)y=x3x^2 y''-2x(1+x)y'+2(1+x)y=x^3 by variation of parameters.

Technique

Spot y1=xy_1=x by inspection; reduction of order gives y2=xe2xy_2=xe^{2x}; standard VoP yields particular solution.

Solution

Step 1 — Find one solution by inspection

Try y=xy=x: y′=1y'=1, y′′=0y''=0. Substitute: x2⋅0−2x(1+x)⋅1+2(1+x)⋅x=−2x(1+x)+2x(1+x)=0x^2\cdot 0-2x(1+x)\cdot 1+2(1+x)\cdot x=-2x(1+x)+2x(1+x)=0 ✓.

So y1=xy_1=x.

Step 2 — Find second solution via reduction of order

Try y2=v(x)⋅xy_2=v(x)\cdot x. Then y2′=v′x+vy_2'=v'x+v, y2′′=v′′x+2v′y_2''=v''x+2v'.

Substitute into x2y′′−2x(1+x)y′+2(1+x)y=0x^2 y''-2x(1+x)y'+2(1+x)y=0: x2(v′′x+2v′)−2x(1+x)(v′x+v)+2(1+x)vx=0x^2(v''x+2v')-2x(1+x)(v'x+v)+2(1+x)vx=0, x3v′′+2x2v′−2x2(1+x)v′−2x(1+x)v+2x(1+x)v=0x^3 v''+2x^2 v'-2x^2(1+x)v'-2x(1+x)v+2x(1+x)v=0, x3v′′+2x2v′−2x2(1+x)v′=0x^3 v''+2x^2 v'-2x^2(1+x)v'=0.

Simplify 2x2v′−2x2(1+x)v′=2x2v′[1−(1+x)]=−2x3v′2x^2 v'-2x^2(1+x)v'=2x^2 v'[1-(1+x)]=-2x^3 v'.

So x3v′′−2x3v′=0x^3 v''-2x^3 v'=0, i.e., v′′=2v′v''=2v'.

Let u=v′u=v': u′=2uu'=2u, so u=Ce2xu=Ce^{2x}. Take C=1C=1: v′=e2xv'=e^{2x}, v=e2x/2v=e^{2x}/2.

So y2=v⋅x=xe2x/2y_2=v\cdot x=xe^{2x}/2. Up to a constant, take y2=xe2xy_2=xe^{2x}.

Step 3 — Verify y2=xe2xy_2=xe^{2x}

y2′=e2x+2xe2x=(1+2x)e2xy_2'=e^{2x}+2xe^{2x}=(1+2x)e^{2x}. y2′′=2e2x+(1+2x)(2)e2x=2e2x+2(1+2x)e2x=(4+4x)e2x=4(1+x)e2xy_2''=2e^{2x}+(1+2x)(2)e^{2x}=2e^{2x}+2(1+2x)e^{2x}=(4+4x)e^{2x}=4(1+x)e^{2x}.

LHS: x2⋅4(1+x)e2x−2x(1+x)(1+2x)e2x+2(1+x)xe2xx^2\cdot 4(1+x)e^{2x}-2x(1+x)(1+2x)e^{2x}+2(1+x)xe^{2x} =e2x(1+x)[4x2−2x(1+2x)+2x]=e^{2x}(1+x)[4x^2-2x(1+2x)+2x] =e2x(1+x)[4x2−2x−4x2+2x]=e^{2x}(1+x)[4x^2-2x-4x^2+2x] =e2x(1+x)⋅0=0=e^{2x}(1+x)\cdot 0=0 ✓.

Step 4 — General homogeneous solution

yh=C1x+C2xe2xy_h=C_1 x+C_2 xe^{2x}.

Step 5 — Variation of parameters for x3x^3 RHS

Standard form: divide by x2x^2: y′′−2(1+x)xy′+2(1+x)x2y=xy''-\dfrac{2(1+x)}{x}y'+\dfrac{2(1+x)}{x^2}y=x.

So g(x)=xg(x)=x in standard form y′′+…=g(x)y''+\ldots=g(x).

VoP: yp=u1y1+u2y2y_p=u_1 y_1+u_2 y_2 with u1′y1+u2′y2=0u_1'y_1+u_2'y_2=0, u1′y1′+u2′y2′=g(x)u_1'y_1'+u_2'y_2'=g(x).

With y1=xy_1=x, y2=xe2xy_2=xe^{2x}, y1′=1y_1'=1, y2′=(1+2x)e2xy_2'=(1+2x)e^{2x}:

System: xu1′+xe2xu2′=0⇒u1′=−e2xu2′xu_1'+xe^{2x}u_2'=0\Rightarrow u_1'=-e^{2x}u_2'.

u1′+(1+2x)e2xu2′=xu_1'+(1+2x)e^{2x}u_2'=x.

Sub: −e2xu2′+(1+2x)e2xu2′=x-e^{2x}u_2'+(1+2x)e^{2x}u_2'=x, e2xu2′(2x)=xe^{2x}u_2'(2x)=x, u2′=12e−2xu_2'=\dfrac{1}{2}e^{-2x}.

u2=∫12e−2x dx=−14e−2xu_2=\int\dfrac{1}{2}e^{-2x}\,dx=-\dfrac{1}{4}e^{-2x}.

u1′=−e2x⋅12e−2x=−1/2u_1'=-e^{2x}\cdot\dfrac{1}{2}e^{-2x}=-1/2.

u1=−x/2u_1=-x/2.

Step 6 — Particular solution

yp=u1y1+u2y2=(−x/2)(x)+(−e−2x/4)(xe2x)=−x2/2−x/4y_p=u_1 y_1+u_2 y_2=(-x/2)(x)+(-e^{-2x}/4)(xe^{2x})=-x^2/2-x/4.

Step 7 — General solution

Answer

  y=C1x+C2xe2x−x22−x4.  \boxed{\;y=C_1 x+C_2 xe^{2x}-\dfrac{x^2}{2}-\dfrac{x}{4}.\;}
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