← 2013 Paper 1

UPSC 2013 Maths Optional Paper 1 Q6c — Step-by-Step Solution

15 marks · Section B

Euler-Cauchy equation · ODEs · asked 9× in 14 yrs · Read the full method →

Question

Find the general solution of the equation

x2d2ydx2+xdydx+y=ln⁡x sin⁡(ln⁡x).x^{2}\frac{d^{2}y}{dx^{2}}+x\frac{dy}{dx}+y=\ln x\,\sin(\ln x).

Technique

Cauchy-Euler x=etx=e^{t} substitution; constant-coefficient ODE with resonant RHS; complex-method particular solution (y=eituy=e^{it}u followed by integrating-factor solution of u′′+2iu′=tu''+2iu'=t).

Solution

Strategy. Cauchy-Euler equation: substitute x=etx=e^{t} to convert to a constant-coefficient ODE. The RHS becomes tsin⁡tt\sin t — resonant with the homogeneous solution, requiring a higher-order ansatz.

Step 1 — Substitute x=etx=e^{t}, t=ln⁡xt=\ln x

With D=d/dtD=d/dt:

xdydx=Dy,x2d2ydx2=D(D−1)y.x\frac{dy}{dx}=Dy,\qquad x^{2}\frac{d^{2}y}{dx^{2}}=D(D-1)y.

The ODE becomes

D(D−1)y+Dy+y=tsin⁡t  ⟹  (D2+1)y=tsin⁡t.D(D-1)y+Dy+y=t\sin t\;\Longrightarrow\;(D^{2}+1)y=t\sin t.

Step 2 — Homogeneous (complementary) solution

D2+1=0D^{2}+1=0 gives D=±iD=\pm i, so

yc=C1cos⁡t+C2sin⁡t.y_c=C_1\cos t+C_2\sin t.

Step 3 — Particular solution via complex method

Write tsin⁡t=Im⁡(t eit)t\sin t=\operatorname{Im}(t\,e^{it}). Solve (D2+1)y=t eit(D^{2}+1)y=t\,e^{it}; take the imaginary part for the real solution.

The RHS contains the resonant factor eite^{it}. Substitute y=eituy=e^{it}u. Then

y′′+y=eit(u′′+2iu′)y''+y=e^{it}(u''+2iu')

(computed via y′=eit(u′+iu),  y′′=eit(u′′+2iu′−u)y'=e^{it}(u'+iu),\;y''=e^{it}(u''+2iu'-u), then y′′+y=eit(u′′+2iu′)y''+y=e^{it}(u''+2iu').)

Setting =t eit=t\,e^{it}:

u′′+2iu′=t.u''+2iu'=t.

Let v=u′v=u': v′+2iv=tv'+2iv=t. Integrating factor e2ite^{2it} gives (e2itv)′=te2it(e^{2it}v)'=te^{2it}.

Integrating by parts:

∫t e2it dt=t e2it2i−e2it(2i)2=t e2it2i+e2it4.\int t\,e^{2it}\,dt=\frac{t\,e^{2it}}{2i}-\frac{e^{2it}}{(2i)^{2}}=\frac{t\,e^{2it}}{2i}+\frac{e^{2it}}{4}.

So v=t2i+14+(transient)=−it2+14v=\dfrac{t}{2i}+\dfrac{1}{4}+(\text{transient})=-\dfrac{it}{2}+\dfrac{1}{4} (drop homogeneous part).

Integrate: u=−it24+t4u=-\dfrac{it^{2}}{4}+\dfrac{t}{4}.

Hence

yp(complex)=eit ⁣(t4−it24)=(cos⁡t+isin⁡t) ⁣(t4−it24).y_p^{\text{(complex)}}=e^{it}\!\left(\dfrac{t}{4}-\dfrac{it^{2}}{4}\right)=(\cos t+i\sin t)\!\left(\dfrac{t}{4}-\dfrac{it^{2}}{4}\right).

Multiply out and take imaginary part:

yp(complex)=(t4cos⁡t+t24sin⁡t)+i(t4sin⁡t−t24cos⁡t),y_p^{\text{(complex)}}=\Bigl(\dfrac{t}{4}\cos t+\dfrac{t^{2}}{4}\sin t\Bigr)+i\Bigl(\dfrac{t}{4}\sin t-\dfrac{t^{2}}{4}\cos t\Bigr), yp=Im⁡(⋅)=tsin⁡t−t2cos⁡t4.y_p=\operatorname{Im}(\cdot)=\dfrac{t\sin t-t^{2}\cos t}{4}.

Step 4 — Verify

yp=tsin⁡t4−t2cos⁡t4y_p=\dfrac{t\sin t}{4}-\dfrac{t^{2}\cos t}{4}.

yp′=sin⁡t+tcos⁡t4−2tcos⁡t−t2sin⁡t4=sin⁡t−tcos⁡t+t2sin⁡t4y_p'=\dfrac{\sin t+t\cos t}{4}-\dfrac{2t\cos t-t^{2}\sin t}{4}=\dfrac{\sin t-t\cos t+t^{2}\sin t}{4}.

yp′′=cos⁡t−(cos⁡t−tsin⁡t)+2tsin⁡t+t2cos⁡t4=3tsin⁡t+t2cos⁡t4y_p''=\dfrac{\cos t-(\cos t-t\sin t)+2t\sin t+t^{2}\cos t}{4}=\dfrac{3t\sin t+t^{2}\cos t}{4}.

yp′′+yp=3tsin⁡t+t2cos⁡t4+tsin⁡t−t2cos⁡t4=4tsin⁡t4=tsin⁡ty_p''+y_p=\dfrac{3t\sin t+t^{2}\cos t}{4}+\dfrac{t\sin t-t^{2}\cos t}{4}=\dfrac{4t\sin t}{4}=t\sin t ✓.

Step 5 — Back-substitute and write general solution

Replace t=ln⁡xt=\ln x:

Answer

  y=C1cos⁡(ln⁡x)+C2sin⁡(ln⁡x)+ln⁡x sin⁡(ln⁡x)−(ln⁡x)2cos⁡(ln⁡x)4.  \boxed{\;y=C_1\cos(\ln x)+C_2\sin(\ln x)+\dfrac{\ln x\,\sin(\ln x)-(\ln x)^{2}\cos(\ln x)}{4}.\;}
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