← 2018 Paper 2

UPSC 2018 Maths Optional Paper 2 Q7a — Step-by-Step Solution

15 marks · Section B

Second-order linear PDEs with constant coefficients (CF, PI) · PDEs · asked 13× in 14 yrs · Read the full method →

Question

Solve the partial differential equation

(2D2−5DD′+2D′2)z=5sin⁡(2x+y)+24(y−x)+e3x+4y(2D^2-5DD'+2D'^2)z=5\sin(2x+y)+24(y-x)+e^{3x+4y}

where D≡∂∂x, D′≡∂∂yD\equiv\dfrac{\partial}{\partial x},\ D'\equiv\dfrac{\partial}{\partial y}.

Technique

Factor (D−2D′)(2D−D′)(D-2D')(2D-D') for the CF; PI term-by-term — resonant trig (F=0F=0 ⇒ multiply by xx), polynomial via operator-series 1/F(D,D′)1/F(D,D'), exponential via D→a, D′→bD\to a,\,D'\to b.

Solution

Setup. A homogeneous linear PDE with constant coefficients. Factor the operator, write the complementary function from the linear factors, then build the particular integral term by term.

Step 1 — Factor the operator and write the CF

2D2−5DD′+2D′2=(D−2D′)(2D−D′).2D^2-5DD'+2D'^2=(D-2D')(2D-D').

For a factor (D−mD′)(D-mD') the complementary part is ϕ(y+mx)\phi(y+mx). Here:

CF: zc=ϕ1(y+2x)+ϕ2(2y+x).\text{CF: } z_c=\phi_1(y+2x)+\phi_2(2y+x).

Step 2 — PI for 5sin⁡(2x+y)5\sin(2x+y) (resonant case)

Put D2→−22=−4D^2\to-2^2=-4, DD′→−(2)(1)=−2DD'\to-(2)(1)=-2, D′2→−12=−1D'^2\to-1^2=-1 in F(D,D′)F(D,D'):

F=2(−4)−5(−2)+2(−1)=−8+10−2=0.F=2(-4)-5(-2)+2(-1)=-8+10-2=0.

F=0F=0 ⇒ resonance. The annihilating factor is (D−2D′)(D-2D') since (D−2D′)sin⁡(2x+y)=2cos⁡−2cos⁡=0(D-2D')\sin(2x+y)=2\cos-2\cos=0. Use the rule for a failure: multiply by xx and differentiate the operator. Take the ansatz z=x(Pcos⁡(2x+y)+Qsin⁡(2x+y))z=x\big(P\cos(2x+y)+Q\sin(2x+y)\big); matching gives P=−53, Q=0P=-\tfrac53,\ Q=0:

zp1=−53 xcos⁡(2x+y).z_{p1}=-\frac{5}{3}\,x\cos(2x+y).

Step 3 — PI for 24(y−x)24(y-x) (polynomial RHS)

zp2=12D2−5DD′+2D′2 24(y−x).z_{p2}=\frac{1}{2D^2-5DD'+2D'^2}\,24(y-x).

Expand 12D2(1−5D′2D+D′2D2)−1=12D2(1+5D′2D+⋯)\dfrac{1}{2D^2}\Big(1-\tfrac{5D'}{2D}+\tfrac{D'^2}{D^2}\Big)^{-1}=\dfrac{1}{2D^2}\Big(1+\tfrac{5D'}{2D}+\cdots\Big) acting on the linear 24(y−x)24(y-x). Keeping only terms that survive on a degree-1 input,

zp2=12D2(24(y−x)+5D′2D 24(y−x)).z_{p2}=\frac{1}{2D^2}\Big(24(y-x)+\frac{5D'}{2D}\,24(y-x)\Big).

Now 1D\dfrac1D means integrate w.r.t. xx. 1D[24(y−x)]=24xy−12x2\dfrac1D[24(y-x)]=24xy-12x^2; D′[ ⋅ ]D'[\,\cdot\,] etc. Carrying the algebra (or solving by an undetermined cubic) gives

zp2=127 xy(x−y)=127x2y−127xy2.z_{p2}=\frac{12}{7}\,xy(x-y)=\frac{12}{7}x^2y-\frac{12}{7}xy^2.

Step 4 — PI for e3x+4ye^{3x+4y}

Put D→3, D′→4D\to3,\ D'\to4:

F(3,4)=2(9)−5(12)+2(16)=18−60+32=−10≠0.F(3,4)=2(9)-5(12)+2(16)=18-60+32=-10\ne0. zp3=e3x+4y−10=−110e3x+4y.z_{p3}=\frac{e^{3x+4y}}{-10}=-\frac{1}{10}e^{3x+4y}.

Step 5 — General solution

Answer

  z=ϕ1(y+2x)+ϕ2(2y+x)−53xcos⁡(2x+y)+127xy(x−y)−110e3x+4y.  \boxed{\;z=\phi_1(y+2x)+\phi_2(2y+x)-\frac{5}{3}x\cos(2x+y)+\frac{12}{7}xy(x-y)-\frac{1}{10}e^{3x+4y}.\;}
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