← 2017 Paper 2

UPSC 2017 Maths Optional Paper 2 Q7a — Step-by-Step Solution

15 marks · Section B

Classification and reduction to canonical form · PDEs · asked 9× in 14 yrs · Read the full method →

Question

Reduce the equation

y2∂2z∂x2−2xy∂2z∂x∂y+x2∂2z∂y2=y2x∂z∂x+x2y∂z∂yy^2\frac{\partial^2 z}{\partial x^2}-2xy\frac{\partial^2 z}{\partial x\partial y}+x^2\frac{\partial^2 z}{\partial y^2}=\frac{y^2}{x}\frac{\partial z}{\partial x}+\frac{x^2}{y}\frac{\partial z}{\partial y}

to canonical form and hence solve it.

Technique

Discriminant H2−AB=0H^2-AB=0 ⇒ parabolic; one repeated characteristic x2+y2=x^2+y^2=const taken as ξ\xi, independent η=y2\eta=y^2; transform reduces to Zηη=0Z_{\eta\eta}=0; integrate twice.

Solution

Setup. Compare with Azxx+2Hzxy+Bzyy+⋯=0A z_{xx}+2H z_{xy}+B z_{yy}+\cdots=0:

A=y2,2H=−2xy (H=−xy),B=x2.A=y^2,\qquad 2H=-2xy\ (H=-xy),\qquad B=x^2.

Step 1 — Classify

Discriminant:

H2−AB=(−xy)2−(y2)(x2)=x2y2−x2y2=0.H^2-AB=(-xy)^2-(y^2)(x^2)=x^2y^2-x^2y^2=0.

The equation is parabolic everywhere (away from the axes).

Step 2 — Characteristic curves

The characteristics satisfy A dy2−2H dx dy+B dx2=0A\,dy^2-2H\,dx\,dy+B\,dx^2=0:

y2 dy2+2xy dx dy+x2 dx2=0 ⟹ (y dy+x dx)2=0.y^2\,dy^2+2xy\,dx\,dy+x^2\,dx^2=0\ \Longrightarrow\ (y\,dy+x\,dx)^2=0.

A single (repeated) family:

y dy+x dx=0 ⟹ x2+y2=const.y\,dy+x\,dx=0\ \Longrightarrow\ x^2+y^2=\text{const}.

Step 3 — Choose canonical coordinates

Take the characteristic as one coordinate and any independent function as the second:

ξ=x2+y2,η=y2.\xi=x^2+y^2,\qquad \eta=y^2.

(The choice η=y2\eta=y^2 is convenient; any η\eta functionally independent of ξ\xi works.)

Step 4 — Transform the equation

Writing z=Z(ξ,η)z=Z(\xi,\eta) and substituting the chain-rule derivatives, the second-order part collapses (as it must for a parabolic equation) to a single pure second derivative, and the given first-order right-hand side exactly cancels the first-order terms generated by the transformation. The equation reduces to the canonical form

  ∂2Z∂η2=0.  \boxed{\;\frac{\partial^2 Z}{\partial\eta^2}=0.\;}

Step 5 — Solve the canonical equation

Integrating Zηη=0Z_{\eta\eta}=0 twice in η\eta (treating ξ\xi as a parameter):

Z=η f(ξ)+g(ξ),Z=\eta\,f(\xi)+g(\xi),

where f,gf,g are arbitrary functions. Returning to x,yx,y with η=y2, ξ=x2+y2\eta=y^2,\ \xi=x^2+y^2:

Answer

  z=y2 f(x2+y2)+g(x2+y2),  \boxed{\;z=y^2\,f(x^2+y^2)+g(x^2+y^2),\;}
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