← 2014 Paper 2

UPSC 2014 Maths Optional Paper 2 Q3b — Step-by-Step Solution

15 marks · Section A

Partial derivatives; equality of mixed partials (Schwarz) · Real Analysis · asked 2× in 14 yrs · Read the full method →

Question

Obtain ∂2f(0,0)∂x ∂y\dfrac{\partial^{2}f(0,0)}{\partial x\,\partial y} and ∂2f(0,0)∂y ∂x\dfrac{\partial^{2}f(0,0)}{\partial y\,\partial x} for the function

f(x,y)={xy(3x2−2y2)x2+y2,(x,y)≠(0,0)0,(x,y)=(0,0).f(x,y)=\begin{cases}\dfrac{xy(3x^{2}-2y^{2})}{x^{2}+y^{2}},&(x,y)\ne(0,0)\\ 0,&(x,y)=(0,0)\end{cases}.

Also, discuss the continuity of ∂2f∂x ∂y\dfrac{\partial^{2}f}{\partial x\,\partial y} and ∂2f∂y ∂x\dfrac{\partial^{2}f}{\partial y\,\partial x} at (0,0)(0,0).

Technique

Same as 2013 P1 Q3(b): compute partial derivatives off-origin by smooth formulas; use limit definition at origin; check Clairaut’s hypothesis (continuity of 2nd partials).

Solution

Strategy. Use the limit definition to compute partial derivatives at (0,0)(0,0); the mixed partials fxy(0,0)f_{xy}(0,0) and fyx(0,0)f_{yx}(0,0) can differ when fxyf_{xy} and fyxf_{yx} are discontinuous at the origin (Clairaut’s theorem fails).

Step 1 — First partials at (0,0)(0,0)

f(h,0)=0f(h,0)=0 for any hh (since ff has factor xyxy in numerator). So

fx(0,0)=lim⁡h→0f(h,0)−0h=0.f_x(0,0)=\lim_{h\to 0}\frac{f(h,0)-0}{h}=0.

Similarly fy(0,0)=0f_y(0,0)=0.

Step 2 — fx(0,y)f_x(0,y) for y≠0y\ne 0

For (x,y)≠(0,0)(x,y)\ne(0,0), the formula for ff is smooth. Differentiate w.r.t. xx:

fx=∂∂x ⁣[xy(3x2−2y2)x2+y2]=y(9x2−2y2)x2+y2−2x2y(3x2−2y2)(x2+y2)2.f_x=\frac{\partial}{\partial x}\!\left[\frac{xy(3x^{2}-2y^{2})}{x^{2}+y^{2}}\right]=\frac{y(9x^{2}-2y^{2})}{x^{2}+y^{2}}-\frac{2x^{2}y(3x^{2}-2y^{2})}{(x^{2}+y^{2})^{2}}.

At x=0x=0, y≠0y\ne 0:

fx(0,y)=y(0−2y2)y2−0=−2y.f_x(0,y)=\frac{y(0-2y^{2})}{y^{2}}-0=-2y.

Step 3 — Compute fxy(0,0)f_{xy}(0,0)

fxy(0,0)=lim⁡k→0fx(0,k)−fx(0,0)k=lim⁡k→0−2k−0k=−2.f_{xy}(0,0)=\lim_{k\to 0}\frac{f_x(0,k)-f_x(0,0)}{k}=\lim_{k\to 0}\frac{-2k-0}{k}=-2.

Step 4 — fy(x,0)f_y(x,0) for x≠0x\ne 0

Differentiating ff w.r.t. yy gives:

fy=3x(x2−2y2)x2+y2−2xy2(3x2−2y2)(x2+y2)2.f_y=\frac{3x(x^{2}-2y^{2})}{x^{2}+y^{2}}-\frac{2xy^{2}(3x^{2}-2y^{2})}{(x^{2}+y^{2})^{2}}.

At y=0y=0, x≠0x\ne 0:

fy(x,0)=3x⋅x2x2−0=3x.f_y(x,0)=\frac{3x\cdot x^{2}}{x^{2}}-0=3x.

Step 5 — Compute fyx(0,0)f_{yx}(0,0)

fyx(0,0)=lim⁡h→0fy(h,0)−fy(0,0)h=lim⁡h→03h−0h=3.f_{yx}(0,0)=\lim_{h\to 0}\frac{f_y(h,0)-f_y(0,0)}{h}=\lim_{h\to 0}\frac{3h-0}{h}=3.

Summary

  fxy(0,0)=−2,fyx(0,0)=3.  \boxed{\;f_{xy}(0,0)=-2,\quad f_{yx}(0,0)=3.\;}

Since these are different, Clairaut’s theorem must fail — meaning at least one of fxyf_{xy} or fyxf_{yx} is discontinuous at (0,0)(0,0). In fact, both are.

Continuity discussion

Away from (0,0)(0,0), f∈C∞f\in C^{\infty}, so fxy=fyxf_{xy}=f_{yx} as functions (Clairaut). Call this common formula g(x,y)g(x,y). From the calculations above:

Different limits along different paths through the origin ⇒ gg has no limit at (0,0)(0,0). Hence both fxyf_{xy} and fyxf_{yx} (which equal gg off the origin) are discontinuous at (0,0)(0,0) — the limit doesn’t exist, regardless of how we set the value at the origin.

Answer

  Both fxy and fyx are discontinuous at (0,0).  \boxed{\;\text{Both }f_{xy}\text{ and }f_{yx}\text{ are discontinuous at }(0,0).\;}
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