Theorem The Mix Derivative
Theorem (Symmetry of Second Partial Derivative): If the function f:R2→R has continuous derivatives fxy and fyx at some point (a,b), then
fxy(a,b)=fyx(a,b)Proof:
W.L.O.G, for h>0,k>0, define
Δ=[f(a+h,b+k)−f(a+h,b)]−[f(a,b+h)−f(a,b)]Define F(x)=f(x,b+k)−f(x,b), which is continuous and differentiable (since fx exists on R). By mean value theorem, ∃a1∈[a,a+h] for which
Δ=F(a+h)−F(a)=F′(a1)h=[fx(a1,b+k)−fx(a1,b)]hApply again mean value theorem, ∃b1∈[b,b+k], s.t.,
Δ=fxy(a1,b1)khWe can also define G(y)=f(a+h,y)−f(a,y) and rewrite
Δ=G(b+h)−G(b)Similarly, by applying mean value theorem twice, ∃b2∈[b,b+k],a2∈[a,a+h], s.t,
Δ=fyx(a2,b2)hkPutting together
Δ=fxy(a1,b1)kh=fyx(a2,b2)hkBecause both fxy and fyx are continuous, as h→0 and k→0, fxy(a1,b1)→fxy(a,b) and fyx(a2,b2)→fyx(a,b), as desired.
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Theorem The Increment
If function f:R2→R has continuous derivative fx and fy at some point (a,b), then
f(a+h,b+k)−f(a,b)=fx(a,b)h+fy(a,b)k+ϵ1h+ϵ2kwhere ϵ1,ϵ2→0 as h,k→0.
Proof:
By mean value theorem, ∃a1 between a and a+h, ∃b1 between b and b+k, s.t.,
f(a+h,b+k)−f(a,b)=f(a+h,b+k)−f(a+h,b)+f(a+h,b)−f(a,b)=fy(a+h,b1)k+fx(a1,b)hDefine ϵ1=fx(a1,b)−fx(a,b) and ϵ2=fy(a+h,b1)−fy(a,b), we infer that
f(a+h,b+k)−f(a,b)=fx(a,b)h+fy(a,b)k+ϵ1h+ϵ2kThe claim ϵ1,ϵ2→0 as h,k→0 results from the continuity of fx and fy.
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Reference
- George B. Thomas, Jr., Maurice D. Weir, Joel Hass, THOMAS’ CALCULUS