Calculus: Analytic Geometry and Calculus, with Vectors

(lu) #1
11.3 Formulas involving partial derivatives 581

Tau__au au sin 4,
apcos 0 -a4, P
On au au cos
aY

=
aP

sin }
To P

Then show that the formulas


axe=

Ca49
p(az)] ax+ [aO CaxJJ ax
49 a
ay2=Cap ayay + TOCaYU aye

can be put in the forms

(6) a2u =a2u cost4, - 2 a2u sin ¢ cos 4,

axe ape aP a P

+ au sins t + a2u sins + 2 au sin 0 cos 4,
ap p P2 To p2
(7) a2u=

192U
sins -I- 2 a2u sin ¢ cos 4,
aY2 a p2 ap ao P
+ au cost + a2u cost _ 2au sin ¢ cos 4,
ap p a4,2 p2 To p2
Show finally that

(8)

and hence
(9)

a2u a2u a2u 1 On 1 a2u
axe+ 0y2= apt + p oP+ pt 84,2

a2u a2u a2u 492U 1 au 1 a2u a2u
axe+8y2+az2

=apt+Pap+p'a2+az2

For use in the next remark, we note also the formula

(10) l auy aY l au + cos 4, au
P aP p2 sin ¢ 90

which comes from (5) and (1).
5 This remark can be very helpful to those who will study brands of physics
and engineering in which the Laplace equation, the heat equation, and the wave
equation appear. While the operation might be tedious and need not be per-
formed, we could copy all of Problem 4 with x, y, p, and 0 respectively replaced
by z, p, r, and 0. This shows us that if u is a function of z and p and if

z=rcos0, p = r sin 0,

(3)

a2u a2u atu 1 au

+

I a2u
az2 + apt are + r Or r2 002
lau__lau
+

cos0 au
p ap r ar 0 T O *
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