11.2 Increments, chain rule, and gradients 565linked to t by the intermediate variables x, y, z which are functions of t.
We can then abbreviate (11.232) to
du au dx audy au dz
(11.234)
dt - ax dt + ay St + -Oz dtIt turns out that, in practice, the version (11.234) of the chain formula
is often very convenient. For example, if
u = x2 + y2 + z2, x = sin t, y = et, Z = t2,
then
du
= 2x cos t + 2ye° + 4zt
atand it is, in fact, not always necessary or even desirable to express the
right side entirely in terms of t. The abbreviations are not always so
agreeable, however. In case the parameter t is x itself, we must employ
considerable fortitude to comprehend the sentence containing (11.233)
and the formula
(11.235)du_au +audy+au dz
dx ax ay dx az dxIt is awkward and perhaps even undesirable to be required to think of u
depending upon x in two different ways. It is easier to letand to writew(x) = u(x, y(x), z(x))dw_au dx au dy au A
dx axdx+aydx+azdxand then observe that dx/dx = 1. While Theorem 11.23 is the fully
meaningful theorem to which we can refer when meanings of symbols
must be carefully set forth, we give a restatement of the theorem in
terms of the simpler curly dee notation.
Theorem 11.24 (chain rule, second version) If u is continuous and
has continuous partial derivatives au/ax, au/ay, au/az over a region R in
Ea, and if
(11.241) u = u(x,y,z),where x, y, z are differentiable functions of t over some interval T, and if the
point P having coordinate (x,y,z) traverses a curve C in R as t increases
over T, then is is differentiable over T anddu_au d x audy au dz
(11.242) dt ax YT+ay 77+az dt
It is not often that we have an opportunity to make an observation