Multivariate Calculus - Bruce E. Shapiro
Multivariate Calculus - Bruce E. Shapiro
Multivariate Calculus - Bruce E. Shapiro
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76 LECTURE 11. GRADIENTS AND THE DIRECTIONAL DERIVATIVE<br />
Returning to equation 11.3, let u = uh/h where h = ‖h‖,i.e., any vector that is<br />
parallel to h but has magnitude u. Then<br />
f(P + (h/u)u) − f(P)<br />
lim<br />
= u · ∇f(P)<br />
h→0 h<br />
u<br />
(11.9)<br />
Since u is finite (but fixed), then h/u → 0 as h → 0, so that<br />
u · ∇f(P) =<br />
f(P + (h/u)u) − f(P)<br />
lim<br />
h/u→0 h/u<br />
(11.10)<br />
Finally, if we define a new k = h/u then we can make the following generalization<br />
of the derivative.<br />
Definition 11.6 The directional derivative of f in the direction of u at P<br />
is given by<br />
f(P + ku) − f(P)<br />
D u f(P) = u · ∇f(P) = lim<br />
(11.11)<br />
k→0 k<br />
Theorem 11.2 The following are equivalent:<br />
1. f(x, y) is differentiable at P<br />
2. f(x, y) is locally linear at P<br />
3. D u f(P) is defined at P<br />
4. The partial derivatives ∂f/∂x and ∂f/∂y exists and are continuous in some<br />
neighborhood of P.<br />
Figure 11.1: Geometric interpretation of partial derivatives as the slopes of a function<br />
in planes parallel to the coordinate planes.<br />
Example 11.3 Find the directional derivative of f(x, y) = 2x 2 + xy − y 2 at p =<br />
(3, −2) in the direction a = i − j.<br />
Revised December 6, 2006. Math 250, Fall 2006