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Multivariate Calculus - Bruce E. Shapiro

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LECTURE 12. THE CHAIN RULE 87<br />

because the velocity vector has been defined as v = r ′ (t). Thus<br />

df<br />

dt<br />

= v(t) · ∇f = D v f(t)<br />

where v = ‖v(t)‖ is the speed at time t. Thus the total rate of change of a function<br />

as you move along a curve r(t) is the directional derivative in the direction of the<br />

tangent (or velocity) vector.<br />

Proof of the Chain Rule<br />

We outline the proof for a function f (x(t), y(t)) of two variables; the generalization<br />

to higher dimensions is the same.The derivative of f with respect to t is<br />

df<br />

dt = lim f(t + ∆t) − f(t)<br />

∆t→0 ∆t<br />

But<br />

f(t + ∆t) = f(x(t + ∆t), y(t + ∆t))<br />

so that<br />

f(t + ∆t) − f(t) = f(x(t + ∆t), y(t + ∆t)) − f(x(t), y(t))<br />

= f(x(t + ∆t), y(t + ∆t)) − f(x(t), y(t + ∆t))<br />

+f(x(t), y(t + ∆t)) − f(x(t), y(t))<br />

This is allowed because the two middle terms add to zero. Let<br />

∆x = x(t + ∆t) − x(t), ∆y = y(t + ∆t) − y(t)<br />

Then<br />

f(t + ∆t) − f(t) = f(x + ∆x, y + ∆y) − f(x, y + ∆y)<br />

+f(x, y + ∆y) − f(x(t), y(t))<br />

Math 250, Fall 2006 Revised December 6, 2006.

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