Multivariate Calculus - Bruce E. Shapiro

Multivariate Calculus - Bruce E. Shapiro Multivariate Calculus - Bruce E. Shapiro

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80 LECTURE 11. GRADIENTS AND THE DIRECTIONAL DERIVATIVE Hence At the point (1,1,1) we have 200(xi + yj + zk) ∇T (x, y, z) = − (10 + x 2 + y 2 + z 2 ) 2 ∂ ∂x ∣ −200x ∣∣∣(1,1,1) 10 + x 2 + y 2 + z 2 = −200 169 and similarly for the other two partial derivatives. Hence the direction of steepest increase in temperature is ∇T (x, y, z)| (1,1,1) = − 200 (i + j + k) 169 Theorem 11.5 The gradient vector is perpendicular to the level curves of a function. To see why this theorem is true, recall the definition of a level curve: it is a curve along which the value of z = f(x, y) is a constant. Thus if you move along a tangent vector to a level curve, the function will not change, and the directional derivative is zero. Since the directional derivative is the dot product of the gradient and the direction of motion, which in this case is the tangent vector to the level curve, this dot product is zero. But a dot product of two non-zero vectors can only be zero if the two vectors are perpendicular to one another. Thus the gradient must be perpendicular to the level curve. Corollary 11.1 Let f(x, y, z) = 0 describe a surface in 3D space. Then the threedimensional gradient vector ∇f is a normal vector to the surface. This result follows because a surface f(x, y, z) = 0 is a level surface of a function w = f(x, y, z). The value of f(x, y, z) does not change. So if you consider any tangent vector, the directional derivative along the tangent vector is zero. Consequently the tangent vector is perpendicular to the gradient. Revised December 6, 2006. Math 250, Fall 2006

Lecture 12 The Chain Rule Recall the chain rule from Calculus I: To find the derivative of some function u = f(x) with respect to a new variable t, we calculate du dt = du dx dx dt We can think of this as a sequential process, as illustrated in figure 12.1. 1. Draw a labeled node for each variable. The original function should be the furthest to the left, and the desired final variable the node furthest to the right. 2. Draw arrows connecting the nodes. 3. Label each arrow with a derivative. The variable on the top of the derivative corresponds to the variable the arrow is coming from and the variable on the bottom of the derivative is the variable the arrow is going to. 4. follow the path described by the labeled arrows. The derivative of the variable at the start of the path with respect to the variable at the end of the path is the product of the derivatives you meet along the way. Figure 12.1: Visualization of the chain rule for a function of a single variable Now suppose u is a function of two variables x and y rather than just one. Then we need to have two arrows emanating from u, one to each variable. This is illustrated in figure 12.2. The procedure is modified as follows: 1. Draw a node for the original function u, each variable it depends on x, y, ..., and the final variable that we want to find the derivative with respect to t. 81

80 LECTURE 11. GRADIENTS AND THE DIRECTIONAL DERIVATIVE<br />

Hence<br />

At the point (1,1,1) we have<br />

200(xi + yj + zk)<br />

∇T (x, y, z) = −<br />

(10 + x 2 + y 2 + z 2 ) 2<br />

∂<br />

∂x<br />

∣<br />

−200x ∣∣∣(1,1,1)<br />

10 + x 2 + y 2 + z 2 = −200<br />

169<br />

and similarly for the other two partial derivatives. Hence the direction of steepest<br />

increase in temperature is<br />

∇T (x, y, z)| (1,1,1)<br />

= − 200 (i + j + k)<br />

169<br />

Theorem 11.5 The gradient vector is perpendicular to the level curves of a function.<br />

To see why this theorem is true, recall the definition of a level curve: it is a<br />

curve along which the value of z = f(x, y) is a constant. Thus if you move along<br />

a tangent vector to a level curve, the function will not change, and the directional<br />

derivative is zero. Since the directional derivative is the dot product of the gradient<br />

and the direction of motion, which in this case is the tangent vector to the level<br />

curve, this dot product is zero. But a dot product of two non-zero vectors can only<br />

be zero if the two vectors are perpendicular to one another. Thus the gradient must<br />

be perpendicular to the level curve.<br />

Corollary 11.1 Let f(x, y, z) = 0 describe a surface in 3D space. Then the threedimensional<br />

gradient vector ∇f is a normal vector to the surface.<br />

This result follows because a surface f(x, y, z) = 0 is a level surface of a function<br />

w = f(x, y, z). The value of f(x, y, z) does not change. So if you consider any tangent<br />

vector, the directional derivative along the tangent vector is zero. Consequently<br />

the tangent vector is perpendicular to the gradient.<br />

Revised December 6, 2006. Math 250, Fall 2006

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