Multivariate Calculus - Bruce E. Shapiro
Multivariate Calculus - Bruce E. Shapiro Multivariate Calculus - Bruce E. Shapiro
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
- Page 41 and 42: Lecture 4 Lines and Curves in 3D We
- Page 43 and 44: LECTURE 4. LINES AND CURVES IN 3D 3
- Page 45 and 46: LECTURE 4. LINES AND CURVES IN 3D 3
- Page 47 and 48: LECTURE 4. LINES AND CURVES IN 3D 3
- Page 49 and 50: Lecture 5 Velocity, Acceleration, a
- Page 51 and 52: LECTURE 5. VELOCITY, ACCELERATION,
- Page 53 and 54: LECTURE 5. VELOCITY, ACCELERATION,
- Page 55 and 56: LECTURE 5. VELOCITY, ACCELERATION,
- Page 57 and 58: Lecture 6 Surfaces in 3D The text f
- Page 59 and 60: Lecture 7 Cylindrical and Spherical
- Page 61 and 62: LECTURE 7. CYLINDRICAL AND SPHERICA
- Page 63 and 64: Lecture 8 Functions of Two Variable
- Page 65 and 66: LECTURE 8. FUNCTIONS OF TWO VARIABL
- Page 67 and 68: LECTURE 8. FUNCTIONS OF TWO VARIABL
- Page 69 and 70: LECTURE 8. FUNCTIONS OF TWO VARIABL
- Page 71 and 72: Lecture 9 The Partial Derivative De
- Page 73 and 74: LECTURE 9. THE PARTIAL DERIVATIVE 6
- Page 75 and 76: LECTURE 9. THE PARTIAL DERIVATIVE 6
- Page 77 and 78: LECTURE 9. THE PARTIAL DERIVATIVE 6
- Page 79 and 80: Lecture 10 Limits and Continuity In
- Page 81 and 82: LECTURE 10. LIMITS AND CONTINUITY 6
- Page 83 and 84: LECTURE 10. LIMITS AND CONTINUITY 7
- Page 85 and 86: Lecture 11 Gradients and the Direct
- Page 87 and 88: LECTURE 11. GRADIENTS AND THE DIREC
- Page 89 and 90: LECTURE 11. GRADIENTS AND THE DIREC
- Page 91: LECTURE 11. GRADIENTS AND THE DIREC
- Page 95 and 96: LECTURE 12. THE CHAIN RULE 83 The p
- Page 97 and 98: LECTURE 12. THE CHAIN RULE 85 Examp
- Page 99 and 100: LECTURE 12. THE CHAIN RULE 87 becau
- Page 101 and 102: LECTURE 12. THE CHAIN RULE 89 Solut
- Page 103 and 104: LECTURE 12. THE CHAIN RULE 91 Examp
- Page 105 and 106: Lecture 13 Tangent Planes Since the
- Page 107 and 108: LECTURE 13. TANGENT PLANES 95 Solut
- Page 109 and 110: LECTURE 13. TANGENT PLANES 97 Multi
- Page 111 and 112: LECTURE 13. TANGENT PLANES 99 Accor
- Page 113 and 114: Lecture 14 Unconstrained Optimizati
- Page 115 and 116: LECTURE 14. UNCONSTRAINED OPTIMIZAT
- Page 117 and 118: LECTURE 14. UNCONSTRAINED OPTIMIZAT
- Page 119 and 120: LECTURE 14. UNCONSTRAINED OPTIMIZAT
- Page 121 and 122: LECTURE 14. UNCONSTRAINED OPTIMIZAT
- Page 123 and 124: LECTURE 14. UNCONSTRAINED OPTIMIZAT
- Page 125 and 126: LECTURE 14. UNCONSTRAINED OPTIMIZAT
- Page 127 and 128: LECTURE 14. UNCONSTRAINED OPTIMIZAT
- Page 129 and 130: Lecture 15 Constrained Optimization
- Page 131 and 132: LECTURE 15. CONSTRAINED OPTIMIZATIO
- Page 133 and 134: LECTURE 15. CONSTRAINED OPTIMIZATIO
- Page 135 and 136: LECTURE 15. CONSTRAINED OPTIMIZATIO
- Page 137 and 138: LECTURE 15. CONSTRAINED OPTIMIZATIO
- Page 139 and 140: Lecture 16 Double Integrals over Re
- Page 141 and 142: LECTURE 16. DOUBLE INTEGRALS OVER R
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