Multivariate Calculus - Bruce E. Shapiro
Multivariate Calculus - Bruce E. Shapiro Multivariate Calculus - Bruce E. Shapiro
186 LECTURE 22. LINE INTEGRALS The first integral does not depend on x; in fact the only place that x appears on the right hand side of the equation is in the upper limit of the second integral. But in the second integral the values of y and z are constant, hence F · dr = M(x, y, z)dx. ∂f(x, y, z) ∂x = ∂ ∂x ∫ x x 1 M(u, y, z)du = M(x, y, z) (22.32) where the last equality follows from the fundamental theorem of calculus. Similarly we can pick a point (x, y 1 , z) such that f(x, y, z) − f(A) = ∫ (x,y1 ,z) (x a,y a,z a) F · dr + ∫ (x,y,z) (x,y 1 ,z) F · dr Now the first integral does not depend on y, and the second integral has x and z fixed, so that F · dr = N(x, y, z)dy in the second integrand and ∂f(x, y, z) ∂y = ∂ ∂y ∫ y y 1 N(x, u, z)du = N(x, y, z) (22.33) Finally, we can pick a point (x, y, z 1 ) such that f(x, y, z) − f(A) = ∫ (x,y,z1 ) (x a,y a,z a) F · dr + ∫ (x,y,z) (x,y,z 1 ) F · dr Now the first integral does not depend on z, and the second integral has x and y fixed, so that F · dr = P (x, y, z)zy in the second integrand and ∂f(x, y, z) ∂z = ∂ ∂z ∫ z z 1 P (x, y, u)du = P (x, y, z) (22.34) Combining equations 22.31, 22.32, 22.33, and 22.34, we have ( ) ∂f F = (M, N, P ) = ∂x , ∂f ∂y , ∂f = ∇f (22.35) ∂z Thus F = ∇f, i.e, F is a gradient field. Theorem 22.3 A vector field F is a gradient field if and only if ∮ F · dr = 0 for every closed curved C. C Proof. F is a gradient field if and only if it is path independent. Pick any two points on the closed curve C, and call them A and B. Let C 1 be one path from A to B along C, and let C 2 be the path from A to B along the other half of C. Then ∮ F · dr = C ∫ F · dr − C 1 ∫ F · dr C 2 Revised December 6, 2006. Math 250, Fall 2006
LECTURE 22. LINE INTEGRALS 187 The second integral is negative because the C 2 is oriented from A to B and not from B to A as it would have to be to complete the closed curves. But the integrals over C 1 and C 2 are two paths between the same two points; hence by the path independence theorem, ∫ ∫ F · dr = F · dr C 1 C 2 and conseequently ∮ C F · dr = 0. The following theorem gives an easy test to see if any given field is a gradient field. Theorem 22.4 F is a gradient field if and only if ∇ × F = 0. Proof. First, suppose F is a gradient field. Then there exists some scalar function f such that F = ∇f. But ∇ × F = ∇ × ∇f = 0 because curl gradf = 0 for any function f. The proof in the other direction, namely, that if ∇ × F = 0 then F is a gradient function, requires the use of Stoke’s theorem, which we shall prove in the next section. Stoke’s theorem gives us the formula ∮ F · dr = (∇ × F) · dr C where A is the area encloses by a closed path C. But if the curl F is zero, then ∮ F · dr = 0 C A Since the integral over a closed path is zero, the integral must be path-independent, and hence the integrand must be a gradient field. Theorem 22.5 The following statements are equivalent: 1. F is a gradient field. 2. ∇ × F = 0 3. There exists some scalar function f such that F = ∇f. 4. The line integral is path independent: for some scalar function f, ∫ B A F · dr = f(B) − f(A) Math 250, Fall 2006 Revised December 6, 2006.
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LECTURE 22. LINE INTEGRALS 187<br />
The second integral is negative because the C 2 is oriented from A to B and not from<br />
B to A as it would have to be to complete the closed curves.<br />
But the integrals over C 1 and C 2 are two paths between the same two points;<br />
hence by the path independence theorem,<br />
∫ ∫<br />
F · dr = F · dr<br />
C 1 C 2<br />
and conseequently<br />
∮<br />
C<br />
F · dr = 0. <br />
The following theorem gives an easy test to see if any given field is a gradient field.<br />
Theorem 22.4 F is a gradient field if and only if ∇ × F = 0.<br />
Proof. First, suppose F is a gradient field. Then there exists some scalar function<br />
f such that F = ∇f. But<br />
∇ × F = ∇ × ∇f = 0<br />
because curl gradf = 0 for any function f.<br />
The proof in the other direction, namely, that if ∇ × F = 0 then F is a gradient<br />
function, requires the use of Stoke’s theorem, which we shall prove in the next<br />
section. Stoke’s theorem gives us the formula<br />
∮ <br />
F · dr = (∇ × F) · dr<br />
C<br />
where A is the area encloses by a closed path C. But if the curl F is zero, then<br />
∮<br />
F · dr = 0<br />
C<br />
A<br />
Since the integral over a closed path is zero, the integral must be path-independent,<br />
and hence the integrand must be a gradient field. <br />
Theorem 22.5 The following statements are equivalent:<br />
1. F is a gradient field.<br />
2. ∇ × F = 0<br />
3. There exists some scalar function f such that F = ∇f.<br />
4. The line integral is path independent: for some scalar function f,<br />
∫ B<br />
A<br />
F · dr = f(B) − f(A)<br />
Math 250, Fall 2006 Revised December 6, 2006.