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Solutions to quiz #6 for math 223-01, focusing on vector calculus problem-solving. The quiz covers techniques for evaluating vector fields along curves, including path independence, green's theorem, and stokes' theorem. The document also includes calculations for determining work done by a force field along a rectangular path and computing line integrals for a non-closed curve.
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Math 223-01 (Salomone)
August 3, 2007
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Name: Solution
Prob. 1
Prob. 2
Prob. 3
Total / 25
Problem 1. (8 points) For each of the following vector field / curve combinations, simply circle the techniques
that you could use to evaluate
C
F · d r. There may be more than one answer. No partial credit will be
assessed on this problem.
(a) (2 points) F (x, y, z) = 〈y, z, x〉 and C is the triangle from (0, 0 , 0) to (1, 0 , 2) to (− 1 , − 1 , 0) and back to (0, 0 , 0).
Path Independence Green’s Theorem Stokes’ Theorem None of the Above
Note that C is a closed curve, and ∇ × F = 〈− 1 , − 1 , − 1 〉 , 0 so F is not path-independent.
(b) (2 points) F (x, y) = 〈x
2 − 2 xy + y
2 , x
2 − 2 xy − y
2 〉 and C is the line segment from (− 3 , 3) to (6, 2).
Path Independence Green’s Theorem Stokes’ Theorem None of the Above
Here, C is not a closed curve, and ∇ ∗ F = 2 x − 2 y − (2y − 2 x) = − 4 x − 4 y , 0, so it is not path independent.
(c) (2 points) F (x, y, z) = 〈xyz, xyz, xyz〉 and C is the curve parameterized by r (t) = (cos t, sin t, 1 + sin
2 t),
0 ≤ t ≤ 2 π.
Path Independence Green’s Theorem Stokes’ Theorem None of the Above
Since r (0) = (1, 0 , 1) = r (2π), this is a closed curve. However, ∇ × F = 〈xz − xy, xy − yz, yz − xz〉 , 0 so it is not path independent.
(d) (2 points) F (x, y) =
x √
x 2 +y 2 − 1
y √
x 2 +y 2 − 1
and C is the circle x
2
2 = 4, traversed counterclockwise.
Path Independence Green’s Theorem Stokes’ Theorem None of the Above
This vector field is undefined on the unit disk x
2
2 ≤ 1; since the path C encircles this hole, all bets are off. Even though F
happens to pass the screening test and C is a closed curve, none of these techniques is guaranteed to give the right answer.
Problem 2. (8 points) A particle moves along a rectangular path from (− 2 , 0) to (3, 0) to (3, 1) to (− 2 , 1) and
back to (− 2 , 0). How much work does the force field F (x, y) = 〈sin
2 x + 2 xy
2 , y
y
2 y〉 do along this path?
Since the path involved is a closed curve in R
2 , we may use Green’s theorem. The region R inside this
curve is the rectangle − 2 ≤ x ≤ 3, 0 ≤ y ≤ 1. Check that the curve C is counterclockwise, so no extra
negative signs are necessary. By Green’s theorem, we have
C
F · d r =
x
R
∂x
∂y
dA.
We compute
∂x
∂y
∂x
(y
y
2 y) −
∂y
(sin
2 x + 2 xy
2 ) = 8 xy − 4 xy = 4 xy.
Thus the integral on the right-hand side of Green’s theorem is
x
R
4 xy dA =
1
0
3
− 2
4 xy dxdy =
1
0
2 x
2 y
x= 3
x=− 2
dy
1
0
10 y dy = 5 y
2
1
0
Problem 3. (9 points) Let F (x, y, z) = 〈x − z, z − x,
x
2
z = x
2
2
y = x
from (0, 0 , 0) to (2, 2 , 8).
Compute
C
F · d r.
x
y
z
(0,0,0)
z = x + y
(2,2,8)
2 2
y = x
The curve C is not closed, so we may not use Stokes’ theorem. Furthermore, the curl of F is
i j k
∂
∂x
∂
∂y
∂
∂z
x − z z − x
x
2
x
√
x
2
so this field is not path independent. We must use brute force to compute this line integral.
First, we parameterize the curve C. As the intersection of two surfaces, we may first parameterize one
of the surfaces and then eliminate a parameter. The graph z = x
2
2 can be parameterized using its
independent variables x = s, y = t:
u (s, t) = ( s, t, s
2
2 ).
Then the equation y = x implies that s = t, which eliminates a parameter and gives us our curve:
r (t) = u (t, t) = ( t, t, t
2
2 ) = ( t, t, 2 t
2 ), 0 ≤ t ≤ 2.
Then
F ( r (t)) = 〈t − 2 t
2 , 2 t
2 − t,
t
2
2 )〉 = 〈t − 2 t
2 , 2 t
2 − t, 3 t〉
· r
′ (t) = 〈 1 , 1 , 4 t〉
F ( r (t)) · r
′ (t) = t − 2 t
2
2 − t + 12 t
2 = 12 t
2 .
So the line integral evaluates to
C
F · d r =
2
0
12 t
2 dt
= 4 t
3
2
0