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This worksheet from math 223-01 covers the evaluation of various vector calculus integrals using techniques such as the divergence theorem, stokes' theorem, and green's theorem. Students are required to identify the appropriate method for each integral and perform the necessary calculations.
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Math 223-01 (Salomone)
August 6, 2007
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Prob. 1
Prob. 2
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Problem 1. (8 points) For each of the following integrals, circle the technique(s) you could use to evaluate it.
There may be more than one answer.
(a) (2 points)
x
S
F · n dA where F (x, y, z) = 〈x, 2 y, 3 z〉 and S is the surface of a 2 × 2 × 2 cube centered at the
origin, oriented outwards.
Path Shape Green’s Stokes’ Divergence None of
Independence Independence Theorem Theorem Theorem the above
Here, S is a closed surface, so the divergence theorem is in play. But ∇ · F = 6 , 0, so this field is not shape independent and hence
F , ∇ × G so Stokes’ theorem is not possible.
(b) (2 points)
x
S
F · n dA where F (x, y, z) = ∇ × 〈x
2 − y, y
2 − z, z
2 − x〉 and S is the upper hemisphere of radius 5
centered at the origin, oriented upwards.
Path Shape Green’s Stokes’ Divergence None of
Independence Independence Theorem Theorem Theorem the above
Here, S is not a closed surface, so divergence theorem won’t work. But since F = ∇ × G is a curl vector field, it must be shape
independent! And since the vector potential G is known, you can use Stokes’ theorem to turn this surface integral into a line integral.
(c) (2 points)
C
F · d r , where F (x, y, z) = 〈yz, xz, xy〉 and C is the triangular path from (1, 0 , 0) to (0, 2 , 0) to (0, 0 , 3)
and back to (1, 0 , 0).
Path Shape Green’s Stokes’ Divergence None of
Independence Independence Theorem Theorem Theorem the above
First of all, notice this is a line integral! The curve C is closed, so we may use Stokes’ theorem. Moreover, ∇ × F = 〈 0 , 0 , 0 〉 so this field
is path-independent. This combination implies the integral is zero, in fact.
(d) (2 points)
x
S
F · n dA where F (x, y, z) = 〈y + z, x + z, x + 2 y〉 and S is the unit disk x
2
2 ≤ 1 in the xz-plane,
oriented in the positive y-direction.
Path Shape Green’s Stokes’ Divergence None of
Independence Independence Theorem Theorem Theorem the above
S is not a closed surface, here; it does not divide space into an inside and outside. Thus the divergence theorem is not an option. But
∇ · F = 0, so this vector field is shape independent, i.e. there is a vector field G such that F = ∇ × G. Since we don’t know what G is,
however, using Stokes’ theorem to convert to a line integral is not an option.
Problem 2. (12 points) Evaluate the following integrals using whatever method is most convenient.
(a) (6 points)
x
S
F · n dA, where F (x, y, z) = 〈yz, x− 2 ye
z , 2 e
z 〉 and S is the portion of the paraboloid z = 49 −x
2 − y
2
lying above the xy-plane, oriented upwards.
S is not a closed surface; thus the divergence theorem is not an option. But
∂x
(yz) +
∂y
(x − 2 ye
z ) +
∂z
(2e
z ) = 0 − 2 e
z
z = 0 ,
so this is a shape-independent vector field! This allows us to replace the surface S with any other
surface, as long as the boundary and orientation are the same.
Since the boundary of this surface lies on the xy-plane where z = 0, the boundary consists of the circle
0 = 49 − x
2 − y
2 i.e. x
2
2 = 49.
We can therefore replace S with the simpler surface T: the disk of radius 7 in the xy-plane, i.e.
x
2
2 ≤ 49, z = 0.
Since this surface lies in the xy-plane, the normal vector can be chosen to be n = 〈 0 , 0 , 1 〉. Then
F · n = 2 e
z , so the surface integral can be computed
x
x
2 +y
2 ≤ 49
2 e
z
z= 0
dA =
x
x
2 +y
2 ≤ 49
2 e
0 dA = 2
x
x
2 +y
2 ≤ 49
dA = 2 π(7)
2 = 98 π.
(b) (6 points)
x
S
Q · n dA, where Q (x, y, z) = 〈x
3
3
3
cone” bounded by z
2 = x
2
2 and x
2
2
2 = 162, oriented outwards.
Since S is a closed surface, we can (and should!) use the divergence theorem. The divergence of Q is
∇ · Q = 3 x
2
2
2 ,
so if we call the solid region inside the ”ice cream cone” W we have
S
Q · n dA =
y
W
(∇ · Q ) dV =
y
W
3(x
2
2
2 ) dV.
To describe the ice-cream cone in spherical coordinates, convert the sphere’s equation to ρ =
2 and the cone’s equation to φ = π/4. Then the tape-measurement yields
0 ≤ ρ ≤ 9
0 ≤ θ ≤ 2 π
0 ≤ φ ≤ π/ 4.
Since ∇ · Q = 3(x
2
2
2 ) = 3 ρ
2 , the triple integral becomes
y
W
3(x
2
2
2 ) dV =
π/ 4
0
2 π
0
9
√
2
0
3 ρ
2 ρ
2 sin φ dρdθdφ
= (− cos φ)
π/ 4
0
(θ)
2 π
0
ρ
5
√
2
0
(2π)
5
1417176 π