Surface area and surface integrals. (Sect. 16.5) Review ...
[Pages:15]Surface area and surface integrals. (Sect. 16.5)
Review: Arc length and line integrals. Review: Double integral of a scalar function. The area of a surface in space. Next class: Surface integrals of a scalar field. The flux of a vector field on a surface. Mass and center of mass thin shells.
Review: Arc length and line integrals.
The integral of a function f : [a, b] R is
b
n
a
f (x) dx = lim
n
f (xi) x.
i =0
The arc length of a curve r : [t0, t1] R3 in space is
t1
st1,t0 = |r (t)| dt.
t0
The integral of a function f : R3 R along a curve
t1
r : [t0, t1] R3 is f ds = f r(t) |r (t)| dt.
C
t0
The circulation of a function F : R3 R3 along a curve
t1
r : [t0, t1] R3 is F ? u ds = F r(t) ? r (t) dt.
C
t0
The flux of a function F : {z = 0} R3 {z = 0} R3 along
a loop r : [t0, t1] {z = 0} R3 is F = F ? n ds.
C
Surface area and surface integrals. (Sect. 16.5)
Review: Arc length and line integrals. Review: Double integral of a scalar function. The area of a surface in space.
Review: Double integral of a scalar function.
The double integral of a function f : R R2 R on a region R R2, which is the volume under the graph of f and above
the z = 0 plane, and is given by
nn
R
f
dA
=
lim
n
i =0
j =0
f
(xi, yj) x
y .
The area of a plane surface R R2 is the particular case f = 1, that is, A(R) = dA.
R
We now show how to compute: The area of a surface in space. The integral of a scalar function on a surface is space. The flux of a vector-valued function on a surface in space.
Surface area and surface integrals. (Sect. 16.5)
Review: Arc length and line integrals. Review: Double integral of a scalar function. The area of a surface in space.
The area of a surface in space.
Theorem
Given a smooth function f : R3 R, the area of a level surface S = {f (x, y , z) = 0}, over a closed, bounded region R in the plane
{z = 0}, is given by
|f |
A(S) =
dA.
R |f ? k|
z S = { f (x,y,z) = 0 } k f
Remark: Eq. (3), page 1183, in
the textbook is more general than the equation above, since the region R can be located on any plane, not only the plane {z = 0} considered here.
The vector p in the textbook is
y
the vector normal to R. In our
x
R
case p = k.
The area of a surface in space.
Proof: Introduce a partition in R R2, and consider an arbitrary
rectangle R in that partition. We compute the area P.
(x i , yi , z i ) u
P
v (x i ,yi +
y, z i )
It is simple to se that P = |u ? v|,
(x i + x, yi, z i )
k0
S u x v
x
y
R
and
u = x, 0, (zi - z^i ) , v = 0, y , (zi - zi ) . Therefore,
ij
k
u ? v = x 0 (zi - z^i ) = -y (zi - z^i ), -x(zi - zi ), xy .
0 y (zi - zi )
The area of a surface in space.
Proof: Recall: u ? v = -y (zi - z^i ), -x(zi - zi ), xy .
The linearization of f (x, y , z) at (xi , yi , zi ) implies f (x, y , z) f (xi , yi , zi ) + (x f )i x + (y f )i y + (z f )i (z - zi ).
Since f (xi , yi , zi ) = 0, f (xi + x, yi , z^i ) = 0, f (xi , yi + y , zi ) = 0,
0 = (x f )i x + (z f )i (zi - z^i )
(zi
-
z^i )
=
- (x f )i (z f )i
x ,
0 = (y f )i y + (z f )i (zi - zi )
(zi
-
zi)
=
- (y f )i (z f )i
y .
u?v =
(x f )i , (y f )i , (z f )i
x y u?v =
(f )i
xy .
(z f )i
(f ? k)i
P = |(f )i | xy A(S) =
|f | dA.
|(f ? k)i |
R |f ? k|
The area of a surface in space.
Example
Find the area of the surface in space given by the paraboloid z = x2 + y 2 between the planes z = 0 and z = 4.
Solution: The surface is the level surface of the function f (x, y , z) = x2 + y 2 - z. The region R is the disk z = x2 + y 2 4.
|f |
A(S) =
dx dy , f = 2x, 2y , -1 , f ? k = -1,
R |f ? k|
A(S) =
1 + 4x2 + 4y 2 dx dy .
R
Since R is a disk radius 2, it is convenient to use polar coordinates in R2. We obtain
2 2
A(S) =
1 + 4r 2 r dr d.
00
The area of a surface in space.
Example
Find the area of the surface in space given by the paraboloid z = x2 + y 2 between the planes z = 0 and z = 4.
2 2
Solution: Recall: A(S) =
00
2
A(S) = 2
1 + 4r 2 r dr ,
0
1 + 4r 2 r dr d. u = 1 + 4r 2, du = 8r dr .
2 A(S) =
17
u1/2 du
=
2
2
u3/2 17 .
81
83
1
We conclude: A(S) = (17)3/2 - 1 . 6
The area of a surface in space.
Remark: The formula for the area of a surface in space can be
generalized as follows.
Theorem
The area of a surface S given by f (x, y , z) = 0 over a closed and bounded plane region R in space is given by
z
f
f (x,y,z) = 0
|f |
A(S) =
dA,
R |f ? p|
R
y k
p
x
where p is a unit vector normal to the region R and f ? p = 0.
The area of a surface in space.
Example
Find the area of the region cut from the plane x + 2y + 2z = 5 by the cylinder with walls x = y 2 and x = 2 - y 2.
Solution:
z x + 2y + 2z = 5
The surface is given by f = 0 with f (x, y , z) = x + 2y + 2z - 5.
The region R is in the plane z = 0,
2
x
x = y2 y
1
x = 2 - y2
(x, y , z) : z = 0, y [-1, 1]
R=
x [y 2, (2 - y 2)]
.
|f |
Recall: A(S) =
dA. Here p = k, f = 1, 2, 2 .
R |f ? p|
The area of a surface in space.
Example
Find the area of the region cut from the plane x + 2y + 2z = 5 by the cylinder with walls x = y 2 and x = 2 - y 2.
|f |
Solution: A(S) =
dA. Here p = k, f = 1, 2, 2 .
R |f ? p|
Therefore: |f | = 1 + 4 + 4 = 3, and |f ? k| = 2.
And the region R = {(x, y ) : y [-1, 1], x [y 2, (2 - y 2)]}.
So we can write down the expression for A(S) as follows,
A(S) =
3
3 1 2-y 2
dx dy =
dx dy .
R2
2 -1 y 2
The area of a surface in space.
Example
Find the area of the region cut from the plane x + 2y + 2z = 5 by the cylinder with walls x = y 2 and x = 2 - y 2.
3 1 2-y 2
Solution: A(S) =
dx dy .
2 -1 y 2
3 A(S) =
1
2 - y2 - y2
3 dy =
1
2 - 2y 2 dy
2 -1
2 -1
A(S) = 3
1
1 - y2
dy = 3
y3 y-
1
1
1
=3 1- +1-
-1
3 -1
3
3
2
4
A(S) = 3 2 - = 3 A(S) = 4.
3
3
Surface area and surface integrals. (Sect. 16.5)
Review: The area of a surface in space. Surface integrals of a scalar field. The flux of a vector field on a surface. Mass and center of mass thin shells.
Review: The area of a surface in space.
Theorem
Given a smooth function f : R3 R, the area of a level surface S = {f (x, y , z) = 0}, over a closed, bounded region R in the plane
{z = 0}, is given by
|f |
A(S) =
dA.
R |f ? k|
z S = { f (x,y,z) = 0 } k f
Remark: Eq. (3), page 1183, in
the textbook is more general than the equation above, since the region R can be located on any plane, not only the plane {z = 0} considered here.
The vector p in the textbook is
y
the vector normal to R. In our
x
R
case p = k.
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