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A comprehensive set of practice problems for calculus iii, covering topics such as vector equations of lines, parametric equations, equations of planes, tangent lines to curves, velocity and acceleration, parametrization of curves, level curves and surfaces, partial derivatives, directional derivatives, gradient vectors, tangent planes, double and triple integrals, line integrals, and conservative vector fields. The problems are designed to reinforce key concepts and provide students with valuable practice for exams.
Typology: Exams
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i − 3
j + 7
k, and contains the point (2, 1 , −3), then its vector
equation is
A. ~r = (1 + 2t)
i − 3 t~j + (−2 + 7t)
k B. ~r = (2 + t)
i − 3
j + (7 − 2 t)
k
C. ~r = (2 + 2t)
i + (1 − 3 t)
j + (−3 + 7t)
k D. ~r = (2 + 2t)
i + (−3 + t)
j + (7 − 3 t)
k
E. ~r = (2 + t)
i +
j + (7 − 3 t)
k
A. x = 1 − 3 t, y = −1 + 4t, z = 5t B. x = t, y = −t, z = 0
C. x = 1 − 2 t, y = −1 + 3t, z = 5t D. x = − 2 t, y = 3t, z = 5t
E. x = −1 + t, y = 2 − t, z = 5
1
2
i + 2
j + 3
k.
A. x − y − z +
9
2
= 0 B. x + 4y + 6z + 9 = 0 C.
x− 1
1
2
y+
2
z+
3
D. x − y − z = 0 E.
1
2
x + 2y + 3z = 1
A. 6 x − 11 y + z = 5 B. 6 x + 11y + z = 5 C. 11 x − 6 y + z = 0
D. ~r = 18
i − 33
j + 3
k E. x − 6 y − 11 z = 12
2 ~ j + t
3 ~ k at the point (2, 4 , 8)
A. x = 2 + t, y = 4 + 4t, z = 8 + 12t B. x = 1 + 2t, y = 4 + 4t, z = 12 + 8t
C. x = 2t, y = 4t, z = 8t D. x = t, y = 4t, z = 12t E. x = 2 + t, y = 4 + 2t, z = 8 + 3t
~r(t) = cos t~i + 3 sin t~j − t
2 ~ k
Find the velocity, acceleration, and speed of the object when t = π.
Velocity Acceleration Speed
i − π
2 ~ k − 3
j − 2 π
k
1 + π
4
i − 3
j + 2π
k −
i − 2
k
10 + 4π
2
j − 2 π
k −
i − 2
k
9 + 4π
2
j − 2 π
k
i − 2
k
9 + 4π
2
i − 2
k − 3
j − 2 π
k
(− 1 , 0 , 5) is
A. ~r(t) = sin t~i + cos t~j + 5
k, 0 ≤ t ≤ π B. ~r(t) = cos t~i + sin t~j + 5
k, 0 ≤ t ≤ π
C. ~r(t) = cos t~i + sin t~j + 5
k,
π
2
≤ t ≤
3 π
2
D. ~r(t) = cos t~i + sin t~j + 5
k, 0 ≤ t ≤
π
2
E. ~r(t) = sin t + cos t~j + 5
k,
π
2
≤ t ≤
3 π
2
2
3
(1 + t)
3
2
i +
2
3
(1 − t)
3
2
j + t
k, − 1 ≤ t ≤ 1 is
1
2
1 − x
2 − 2 y
2 are
A. circles B. lines C. parabolas D. hyperbolas E. ellipses
2
−y
2
that passes through the point (1, 2 , −3) intersects
the (x, z)-plane (y = 0) along the curve
A. z = x
2
2 − 8 C. z = x
2
2 − 8
E. does not intersect the (x, z)-plane
(1) x
2
2
2
= 4 (a) paraboloid
(2) x
2
2
= 4 (b) sphere
(3) x
2
2 = z
2 (c) cylinder
(4) x
2
2 = z (d) double cone
(5) x
2
2
2
= 1 (e) ellipsoid
A. 1b, 2c, 3d, 4a, 5e B. 1b, 2c, 3a, 4d, 5e C. 1e, 2c, 3d, 4a, 5b
D. 1b, 2d, 3a, 4c, 5e E. 1d, 2a, 3b, 4e, 5c
2
/v where u = g 1 (t) and v = g 2 (t) are differentiable functions of t. If g 1
g 2 (1) = 2, g
′
1
(1) = 5 and g
′
2
(1) = −4, find
dw
dt
when t = 1.
uv
and u = r + s, v = rs, find
∂w
∂r
A. e
(r+s)rs
(2rs + r
2
) B. e
(r+s)rs
(2rs + s
2
) C. e
(r+s)rs
(2rs + r
2
)
D. e
(r+s)rs (1 + s) E. e
(r+s)rs (r + s
2 ).
x
2 y
4
x
4
8
when x 6 = 0 and f (0, 0) = 0. Which of the following are (is) true?
i) ∂f /∂x(0, 0) and ∂f /∂y(0, 0) exist at (0, 0).
ii) f (x, y) is continuous at (0, 0).
iii) The graph of z = f (x, y) has a tangent plane at (0, 0 , 0).
A. i) only B. i) and ii) only C. i) and iii) only D. i) ii), and iii) E. None
3
− 6 xy − 3 y
2
has
A. a relative minimum and a saddle point B. a relative maximum and a saddle point
C. a relative minimum and a relative maximum D. two saddle points
E. two relative minima.
2
2
on the curve
xy = 1. In using the method of Lagrange multipliers, the value of λ (even though it is not needed) will
be
1 √
2
3
1
x
0
1
x
dydx.
8
9
B. 2 C. ln 3 D. 0 E. ln 2.
R
f (x, y)dA, where R is the portion of the disk x
2
2
≤ 1, in the upper
half-plane, y ≥ 0. Express the integral as an iterated integral.
1
− 1
√
1 −x
2
−
√
1 −x
2 f (x, y)dydx B.
0
− 1
√
1 −x
2
0
f (x, y)dydx
1
− 1
√
1 −x
2
0
f (x, y)dydx D.
1
0
√
1 −x
2
−
√
1 −x
2
f (x, y)dydx
1
0
√
1 −x
2
0
f (x, y)dydx.
2
0
2 x
x
2 f (x, y)dydx =
4
0
b
a
f (x, y)dxdy.
A. a = y
2
, b = 2y B. a =
y
2
, b =
y C. a =
y
2
, b = y
D. a =
y, b =
y
2
E. cannot be done without explicit knowledge of f (x, y).
R
ydA, where R is the region of the (x, y)-plane inside the triangle with
vertices (0, 0), (2, 0) and (2, 1).
8
3
2
3
1
3
2
, below
by the xy plane, and on the sides by the planes y = 0 and y = x is given by the double integral
1
0
x
0
(1 − x
2 )dydx B.
1
0
1 −x
2
0
x dydx C.
1
− 1
x
−x
(1 − x
2 )dydx
1
0
0
x
(1 − x
2
)dydx E.
1
0
1 −x
2
x
dydx.
5 π
6
25 π
12
25 π
6
5 π
3
25 π
3
2 , y = x, y = 0, z = 0 and x = 4. The
volume of the region is
64
3
32
3
16
3
2
2
2 = 32 and below by the cone
z =
x
2
2
. The mass density at any point of the object is equal to its distance from the xy plane.
Set up a triple integral in rectangular coordinates for the total mass m of the object.
4
− 4
√
16 −x
2
−
√
16 −x
2
32 −x
2 −y
2
−
x
2 +y
2
z dz dy dx B.
4
− 4
√
16 −x
2
−
√
16 −x
2
32 −x
2 −y
2
x
2 +y
2
z dz dy dx
2
− 2
√
4 −x
2
−
√
4 −x
2
32 −x
2 −y
2
−
x
2 +y
2
z dz dy dx D.
4
0
√
16 −x
2
0
32 −x
2 −y
2
x
2 +y
2
z dz dy dx
4
− 4
√
16 −x
2
−
√
16 −x
2
32 −x
2 −y
2
x
2 +y
2
xy dz dy dx.
2 π
0
∫ π
4
0
√
32
0
ρ
3
cos ϕ sin ϕ dρ dϕ dθ B.
2 π
0
∫ π
4
0
√
32
0
ρ cos ϕ sin ϕ dρ dϕ dθ
2 π
0
∫ π
4
0
√
32
0
ρ
3
sin
2
ϕ dρ dϕ dθ D.
2 π
0
∫ π
2
0
√
32
0
ρ
3
cos ϕ sin ϕ dρ dϕ dθ
2 π
0
∫ π
4
0
√
32
0
ρ cos ϕ dρ dϕ dθ.
1
0
√
1 −x
2
0
y
2 (x
2
2 )
3 dydx when converted to polar coordinates becomes
π
0
1
0
r
9
sin
2
θ dr dθ B.
∫ π
2
0
1
0
r
8
sin
2
θ dr dθ C.
π
0
1
0
r
8
sin θ dr dθ
∫ π
2
0
1
0
r
8 sin θ dr dθ E.
∫ π
2
0
1
0
r
9 sin
2
θ dr dθ.
2
− 2
√
4 −x
2
−
√
4 −x
2
2 √
x
2 +y
2
dz dy dx
from rectangular to cylindrical coordinates?
π
0
2
0
2
r
r dz dr dθ B.
2 π
0
2
0
2
r
r dz dr dθ C.
2 π
0
2
− 2
2
r
r dz dr dθ
π
0
2
0
2
r
r dz dr dθ E.
2 π
2
0
2
− 2
2
r
r dz dr dθ.
4 − x
2 − y
2 and
z =
1 − x
2 − y
2 , then
D
x
2
2
2 dV =
14 π
3
16 π
3
15 π
2
D. 8 π E. 15 π.
1 − x
2 to (0, 1), and then back to (0, 0)
along the y-axis, then
C
xy dy =
1
0
√
1 −x
2
0
y dy dx B.
1
0
√
1 −x
2
0
y dy dx C. −
1
0
√
1 −x
2
0
x dy dx
1
0
√
1 −x
2
0
x dy dx E. 0
C
F · d~r, if
F (x, y) = (xy
2 − 1)
i + (x
2 y − x)
j and C is the circle of radius 1 centered at (1, 2)
and oriented counterclockwise.
A. 2 B. π C. 0 D. −π E. − 2
over the boundary C of R, oriented counterclockwise. Area of R =
R
dA =
C
y dx B.
C
y dx C.
C
x dx D.
1
2
C
y dx − x dy E. −
x dy
S
x dσ where S is the part of the plane 2x + y + z = 4 in the first octant.
8
3
8
3
√
14
3
√
10
3
2
2 with z ≤ 4, ~n is the unit normal vector on S directed
upward, and
F (x, y, z) = x~i + y~j + z
k, then
S
F · ~n dσ =
A. 0 B. 8 π C. 4 π D. − 4 π E. − 8 π
F (x, y, z) = cos z~i + sin z~j + xy
k, S is the complete boundary of the rectangular solid region bounded
by the planes x = 0, x = 1, y = 0, y = 1, z = 0 and z =
π
2
, and ~n is the outward unit normal on S, then
S
F · ~n dσ =
1
2
π
2
F (x, y, z) = x~i + y~j + z
k, S is the unit sphere x
2
2
2 = 1 and ~n is the outward unit normal on
S, then
S
F · ~n dσ =
A. − 4 π B.
2 π
3
4 π
3
E. 4 π
n→∞
n
n
A. 0 B. 1 C. − 1 D. 2 E. limit does not exist
n→∞
n
n +
n!
A. 0 B. 1 C. e D. 1/e E. limit does not exist
∞ ∑
n=
n+
n
, then s =
∞ ∑
n=
n
∞ ∑
n=
n
n
, then L =
∞ ∑
n=
(n
2
p
converges when
A. p > 1 B. p ≤ 1 C. p ≥ 1 D. p >
1
2
E. p ≤
1
2
∞ ∑
n=
n
p
converges for
A. p ≤ 1 B. p > 1 C. p < 0 D. p > 0 E. no values of p
(i)
∞ ∑
n=
n
n
2
(ii)
∞ ∑
n=
n
n
ln n
(iii)
∞ ∑
n=
n
n
e
n
A. only (ii) B. only (i) and (iii) C. only (i) and (ii) D. all three E. none of them
(i)
∞ ∑
n=
n
n
1
4
(ii)
∞ ∑
n=
n!
1 · 3 · 5 · · · (2n − 1)
(iii)
∞ ∑
n=
n
A. only (ii) B. only (i) and (iii) C. only (i) and (ii) D. all three E. none of them
∞ ∑
n=
n
x
n
n ln n
is
1
3
≤ x <
1
3
1
3
< x ≤
1
3
C. 0 ≤ x ≤
1
3
D. − 1 ≤ x ≤ 2 E. − 1 < x < 1
∞ ∑
n=
nx
n
n
1
2
< x <
1
2
B. − 2 < x < 2 C. − 2 ≤ x ≤ 2 D. − 2 < x ≤ 2 E. −∞ < x < ∞
x
2
x− 1
is
A. −x
3
B. 3x
3
C. − 3 x
3
D. − 4 x
3
E. 4x
3
2 ) sin x are
A. x −
5
6
x
3
31
150
x
5
B. 1 −
3
2
x
2
13
24
x
4
C. x −
7
6
x
3
31
150
x
5
D. x
2
−
7
6
x
3
1
25
x
5
E. x −
7
6
x
3
21
120
x
5