Solutions to Final Exam Problems in Vector Calculus, Exams of Calculus

The solutions to problems on vector calculus, including finding vector differences, unit vectors, projections, identifying and sketching surfaces, using the chain rule, and applying the lagrange multiplier method. It also includes problems on spherical coordinates and conservative vector fields.

Typology: Exams

Pre 2010

Uploaded on 08/19/2009

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Final Exam: Solutions
Problem 1. Given vectors u= (1,0,2), v= (2,1,3), and w=
(2,1,0), find
(a) the vector uv;
(b) the unit vector in the direction of w;
(c) the projection of uvonto the direction of w.
Solution. (a) uv= (1 2,0(1),23) = (1,1,1).
(b) kwk=p(2)2+ 12+ 02=5. The unit vector in the direction
of wis w
kwk=2
5,1
5,0.
(c) the projection of uvonto the direction of wis
(uv)·w
kwk= (1,1,1)·2
5,1
5,0=1·2
5+1·1
5+(1)·0 = 3
5.
Problem 2. Identify and sketch the following surfaces:
(a) 2x2+y2z2= 0;
(b) x2=z;
(c) x2+ 2y2+z24y= 0.
Solution. (a) 2x2+y2z2= 0 is equivalent to z2= 2x2+y2, i.e.,
z2=x2
(1/2)2+y2, which is an equation of an elliptic cone.
(b) x2=zis an equation of a parabolic cylinder.
(c) x2+2y2+z24y= 0 is equivalent to x2+2(y22y+ 1) + z2= 2,
i.e., x2
(2)2+ (y1)2+z2
(2)2= 1, which is an equation of an ellipsoid
centered at (0,1,0).
Problem 3. Use an appropriate form of the chain rule to find
(a) dz
dt , where z= 5x2y,x=t3,y=t2;
(b) ∂ω
∂u and ∂ω
∂v , where ω= 4xy+ 2z,x=usin v,y=vsin u,
z= sin usin v.
Solution. (a) dz
dt =∂z
∂x
dx
dt +∂z
∂y
dy
dt , thus
dz
dt = 10xy·3t2+5x2·2t= 10·t3·t2·3t2+5 ·(t3)2·2t= 30t7+10t7= 40t7.
(b) ∂ω
∂u =∂ω
∂x
∂x
∂u +∂ω
∂y
∂y
∂u , thus
∂ω
∂u = 4 sin vvcos u+ 2 cos usin v.
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Final Exam: Solutions

Problem 1. Given vectors u = (1, 0 , 2), v = (2, − 1 , 3), and w = (− 2 , 1 , 0), find (a) the vector u − v; (b) the unit vector in the direction of w; (c) the projection of u − v onto the direction of w.

Solution. (a) u − v = (1 − 2 , 0 − (−1), 2 − 3) = (− 1 , 1 , −1). (b) ‖w‖ =

(−2)^2 + 1^2 + 0^2 =

  1. The unit vector in the direction

of w is (^) ‖ww‖ =

−√ 2 5 ,^ √^1 5 ,^0

(c) the projection of u − v onto the direction of w is

(u−v)·

w ‖w‖

Problem 2. Identify and sketch the following surfaces: (a) 2x^2 + y^2 − z^2 = 0; (b) x^2 = z; (c) x^2 + 2y^2 + z^2 − 4 y = 0.

Solution. (a) 2x^2 + y^2 − z^2 = 0 is equivalent to z^2 = 2x^2 + y^2 , i.e., z^2 = x 2 (1/√2)^2 +^ y

(^2) , which is an equation of an elliptic cone.

(b) x^2 = z is an equation of a parabolic cylinder. (c) x^2 + 2y^2 + z^2 − 4 y = 0 is equivalent to x^2 + 2(y^2 − 2 y + 1) + z^2 = 2, i.e., x

2 ( √ 2)^2 + (y^ −^ 1)

(^2) + z^2 ( √ 2)^2 = 1, which is an equation of an ellipsoid centered at (0, 1 , 0).

Problem 3. Use an appropriate form of the chain rule to find (a) dzdt , where z = 5x^2 y, x = t^3 , y = t^2 ; (b) ∂ω∂u and ∂ω∂v , where ω = 4x − y + 2z, x = u sin v, y = v sin u, z = sin u sin v.

Solution. (a) dzdt = ∂z∂xdxdt + ∂z∂ydydt , thus

dz dt

= 10xy · 3 t^2 +5x^2 · 2 t = 10·t^3 ·t^2 · 3 t^2 +5·(t^3 )^2 · 2 t = 30t^7 +10t^7 = 40t^7.

(b) ∂ω∂u = ∂ω∂x∂x∂u + ∂ω∂y∂u∂y , thus

∂ω ∂u

= 4 sin v − v cos u + 2 cos u sin v. 1

∂ω ∂v =^

∂ω ∂x

∂x ∂v +^

∂ω ∂y

∂y ∂v , thus

∂ω ∂v

= 4u cos v − sin u + 2 sin u cos v.

Problem 4. Use the Lagrange multiplier method to find the maxi- mum sum of x^2 + y^2 + z^2 if x + 2y + 2z = 12.

Solution. The problem can be formulated as follows: find the maximum value of f (x, y, z) = x^2 + y^2 + z^2 under the constraint g(x, y, z) = x + 2y + 2z − 12 = 0. The Lagrange (vector) equation ∇f = λ∇g is equivalent to the three scalar equations

fx = λgx, fy = λgy, fz = λgz ,

i.e.,

2 x = λ · 1 , 2 y = λ · 2 , 2 z = λ · 2.

Eliminating λ, we get 2x = y = z. Using the constraint equation we get x + 2 · 2 x + 2 · 2 x − 12 = 0, i.e., 9x = 12. Therefore, x = 129 = 43 , y = z = 2 · 43 = 83. The maximum value of f (x, y, z) = x^2 + y^2 + z^2 is, therefore,

( 4 3

Problem 5. Use spherical coordinates to find the mass of the solid bounded below by the cone z =

x^2 + y^2 and above by the sphere x^2 + y^2 + z^2 = 9 if its density is given by δ(x, y, z) = x^2 + y^2 + z^2.

Solution. The solid has a shape of “ice-cream cone”. It can be de- scribed in spherical coordinates by the inequalities 0 ≤ θ ≤ 2 π (because it is axial symmetric about the z-axis), 0 ≤ φ ≤ π 4 (because the conic surface has an equation φ = π 4 in spherical coordinates), and 0 ≤ ρ ≤ 3 (because the radius of a spherical cap is 3). Since x^2 + y^2 + z^2 = ρ^2 , the density function in spherical coordinates is δ(ρ, φ, θ) = ρ^2. Therefore,

is

W =

∫ Q(1,1)

P (0,1)

F · dr =

0

F(x(t), y(t)) · r′(t) dt

0

(f (x(t), y(t))x′(t) + g(x(t), y(t))y′(t)) dt =

0

t^2 + 1

t t^2 + 1

dt

0

t^2 + 1

dt = − tan−^1 (t)

∣^1

0

= − tan−^1 (1) = −

π 4