Calculus III: Practice Final, Study notes of Calculus

The exam contains 10 problems. • The last page is the formula sheet, which you may detach. • Good luck! ... by the Fundamental Theorem of Calculus.

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Calculus III: Practice Final
Name:
Circle one: Section 6 Section 7 .
Read the problems carefully.
Show your work unless asked otherwise.
Partial credit will be given for incomplete work.
The exam contains 10 problems.
The last page is the formula sheet, which you may detach.
Good luck!
Question: 1 2 3 4 5 6 7 8 9 10 Total
Points: 10 10 10 10 10 10 10 10 10 10 100
Score:
1
pf3
pf4
pf5
pf8
pf9
pfa

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Calculus III: Practice Final

Name:

Circle one: Section 6 Section 7.

  • Read the problems carefully.
  • Show your work unless asked otherwise.
  • Partial credit will be given for incomplete work.
  • The exam contains 10 problems.
  • The last page is the formula sheet, which you may detach.
  • Good luck!

Question: 1 2 3 4 5 6 7 8 9 10 Total Points: 10 10 10 10 10 10 10 10 10 10 100 Score:

  1. (10 points) Circle True or False. No justifation is needed.

(a) The curve traced by 〈cos^2 (t), sin^2 (t)〉 is a circle. True False

Solution: False.

(b) The plane 3x + 2y − z = 0 is perpendicular to the line x = 3t, y = 2t, z = −t. True False

Solution: True.

(c) The function f (x, y, z) =

{sin(x+y+z) x+y+z if^ x^ +^ y^ +^ z^6 = 0 1 if x + y + z = 0 is continuous at (0, 0 , 0). True False

Solution: True.

(d) If the acceleration is constant, then the trajectory must be a straight line. True False

Solution: False.

(e) The complex number e2+3i^ has magnitude 2. True False

Solution: False.

  1. Use the contour plot of f (x, y) to answer the questions. No justification is needed.

A

B

C

D

E

(a) (3 points) Mark any three critical points of f. Label them A, B, and C. Identify whether they are local minima, local maxima or saddle points.

Solution: A: Saddle; B, D: Local maxima, C, E: Local minima.

(b) (2 points) Draw a vector at (1, 1) indicating the direction of ∇f at (1, 1). (c) (3 points) Determine the sign of

  1. ∂f∂x (3, 4): Positve.
  2. ∂f∂y (2, 3): Negative.
  3. Duf (5, 3) where u is the South–East direction: Negative. (d) (2 points) Give a (admittedly rough) numerical estimate of ∂f∂x (1, 1).

Solution: ∂f /∂x(1, 1) ≈ 0. 2 / 0 .2 = 1. 0

  1. (a) (5 points) Write parametric equations for the tangent line at 〈 1 , 0 , 1 〉 to the curve traced by 〈t^2 , ln t, t^3 〉.

Solution: Let r(t) = 〈t^2 , ln t, t^3 〉. Then r(1) = 〈 1 , 0 , 1 〉.

r′(t) = 〈 2 t, 1 /t, 3 t^2 〉 r′(1) = 〈 2 , 1 , 3 〉.

The tangent line is the line through 〈 1 , 0 , 1 〉 in the direction of 〈 2 , 1 , 3 〉, that is:

(x, y, z) = 〈 1 , 0 , 1 〉 + t〈 2 , 1 , 3 〉.

In other words, x = 1 + 2t, y = t, z = 1 + 3t.

(b) (5 points) Write an equation of the normal plane to the curve at the same point.

Solution: The normal plane is the plane through 〈 1 , 0 , 1 〉 perpendicular to r′(1) = 〈 2 , 1 , 3 〉. The equation is

〈x − 1 , y, z − 1 〉 · 〈 2 , 1 , 3 〉 = 0 =⇒ 2(x − 1) + y + 3(z − 1) = 0 =⇒ 2 x + y + 3z = 5.

  1. A ball of unit mass is thrown with the initial velocity of i + j. It experiences the force of gravity of magnitude 10 units in the −j direction and a force due to the wind of magnitude 1 unit in the i direction. Suppose the ball is initially at (0, 4). (a) (7 points) Find the position of the ball at time t.

Solution: We have

Acceleration −→a = i − 10 j Therefore, velocity −→v (t) =

−→a dt

= ti − 10 tj + −→c.

Since −→v (0) = i + j, we get −→c = i + j. Therefore −→v (t) = (1 + t)i + (1 − 10 t)j

Therefore, position −→r (t) =

−→v (t) dt

t + t

2 2

i + (t − 5 t^2 )j + −→c.

Since −→r (0) = 4j, we get −→c = 4j. Therefore,

−→r (t) =

t + t

2 2

i + (4 + t − 5 t^2 )j.

In other words, at time t, the ball is at x = t + t^2 /2 and y = 4 + t − 5 t^2.

(b) (3 points) Where is the ball when it hits the ground?

Solution: The ball hits the ground when y = 0. That is

4 + t − 5 t^2 = 0 5 t^2 − t − 4 = (5t + 4)(t − 1) = 0.

The only positive solution is t = 1. So the ball hits the ground at t = 1. At this point, it is at x = 1 + 1/2 = 3/2 and y = 0.

  1. Suppose u = exy^ where x = st + s + t and y = st − s − t.

(a) (2 points) Find the value of u when s = 2 and t = 2.

Solution: Then x = 8 and y = 0, so that exy^ = e^0 = 1.

(b) (8 points) Find an approximate numerical value of u when s = 2.01 and t = 1.98.

Solution: We know that

∆u ≈ ∂u∂s ∆s + ∂u∂t ∆t.

By the chain rule, ∂u ∂s =^

∂u ∂x ·^

∂x ∂s +^

∂u ∂y ·^

∂y ∂s = yexy(t + 1) + xexy(t − 1) = 8 at s = 2, t = 2.

Likewise, ∂u ∂t

= ∂u ∂x

· ∂x ∂t

  • ∂u ∂y

· ∂y ∂t = yexy(s + 1) + xexy(s − 1) = 8 at s = 2, t = 2.

Hence

∆u ≈ 8 · 0 .01 + 8 · (− 0 .02) = − 0. 08.

In other words, u ≈ 1 − 0 .08 = 0.92. (By the way, the exact answer is u = 0. 92192448707... .)

  1. (10 points) A race track is in the shape of an ellipse with minor radius 1 km and ma- jor radius 2 km as shown. A car is going along this track at a constant speed of 100 km/h. Find the tangent and normal com- ponent of its accelaration when it as at P.

Race track

P

Solution: Let r(t) be the position of the car at time t. We know that at time t, the tangent and normal components of accelaration are given by

aT = |r′(t)|′^ and aN = κ|r′(t)|^2 ,

where κ is the curvature of the trajectory at the point r(t). Since the speed |r′(t)| is constant, we immediately get that

aT = 0.

What remains is aN = κ|r′(t)|^2 = 100^2 κ. To get the answer, we must compute the curvature of the ellipse at the point P. To compute the curvature, we first conveniently parametrize the ellipse. For example,

x = 2 cos t, y = sin t.

Then

κ = |〈−2 sin^ t,^ cos^ t〉 × 〈−2 cos^ t,^ −^ sin^ t〉| |〈−2 sin t, cos t〉|^3 = |(2 sin

(^2) t + 2 cos (^2) t)k| (4 sin^2 t + cos^2 t)^3 /^2 = 2 (4 sin^2 t + cos^2 t)^3 /^2 = 2 at P (set t = 0).

Therefore, aN = 2 · 1002 = 20000 km/h^2.

  1. (10 points) You want to design a cylindrical cup that can hold 100π ml coffee. To minimize the material to be used, you decide to minimize the surface area. What is the radius and height of the optimal cup? (Ignore the thickness of the walls.)

Solution: Let the radius of the cup be r and the height h. We want

Volume = πr^2 h = 100π, that is r^2 h = 100.

We want to minimize

Surface area = πr^2 (bottom) + 2πrh(side) = π(r^2 + 2rh).

So, we want to minimize f (r, h) = r^2 + 2rh subject to g(r, h) = r^2 h = 100. By the method of Lagrange multipliers, the extremal values are attained when

∇f = λ∇g.

We have ∇f = 〈 2 r + 2h, 2 r〉, ∇g = 〈 2 rh, r^2 〉. These two are multiples of each other when 2 r + 2h 2 rh =

2 r r^2. Simplifying and cross-multiplying gives

r + h = 2h =⇒ r = h.

So the only critical point is when r = h. To find this value, we use the constraint

r^2 h = 100.

This gives r = h = 100^1 /^3. (By the way, r = h would result in a very bizarre coffee cup!)