Practice Midterm 2 Solutions - Multivariable Calculus | MATH 53, Study notes of Calculus

Practice Midterm 1 Solution Material Type: Notes; Professor: Auroux; Class: Multivariable Calculus; Subject: Mathematics; University: University of California - Berkeley; Term: Fall 2010;

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Pre 2010

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Math 53 Practice Midterm 2 A Solutions
1. a) The area of the triangle is 2, so ¯y=1
2Z1
0Z22y
2y2
y dxdy.
b) By symmetry ¯x= 0.
2. ρ=|x|=r|cos θ|. Using symmetry, I0=ZZD
r2ρ rdrdθ =
Z2π
0Z1
0
r2|rcos θ|rdrdθ = 4Zπ /2
0Z1
0
r4cos θdrdθ = 4Zπ /2
0
1
5cos θdθ =4
5.
3. x=x,y=x2, 0 x1: so ZC
yx3dx +y2dy =Z1
0
x2x3dx + (x2)2(2xdx) = Z1
0
3x5dx =1
2.
4. a) Qx= 6x2+by2,Py=ax2+ 3y2.Qx=Pyprovided a= 6 and b= 3.
b) fx= 6x2y+y3+ 1 f= 2x3y+xy3+x+g(y). Therefore, fy= 2x3+ 3xy2+g(y).
Comparing this with Q, we get 2x3+ 3xy2+g(y) = 2x3+ 3xy2+ 2 so g(y) = 2 and g= 2y+c. So
f= 2x3y+xy3+x+ 2y(+constant).
c) Cstarts at (1,0) and ends at (eπ,0), so ZC
~
F·d~r =f(eπ,0) f(1,0) = eπ1.
5. a) ¯
¯
¯
¯
uxuy
vxvy¯
¯
¯
¯
=¯
¯
¯
¯
2x/y x2/y2
y x ¯
¯
¯
¯
= 3x2/y. Therefore, dudv =|3x2/y|dxdy = 3|u|dxdy
and hence dx dy =1
3|u|du dv.
b) ZZR
dx dy =Z4
2Z5
1
1
3ududv =Z4
2
1
3ln 5 dv =2
3ln 5.
6. a) IC
Mdx =ZZR
MydA. (Green’s theorem)
b) We want Msuch that My= (x+y)2. We can use e.g. M=1
3(x+y)3.
7. a) div ~
F= 2y, so IC
~
F·ˆ
nds =ZZR
2y dA =Z1
0Zx3
0
2y dydx =Z1
0
x6dx =1
7.
b) For the flux through C1,ˆ
n=ˆ
implies ~
F·ˆ
n=(1 + y2) = 1 where y= 0. The length
of C1is 1, so the total flux through C1is RC1(1) ds =1. The flux through C2is zero because
ˆ
n=ˆ
ıand ~
Fˆ
ı.
c) ZC3
~
F·ˆ
nds =ZC1+C2+C3
~
F·ˆ
nds ZC1
~
F·ˆ
nds ZC2
~
F·ˆ
nds =1
7(1) 0 = 8
7.
8.
¡
¡
¡
¡
¡
1
1
Zπ/2
0Z1
0Z1
0
r2r dz dr .
1
pf2

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Math 53 Practice Midterm 2 A – Solutions

  1. a) The area of the triangle is 2, so ¯y =

1

0

2 − 2 y

2 y− 2

y dxdy.

b) By symmetry ¯x = 0.

  1. ρ = |x| = r| cos θ|. Using symmetry, I 0

D

r

2 ρ rdrdθ =

2 π

0

1

0

r

2 |r cos θ|rdrdθ = 4

π/ 2

0

1

0

r

4 cos θdrdθ = 4

π/ 2

0

cos θdθ =

  1. x = x, y = x

2 , 0 ≤ x ≤ 1: so

C

yx

3 dx + y

2 dy =

1

0

x

2 x

3 dx + (x

2 )

2 (2xdx) =

1

0

3 x

5 dx =

  1. a) Qx = 6x

2

  • by

2 , Py = ax

2

  • 3y

2

. Qx = Py provided a = 6 and b = 3.

b) fx = 6x

2 y + y

3

  • 1 ⇒ f = 2x

3 y + xy

3

  • x + g(y). Therefore, fy = 2x

3

  • 3xy

2

  • g

′ (y).

Comparing this with Q, we get 2x

3

  • 3xy

2

  • g

′ (y) = 2x

3

  • 3xy

2

  • 2 so g

′ (y) = 2 and g = 2y + c. So

f = 2x

3

y + xy

3

  • x + 2y (+constant).

c) C starts at (1, 0) and ends at (−e

π , 0), so

C

F · d~r = f (−e

π , 0) − f (1, 0) = −e

−π − 1.

  1. a)

u x

u y

vx vy

2 x/y −x

2 /y

2

y x

= 3x

2

/y. Therefore, dudv = | 3 x

2 /y| dxdy = 3|u| dxdy

and hence dx dy =

3 |u|

du dv.

b)

R

dx dy =

4

2

5

1

3 u

dudv =

4

2

ln 5 dv =

ln 5.

  1. a)

C

M dx =

R

−My dA. (Green’s theorem)

b) We want M such that −M y

= (x + y)

2

. We can use e.g. M = −

(x + y)

3 .

  1. a) div

F = 2y, so

C

F · nˆ ds =

R

2 y dA =

1

0

x

3

0

2 y dydx =

1

0

x

6

dx =

b) For the flux through C 1 , ˆn = −ˆ implies

F · nˆ = −(1 + y

2 ) = −1 where y = 0. The length

of C 1

is 1, so the total flux through C 1

is

C 1

(−1) ds = −1. The flux through C 2

is zero because

nˆ = ˆı and

F ⊥ ˆı.

c)

C 3

F · ˆn ds =

C 1 +C 2 +C 3

F · nˆ ds −

C 1

F · nˆ ds −

C 2

F · nˆ ds =

¡

¡ ¡

¡ ¡

1

1

π/ 2

0

1

0

1

0

r

2 r dz dr dθ.

¡

¡

a) sphere: ρ = 2a cos φ. b) plane: ρ = a sec φ.

c)

2 π

0

π/ 4

0

2 a cos φ

a sec φ

ρ

2

sin φ dρ dφ dθ.

  1. a)

∂y

(2xy + z

3 ) = 2x =

∂x

(x

2

  • 2yz);

∂z

(2xy + z

3 ) = 3z

2

∂x

(y

2

  • 3xz

2 − 1);

∂z

(x

2

  • 2yz) = 2y =

∂y

(y

2

  • 3xz

2 − 1); so

F is conservative.

b)

∂f

∂x

= 2xy + z

3 , so f (x, y, z) = x

2 y + xz

3

  • g(y, z).

∂f

∂y

= x

2

∂g

∂y

= x

2

  • 2yz, so

∂g

∂y

= 2yz.

Therefore g(y, z) = y

2 z + h(z), and f (x, y, z) = x

2 y + xz

3

  • y

2 z + h(z).

∂f

∂z

= 3xz

2

  • y

2

  • h

′ (z) = y

2

  • 3xz

2 − 1, so h

′ (z) = −1.

Therefore h(z) = −z + c, and f (x, y, z) = x

2 y + xz

3

  • y

2 z − z + c.

  1. S is the graph of z = f (x, y) = 1 − x

2 − y

2 , so ˆn dS = 〈−f x

, −f y

, 1 〉 dx dy = 〈 2 x, 2 y, 1 〉 dx dy.

Therefore

S

F · nˆ dS =

S

〈x, y, 2(1 − z)〉 · 〈 2 x, 2 y, 1 〉 dx dy =

S

2 x

2

  • 2y

2

  • 2(1 − z) dx dy = ∫∫

S

4 x

2

  • 4y

2 dx dy (since z = 1 − x

2 − y

2 ).

Shadow = unit disc x

2

  • y

2 ≤ 1; switching to polar coordinates, we have

S

F · nˆ dS =

2 π

0

1

0

4 r

2 r dr dθ =

2 π

0

[

r

4

]

1

0

dθ = 2π.