a1-sol
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AMath 231 ASSIGNMENT # 1 Solutions: Review [15 Total] Fall 2014
Due Monday, September 15, 2014 at 2pm in box 7, slot 11 (A-M) and 12 (N-Z), locatedacross from MC4066. Late assignments or assignments submitted to the incorrect dropboxwill receive a grade of zero. Write your solutions clearly and concisely. Marks will bededucted for poor presentation and incorrect notation.
1. Evaluate
x7
1 + x2 dx. [0 marks]
Solution: We substitute u = x2 and du = 2xdx to rewrite this asx7
1 + x2 dx =
u3
1 + u du.
Next substitute v = 1 + u, expand then integrate,u3
1 + u du =
(1 v)3v dv,
=
(1 3v + 3v2 v3)v dv,
=
[2
3v3/2 6
5v5/2 +
6
7v7/2 2
9v9/2)
]+ c
=
[2
3[(1 + x2)3/2 6
5(1 + x2)5/2 +
6
7(1 + x2)7/2 2
9(1 + x2)9/2)
]+ c.
2. Evaluate
sin(log x) dx. [0 marks]
Solution:
Substitute u = log x and du = dx/x or eudu = dxsin(log x) dx =
eu sin(u) du.
There are several ways to integrate this. The standard way you would have learned inAMATH 250. A more clever way is to use Eulers formula realize that the above is theimaginary part of the following, which is easier to evaluate
Imag
[e(1+i)u du
]= Imag
[1
1 + ie(1+i)u
]+ c,
= Imag
[1 i
2e(1+i)u
]+ c,
=1
2eu [sinu cosu] + c,
=1
2x [sin log x cos log x] + c.
1
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yx
2
0
Rx2 + (y 1)2 = 1
Figure 1: Region R.
3. Evaluate
(log x)2 dx. [3 marks]
Solution:
Substute u = log x and du = dx/x or eudu = dx(log x)2 dx =
euu2 du.
This we integrate by parts twice,u2eu du = u2eu 2
ueu du,
= u2eu 2ueu + 2eu du,
= u2eu 2ueu + 2eu,= x
((log x)2 2 log x+ 2) .
4. Evaluate
R
(9 x2 y2)dA where R is the region x2 + (y 1)2 1. [4 marks]
Solution:
The region of integration is depicted in Figure 1, which is a circle of radius 1 centredat (0, 1) and hence suggests that a transformation into polar coordinates is an idealchoice for integration. Let x = r cos() and y = r sin(). In polar coordinates theregion R is bounded by
(r cos())2 + (r sin() 1)2 = 1 r(r 2 sin()) = 0.
Either r = 0, which is not a possible choice, or r = 2 sin(). It follows to generate theregion R that r = 2 sin() for from 0 to pi. Furthermore, dA = rdrd (this is from
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the Jacobian; convince yourself by trying it out as an exercise). Therefore,R
(9 x2 y2)dA =
pi0
2 sin()0
(9 r2)rdrd
=
pi0
(9
2r2 1
4r4) 2 sin()
0
d
=
pi0
(18 sin2() 4 sin4()) d
=
pi0
(18
2(1 cos(2)) 4
4(1 cos(2))2
)d
= 9( 12
sin(2))
pi0
pi0
(1 2 cos(2) + cos2(2))d
= 9pi pi0
(1 2 cos(2) + cos(4) + 1
2
)d
= 9pi ( sin(2) + sin(4)
8+
2
) pi0
= 9pi pi pi2
=15pi
2
where we have applied the double angle formula
cos2() =cos(2) + 1
2and sin2() =
1 cos(2)2
to aid in the integration.
5. Evaluate
G
xyzdV where G is the solid in the first octant bounded by the sphere
x2 + y2 + z2 = 4 and the coordinate planes. [0 marks]Solution:
The region of integration, G, is a sphere constrained to x 0, y 0, z 0, x2 + y2 +z2 22 (see Figure 2). Apply spherical coordinates,
x = r sin() cos()
y = r sin() sin()
z = r cos().
For the first octant, we must have r 2, 0 pi/2 and 0 pi/2. Furthermore,dV = r2 sin()drdd (this is from the Jacobian; convince yourself by trying it out as
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zy
x
Figure 2: Region G.
an exercise). Therefore, G
xyzdV =
pi2
0
pi2
0
20
(r sin() cos()
)(r sin() sin()
)(r cos()
)r2 sin()drdd
=
20
r5dr
pi2
0
sin3() cos()d
pi2
0
sin() cos()d
=1
6r620
pi2
0
sin3() cos()d
pi2
0
sin() cos()d
=26
6
10
u3du
10
wdw, (where u = sin(), w = sin())
=26
6
u4
4
10
1
2w210
=4
3.
6. The angular momentum of a particle of mass m with position vector r is
H = r (mu).
Let u = r. Using the result
a (b c) = (a c) b (a b) c,
show that H = mr2 when r is perpendicular to . Here r2 = r r. [2 marks]
Solution:
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We begin by computing H:
H = r (mu),= mr ( r),= m(r r) (r ) r= mr2 ,
as we expected.
7. (a) Solve the differential equationdy
dx= y
x. [0 marks]
Solution: The differential equation is separable and hence through integrationwe get
1
ydy =
1
xdx,
log y = log x+ c,
Solving leads to
xy = constant.
Therefore, xy = c where c is a constant.
(b) Find the solution to (a) that passes through the point (1, 2). [0 mark]Solution: Substituting y(1) = 2 into the solution in (a), we obtain 2 = c andhence c = 2. Therefore, xy = 2.
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