Vector Analysis: Homework 3 Solutions - Problem 0 and Problem 1, Assignments of Vector Analysis

The solutions to problems 0 and 1 of homework 3 in a math 550 vector analysis course. Problem 0 deals with the cross product of three vectors and the associated identity. Problem 1 involves the operation of a rotation matrix on a vector product. Both problems are solved using direct calculation and the triple product identity.

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MATH 550, VECTOR ANALYSIS, EXTRA
HOMEWORK 3 AND SOLUTIONS
Problem 0. Suppose a,b,cR3. Show that (a×b)×c=a(b·c)+b(a·c).
Solution: Let a=ha1,a
2
,a
3
i,b=hb
1
,b
2
,b
3
i,c=hc
1
,c
2
,c
3
i. Then
a×b=ha2b3a3b2,a
3
b
1a
1
b
3
,a
1
b
2a
2
b
1
i, and
(a×b)×c
=
(a3b1a1b3)c3(a1b2a2b1)c2
(a1b2a2b1)c1(a2b3a3b2)c3
(a2b3a3b2)c2(a3b1a1b3)c1
=
a1(b2c2+b3c3)+b
1
(a
2
c
2+a
3
c
3
)
a
2
(b
1
c
1+b
3
c
3
)+b
2
(a
1
c
1+a
3
c
3
)
a
3
(b
1
c
1+b
2
c
2
)+b
3
(a
1
c
1+a
2
c
2
)
=
a
1
(b
1
c
1+b
2
c
2+b
3
c
3
)+b
1
(a
1
c
1+a
2
c
2+a
3
c
3
)
a
2
(b
1
c
1+b
2
c
2+b
3
c
3
)+b
2
(a
1
c
1+a
2
c
2+a
3
c
3
)
a
3
(b
1
c
1+b
2
c
2+b
3
c
3
)+b
3
(a
1
c
1+a
2
c
2+a
3
c
3
)
=
a
1
a
2
a
3
(b
1
c
1+b
2
c
2+b
3
c
3
)+
b
1
b
2
b
3
(a
1
c
1+a
2
c
2+a
3
c
3
)
=a(b·c)+b(a·c).
Suppose ˆ
uis a unit vector in the abstract vector space V, and θR. For every vector
rin Vdefine:
R(θ, ˆ
u)r=rcos θ+ˆ
u(ˆ
u·r)(1 cos θ)+ˆ
u×rsin θ.
Suppose v,wV.
Problem 1. Show that [R(θ, ˆ
u)v]·[R(θ, ˆ
u)w]=v·w.
Solution: We use direct calculation:
R(θ, ˆ
u)v·R(θ, ˆ
u)w
=[vcos θ+ˆ
u(ˆ
u·v)(1cos θ)+ ˆ
u×vsin θ]·[wcos θ+ˆ
u(ˆ
u·w)(1 cos θ)+ˆ
u×wsin θ]
=v·wcos2θ+(
ˆ
u·v)(ˆ
u·w) cos θ(1 cos θ)+v·ˆ
u×wcos θsin θ
+(
ˆ
u·w)(ˆ
u·v) cos θ(1 cos θ)+(
ˆ
u·v)(ˆ
u·w)(1 cos θ)2
+ˆ
u·ˆ
u×w(ˆ
u·v)(1 cos θ) sin θ+ˆ
u×v·wcos θsin θ
+ˆ
u×v·ˆ
u(ˆ
u·w)(1 cos θ) sin θ+(
ˆ
u×v)·(
ˆ
u×w) sin2θ
Because ˆ
uis perpendicular to ˆ
u×vand ˆ
u×w, we have ˆ
u·ˆ
u×w=0and ˆ
u×v·ˆ
u=0.
Also by the triple product identity v·ˆ
u×w=ˆ
u×w·v=ˆ
u·w×v=ˆ
u·v×w, and
ˆ
u×v·w=ˆ
u·v×w. Hence the terms involving sin θcos θcancel out. Collecting terms a
bit we get:
R(θ, ˆ
u)v·R(θ, ˆ
u)w=v·wcos2θ+(
ˆ
u·v)(ˆ
u·w) sin2θ+(
ˆ
u×v)·(
ˆ
u×w) sin2θ
pf3

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Download Vector Analysis: Homework 3 Solutions - Problem 0 and Problem 1 and more Assignments Vector Analysis in PDF only on Docsity!

MATH 550, VECTOR ANALYSIS, EXTRA

HOMEWORK 3 AND SOLUTIONS

Problem 0. Suppose a, b, c ∈ R

3

. Show that (a × b) × c = −a(b · c) + b(a · c).

Solution: Let a = 〈a

1

, a

2

, a

3

〉, b = 〈b

1

, b

2

, b

3

〉, c = 〈c

1

, c

2

, c

3

〉. Then

a × b = 〈a 2

b

3

− a

3

b

2

, a

3

b

1

− a

1

b

3

, a

1

b

2

− a

2

b

1

〉, and

(a × b) × c

(a

3

b

1

− a

1

b

3

)c

3

− (a

1

b

2

− a

2

b

1

)c

2

(a

1

b

2

− a

2

b

1

)c

1

− (a

2

b

3

− a

3

b

2

)c

3

(a

2

b

3

− a

3

b

2

)c

2

− (a

3

b

1

− a

1

b

3

)c

1

−a

1

(b

2

c

2

  • b

3

c

3

) + b

1

(a

2

c

2

  • a

3

c

3

−a

2

(b

1

c

1

  • b

3

c

3

) + b

2

(a

1

c

1

  • a

3

c

3

−a

3

(b

1

c

1

  • b

2

c

2

) + b

3

(a

1

c

1

  • a

2

c

2

−a

1

(b

1

c

1

  • b

2

c

2

  • b

3

c

3

) + b

1

(a

1

c

1

  • a

2

c

2

  • a

3

c

3

−a

2

(b

1

c

1

  • b

2

c

2

  • b

3

c

3

) + b

2

(a

1

c

1

  • a

2

c

2

  • a

3

c

3

−a 3

(b 1

c 1

  • b 2

c 2

  • b 3

c 3

) + b 3

(a 1

c 1

  • a 2

c 2

  • a 3

c 3

a 1

a

2

a

3

(b

1

c

1

  • b

2

c

2

  • b

3

c

3

b 1

b

2

b

3

(a

1

c

1

  • a

2

c

2

  • a

3

c

3

= −a(b · c) + b(a · c).

Suppose ˆu is a unit vector in the abstract vector space V , and θ ∈ R. For every vector

r in V define:

R(θ,

u)r = r cos θ + ˆu(ˆu · r)(1 − cos θ) + ˆu × r sin θ.

Suppose v, w ∈ V.

Problem 1. Show that [R(θ, uˆ)v] · [R(θ, uˆ)w] = v · w.

Solution: We use direct calculation:

R(θ, uˆ)v · R(θ, uˆ)w

= [v cos θ + ˆu(ˆu · v)(1− cos θ) + ˆu × v sin θ] · [w cos θ + ˆu(ˆu · w)(1 − cos θ) + ˆu × w sin θ]

= v · w cos

2

θ + (ˆu · v)(ˆu · w) cos θ(1 − cos θ) + v · uˆ × w cos θ sin θ

  • (ˆu · w)(ˆu · v) cos θ(1 − cos θ) + (ˆu · v)(ˆu · w)(1 − cos θ)

2

  • ˆu · uˆ × w(ˆu · v)(1 − cos θ) sin θ + ˆu × v · w cos θ sin θ

  • ˆu × v · ˆu(ˆu · w)(1 − cos θ) sin θ + (ˆu × v) · (ˆu × w) sin

2

θ

Because ˆu is perpendicular to ˆu × v and ˆu × w, we have ˆu · uˆ × w = 0 and ˆu × v · uˆ = 0.

Also by the triple product identity v ·

u × w = ˆu × w · v = ˆu · w × v = −

u · v × w, and

uˆ × v · w = ˆu · v × w. Hence the terms involving sin θ cos θ cancel out. Collecting terms a

bit we get:

R(θ, uˆ)v · R(θ, uˆ)w = v · w cos

2

θ + (ˆu · v)(ˆu · w) sin

2

θ + (ˆu × v) · (ˆu × w) sin

2

θ

Using the triple product identity and problem 0 we get

(ˆu × v) · (ˆu × w) = [(ˆu × v) ×

u] · w = [−

u(v ·

u) + v(ˆu ·

u)] · w = v · w − (ˆu · v)(ˆu · w).

Substituting this into the previous expression we get

R(θ, uˆ)v · R(θ, uˆ)w = v · w(cos

2

θ + sin

2

θ) = v · w.

Using problem 0 we can show the following Jacobi identity holds:

(a × b) × c + (c × a) × b + (b × c) × a = 0. To see this we compute:

(a × b) × c = −a(b · c) + b(a · c)

(c × a) × b = −c(a · b) + a(c · b)

(b × c) × a = −b(c · a) + c(b · a).

Adding both sides we clearly get a zero vector on the right-hand-side.

Problem 2. Show that R(θ, uˆ)(v × w) = [R(θ, uˆ)v] × [R(θ, uˆ)w].

Solution: As before we directly calculate:

R(θ, uˆ)v × R(θ, uˆ)w

= [v cos θ + ˆu(ˆu · v)(1− cos θ) + ˆu × v sin θ]×[w cos θ + ˆu(ˆu · w)(1− cos θ) + ˆu × w sin θ]

= v × w cos

2

θ + (v × uˆ)(ˆu · w) cos θ(1 − cos θ) + v × (ˆu × w) cos θ sin θ

  • (ˆu × w)(ˆu · v) cos θ(1 − cos θ) + ˆu × ˆu(ˆu · v)(ˆu · w)(1 − cos θ)

2

  • ˆu × (ˆu × w)(ˆu · v)(1 − cos θ) sin θ + (ˆu × v) × w cos θ sin θ

  • (ˆu × v) × uˆ(ˆu · w)(1 − cos θ) sin θ + (ˆu × v) × (ˆu × w) sin

2

θ

= [v × w − (v × uˆ)(ˆu · w) − (ˆu × w)(ˆu · v)] cos

2

θ + (ˆu × v) × (ˆu × w) sin

2

θ

  • [v × (ˆu × w) − uˆ × (ˆu × w)(ˆu · v) + (ˆu × v) × w − (ˆu × v) × uˆ(ˆu · w)] cos θ sin θ

  • [(v × uˆ)(ˆu · w) + (ˆu × w)(ˆu · v)] cos θ

  • [ˆu × (ˆu × w)(ˆu · v) + (ˆu × v) × uˆ(ˆu · w)] sin θ

We must work on each of these terms. The first term is (using problem 0):

v × w − (v × uˆ)(ˆu · w) − (ˆu × w)(ˆu · v) = v × w + [−v(w · ˆu) + w(v · uˆ)] × ˆu

= v × w + [(v × w) × ˆu] × uˆ

= v × w − (v × w)(ˆu · ˆu) + ˆu[(v × w) · uˆ]

= ˆu[ˆu · (v × w)].

The second term is (using problem 0 and the triple product identity):

(ˆu × v) × (ˆu × w) = −uˆ[v · (ˆu × w)] + v[ˆu · (ˆu × w)] = ˆu[v · (w × uˆ)] = ˆu[(v × w) · ˆu]

= ˆu[ˆu · (v × w)].