Sample Problems from Boas - Elementary Math Physics | PHYS 227, Study notes of Physics

Material Type: Notes; Professor: Ellis; Class: ELEM MATH PHYS; Subject: Physics; University: University of Washington - Seattle; Term: Autumn 2007;

Typology: Study notes

Pre 2010

Uploaded on 03/10/2009

koofers-user-9nc-1
koofers-user-9nc-1 🇺🇸

10 documents

1 / 7

Toggle sidebar

This page cannot be seen from the preview

Don't miss anything!

bg1
Physics 227 Lecture 7 Appendix B 1 Autumn 2007
Lecture 7 Appendix B: Some sample problems from Boas
Here are some solutions to the sample problems assigned for Chapter 3 (Sections 3, 6,
7 and 9).
§3.3: 5
Solution: We want to find the determinant of a 5x5 matrix by first simplifying the
matrix, using the general invariances of determinants (e.g., adding and subtracting
rows), and then use the Laplace development. We have
3 3 4 4 4 2 1
5 5 5 1
7 0 1 3 5 7 0 1 3 5
2 1 0 1 4 2 1 0 1 4
7 3 2 1 4 15 3 0 8 8
8 6 2 7 4 8 6 2 7 4
1 3 5 7 5 1 3 5 7 5
7 0 1 3 5 7 0 1 3 5
2 1 0 1 4 2 1 0 1 4
15 3 0 8 8 15 3 0 8 8
22 6 0 13 14 22 6 0 13 14
1 3 5 7 5 36 3 0 8 30
2 1 1 4
15 3 8 8
122 6 13 14
36
R R R R R R
R R R
 

2 2 8 1
3 3 13 1
4 4 8 1
3 3 1
2 1 1 4
31 5 0 40
48 7 0 66
3 8 30 52 5 0 62
31 5 40 31 5 40
48 66 31 40
1 48 7 66 48 7 66 5 7
21 22 21 22
52 5 62 21 0 22
R R R
R R R
R R R
R R R


5 1056 1386 7 682 840 1650 1106 544.
§3.3: 17
Solution: Here we apply Cramer’s rule to the equations described the Lorentz
transformation of Special Relativity to find the inverse transformation. We have
pf3
pf4
pf5

Partial preview of the text

Download Sample Problems from Boas - Elementary Math Physics | PHYS 227 and more Study notes Physics in PDF only on Docsity!

Lecture 7 – Appendix B: Some sample problems from Boas

Here are some solutions to the sample problems assigned for Chapter 3 (Sections 3, 6,

7 and 9 ).

§3.3: 5

Solution: We want to find the determinant of a 5x5 matrix by first simplifying the

matrix, using the general invariances of determinants ( e.g ., adding and subtracting

rows), and then use the Laplace development. We have

3 3 4 4 4 2 1

5 5 5 1

7 0 1 3 5 7 0 1 3 5

2 1 0 1 4 2 1 0 1 4

7 3 2 1 4 15 3 0 8 8

8 6 2 7 4 8 6 2 7 4

1 3 5 7 5 1 3 5 7 5

7 0 1 3 5 7 0 1 3 5

2 1 0 1 4 2 1 0 1 4

15 3 0 8 8 15 3 0 8 8

22 6 0 13 14 22 6 0 13 14

1 3 5 7 5 36 3 0 8 30

2 1 1 4

15 3 8 8

1

22 6 13 14

36

R R R R R R

R R R

   

 

 

 

  ^  

   

 

 

 

  

 

 

2 2 8 1

3 3 13 1

4 4 8 1

3 3 1

2 1 1 4

31 5 0 40

48 7 0 66

3 8 30 52 5 0 62

31 5 40 31 5 40

48 66 31 40

1 48 7 66 48 7 66 5 7

21 22 21 22

52 5 62 21 0 22

R R R

R R R

R R R

R R R

 

 

 

 



 

 

     

§3.3: 17

Solution: Here we apply Cramer’s rule to the equations described the Lorentz

transformation of Special Relativity to find the inverse transformation. We have

2 2

2 2 2

2

2 2

2

2 2 2

2

x x vt v x x

t t vx c^ v^ c^ t^ t

x v

t^ x^ vt

x x vt

v v c

v c

x

t vx c v c t

t t vx c

v v c

v c

 ^ 

 ^  

   ^  

It should no surprise that the form of the transformation is what we would obtain by

boosting in the opposite direction, v   v.

§3.6: 2

Solution: Here we practice finding various combinations of 2 matrices. We find

2

A B AB

BA

A B

A B

A

 ^   ^   ^ ^ ^   ^  

 ^ ^ ^    

 ^  

   ^ ^ ^    

 

   

 

   

2

2

det 5 150 125 25 5det 5,

det 5 5 det 25 1 25;

det 3 18 0 18 3det 6

det 3 3 det 9 2 18.

A A

A A

B B

B B

Thus n = 2 as expected for 2x2 matrices. The Mathematica version of most of these

steps can be found on the web page.

§3.6: 22

Solution: Now we use matrices to solve a set of simultaneous equations. We have in

standard matrix notation

x y z x

x y z y

x y z z

So now we work out the inverse of the coefficient matrix using our new technology.

The pieces are

      

1

1 1 1

det 2 1 1 1 2 2 1 4 3 1 4 3 4 7 1 12,

3 2 2

4 7 1 4 4 0 4 4 0

1

4 1 5 , 7 1 3 7 1 3.

12

0 3 3 1 5 3 1 5 3

T

M

C C M

            

      

     

         

     

             

It is informative to check this result via

1

MM

 ^ ^ ^ ^ ^    

So finally we have

4 4 0 4 16 4 0 1

1 1

7 1 3 1 28 1 15 1.

12 12

1 5 3 5 4 5 15 2

x

y

z

      ^    

        

         

        

                    

It is easy to confirm the validity of this result by plugging back into the original

equations.

§3.7: 35

Solution: We want to think about the following matrix as a combination of rotations

and reflections. First we check the determinant to find

  

So we conclude that this transformation contains a reflection. We also note that the

2x2 sub matrix in the upper vector left corner corresponds to an active 90 degree

rotation about the z axis, xy y ,   x (see Eq. 7.12), while the lower right corner

means a reflection through the xy plane, z   z ,

x y

y x

z z

 ^     

1

1

i i i

AA i i i i

i

i

A A i i i i

i i i

 ^    ^ ^  

§3.9: 8

Solution: We want to verify some properties of the Hermitian conjugate. (a) From

Eq. (9.10) in Boas we have  

T T T

ABB A. Here we go through the same argument

including the conjugation. We have

  ^ 

† † † † † † †

.

T T T

kl lj jk jk kj lk jl

l l

jl lk jk l

AB A B A B A B A B

B A B A AB B A

           

(b) Now we apply the transpose (or the Hermitian conjugate) to a product of more

that 2 matrices (Eq. 9.11 in Boas) by using the associative property of matrix

multiplication (see Eq. 9.8 in Boas). We have

T T^ T T T T T

T T T T

ABCD A BCD B CD A CD B A

D C B A