Tensor Algebra Exercises: A Comprehensive Guide to Understanding Tensor Operations, Study Guides, Projects, Research of Mathematical Physics

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EXERCISES
97
--
i.
V.
T.
ii.
T
.
8.
iii.
(V
.
T)
x
V.
iv.
(V
.
T)
x
(1.
v).
v.
(V
.
T)
.
(T
.
V).
(V
.
T)
=
0
for any
V?
T)
=
0
for any
v?
(b)
What values for the elements of
r,
other than
Ti,
=
0,
will result in
V
X
(c)
What values for the elements of
T,
other
than
Tij
=
0,
will result in
V. (V.
--
-
-
16.
Use subscriptlsummation notation
to
show that the expressions
(T.C)XD
and
T.
CxD
=(
1
are not necessarily equal
17.
An orthogonal
(u,
v,z)
coordinate system
is
defined by the set of equations
relating its coordinates to a standard set of Cartesian coordinates,
X
(a)
Determine the elements of the transformation matrix
[a].
(b)
-
At the Cartesian point
(1,1,1)
let the vector
v
=
1
8,
+
2
(c)
At the Cartesian point
(1,1,1)
let the tensor
+
3
Sz.
Express
V
at this point using
(u,
u,
z)
system vector components and basis vectors.
=
1
6183
+
2
&2C1
+
3
6263
+
46362.
Express
T
at this point using
(u,
v,z)
system tensor elements and
basis vectors.
18.
Consider
a
dumbbell positioned in the xy-plane of a Cartesian system, as shown
in the figure below. The moment
of
inertia tensor for this object expressed in this
Cartesian system is
-
- -
1
=
I.
.&&
'1
1
J
-2
0
144,
[;2
;
(I].
Find the basis vectors
of
a coordinate system in which the moment
of
inertia
tensor is diagonalized. Draw the dumbbell in that system.
pf3

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EXERCISES (^97)

i. V. T.

ii. T. 8. iii. (V .T) x V. iv. (V. T) x (1. v). v. (V. T). (T. V).

(V. T ) = 0 for any V?

T) = 0 for any v?

(b) What values for the elements of r, other than Ti, = 0, will result in V X

( c ) What values for the elements of T, other than Tij = 0, will result in V. ( V.

16. Use subscriptlsummation notation to show that the expressions

( T. C ) X D and T. C x D = ( 1 are not necessarily equal

17. An orthogonal ( u , v , z ) coordinate system is defined by the set of equations relating its coordinates to a standard set of Cartesian coordinates, X

(a) Determine the elements of the transformation matrix [a].

(b) - At the Cartesian point ( 1 , 1 , 1 ) let the vector v = 1 8 , + 2

( c ) At the Cartesian point ( 1 , 1 , 1 ) let the tensor

  • 3 Sz. Express V at this point using (u, u, z ) system vector components and basis vectors. = 1 6183 + 2 &2C1 + 3 6263 +

46362. Express T at this point using (u, v , z ) system tensor elements and basis vectors. 18. Consider a dumbbell positioned in the xy-plane of a Cartesian system, as shown in the figure below. The moment of inertia tensor for this object expressed in this Cartesian system is

1 = I. .&& '1 1 J

1 4 4 , [ ; 2 ; (I].

Find the basis vectors of a coordinate system in which the moment of inertia tensor is diagonalized. Draw the dumbbell in that system.

98 INTRODUCTION TO TENSORS

-l /

Y

M

1

19. Let a tensor T = Ti,i$6, in a two-dimensional Cartesian system be represented by the matrix array

(a) Find the eigenvalues and eigenvectors of this matrix array. (b) Plot the eigenvectors and show their relation to the Cartesian basis vectors. (c) Are the eigenvectors orthogonal? Is the matrix array Hermitian? (d) Repeat parts (a)-(c) for the tensor

  1. Let the components of the conductivity tensor in a Cartesian system be repre- sented by

-^ - 1^^0

iT;-[r]= ; ;I.

Identify an electric field vector, by specifying its components, that will result in a current density that is parallel to this electric field.

  1. Using subscript/summation notation, show that the eigenvalues of a Hermitian matrix are pure real. Show that the eigenvectorsgenerated by the diagonalization of a Hermitian matrix generate orthogonal eigenvectors. Start with a second-rank tensor that is assumed to have off-diagonal elements that may be complex,
      T = (^) -4JT. .$.@. I J '