Chapter 10: Q3P (page 505)
As we did in (3.3) , show that the contracted tensor is a first-rank tensor, that is, a vector.
Short Answer
Answer
The equation has been proven.
Chapter 10: Q3P (page 505)
As we did in (3.3) , show that the contracted tensor is a first-rank tensor, that is, a vector.
Answer
The equation has been proven.
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Get started for freeFollowing what we did in equations (2.14) to (2.17), show that the direct product of a vector and a -rank tensor is a -rank tensor. Also show that the direct product of two -rank tensors is a -rank tensor. Generalize this to show that the direct product of two tensors of ranks m and n is a tensor of rank m + n .
Find the inertia tensor about the origin for a mass of uniform density =1, inside the part of the unit sphere where and find the principal moments of inertia and the principal axes. Note that this is similar to Example 5 but the mass is both above and below the plane. Warning hint: This time don’t make the assumptions about symmetry that we did in Example 5.
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Parabolic.
In equation , find whether is a vector or a pseudovector assuming
(a) A, B, C are all vectors
(b) A, B, C are all pseudovectors
(c) A is a vector and B and C are pseudovectors.
Hint: Count up the number of det A factors from pseudovectors and cross products.
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