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Show that the contracted tensor TijkVkis a 2nd-rank tensors.

Short Answer

Expert verified

Answer

The equation has been proven.

Step by step solution

01

Given Information

The contracted tensorTijkVk.

02

Definition of a cartesian tensor.

The first rank tensor is just a vector. A tensor of second rank has nine components (in three dimensions) in every rectangular coordinate system.

03

Prove the statement.

The contracted tensor TijkVk.

TijkVk=ailajmaknTImnakpVpTijkVk=aiIajmaknakpTImnVpTijkVk=aiIaimδpnTImnVpTijkVk=aijajmTImnVn

Hence, Tkjis a 2ndrank vector.

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Most popular questions from this chapter

Show that (3.9) follows from (3.8) . Hint: Give a proof by contradiction. Let Sαβbe the parenthesis in ; you may find it useful to think of the components written as a matrix. You want to prove that all 9 components of Sαβare zero. Suppose it is claimed that S12is not zero. Since V'βis an arbitrary vector, take it to be the vector , and observe that SαβV'βis then not zero in contradiction to .Similarly show that all components of Sαβare zero as claims.

Verify equations(2.6).

Show that the nine quantities Tij=(∂Vi)/(∂xJ) (which are the Cartesian components of ∇V where V is a vector) satisfy the transformation equations (2.14)for a Cartesian 2nd -rank tensor. Show that they do not satisfy the general tensor transformation equations as in (10.12) . Hint: Differentiate (10.9)or(10.10)partially with respect to, say,x'k. You should get the expected terms [as in(10.12) ] plus some extra terms; these extraneous terms show that(∂Vi)/(∂xJ) is not a tensor under general transformations. Comment: It is possible to express the components of∇V correctly in general coordinate systems by taking into account the variation of the basis vectors in length and direction.

Show that the sum of two 3rd-rank tensors is a 3rd-rank tensor. Hint: Write the transformation law for each tensor and then add your two equations. Divide out the factors to leave the result T'αβγ+S'αβγ=aαiaβjaγk(Tijk+Sijk).

Write the transformation equation for a 3rd-rank tensor; for a 5th-rank tensor

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