Micromechanics of composites/Proof 1

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Tensor-vector identity - 1

[(๐ฏ๐š)(๐‘บ๐›)]๐ง=๐š[{๐ฏ(๐‘บT๐ง)}๐›].

Proof:

Using the identity ๐š(๐‘จT๐›)=๐›(๐‘จ๐š) we have

๐ง[(๐ฏ๐š)(๐‘บ๐›)]=๐›[(๐ฏ๐š)(๐‘บT๐ง)].

Also, using the definition (๐ฎ๐ฏ)๐š=(๐š๐ฏ)๐ฎ we have

(๐ฏ๐š)(๐‘บT๐ง)=[(๐‘บT๐ง)๐ฏ]๐š.

Therefore,

๐ง[(๐ฏ๐š)(๐‘บ๐›)]=๐›[{(๐‘บT๐ง)๐ฏ}๐š].

Using the identity ๐š(๐‘จT๐›)=๐›(๐‘จ๐š) we have

๐›[{(๐‘บT๐ง)๐ฏ}๐š]=๐š[{(๐‘บT๐ง)๐ฏ}T๐›].

Finally, using the relation (๐ฎ๐ฏ)T=๐ฏ๐ฎ, we get

๐š[{(๐‘บT๐ง)๐ฏ}T๐›]=๐š[{๐ฏ(๐‘บT๐ง)}๐›].

Hence,

[(๐ฏ๐š)(๐‘บ๐›)]๐ง=๐š[{๐ฏ(๐‘บT๐ง)}๐›]

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