Micromechanics of composites/Proof 2: Difference between revisions

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Tensor-vector identity 2

Let 𝐯 be a vector field and let 𝑺 be a second-order tensor field. Let 𝐚 and 𝐛 be two arbitrary vectors. Show that

[(𝐯𝐚)(𝑺𝐛)]=𝐚[{𝐯𝑺+𝐯(𝑺T)}𝐛].

Proof:

Using the identity (φ𝐮)=𝐮φ+φ𝐮 we have

[(𝐯𝐚)(𝑺𝐛)]=(𝑺𝐛)(𝐯𝐚)+(𝐯𝐚)(𝑺𝐛).

From the identity (𝐮𝐯)=𝐮T𝐯+𝐯T𝐮, we have (𝐯𝐚)=𝐯T𝐚+𝐚T𝐯.

Since 𝐚 is constant, 𝐚=0, and we have

(𝑺𝐛)(𝐯𝐚)=(𝑺𝐛)(𝐯T𝐚).

From the relation 𝐚(𝑨T𝐛)=𝐛(𝑨𝐚) we have

(𝑺𝐛)(𝐯T𝐚)=𝐚[𝐯(𝑺𝐛)].

Using the relation 𝑨(𝑩𝐛)=(𝑨𝑩)𝐛, we get

𝐯(𝑺𝐛)=(𝐯𝑺)𝐛.

Therefore, the final form of the first term is

(𝑺𝐛)(𝐯𝐚)=𝐚[(𝐯𝑺)𝐛].

For the second term, from the identity (𝑺T𝐯)=𝑺:𝐯+𝐯(𝑺) we get, (𝑺𝐛)=𝑺T:𝐛+𝐛(𝑺T).

Since 𝐛 is constant, 𝐛=0, and we have

(𝐯𝐚)(𝑺𝐛)=(𝐯𝐚)[𝐛(𝑺T)]=𝐚[{𝐛(𝑺T)}𝐯].

From the definition (𝐮𝐯)𝐚=(𝐚𝐯)𝐮, we get

[𝐛(𝑺T)]𝐯=[𝐯(𝑺T)]𝐛.

Therefore, the final form of the second term is

(𝐯𝐚)(𝑺𝐛)=𝐚[𝐯(𝑺T)]𝐛.

Adding the two terms, we get

[(𝐯𝐚)(𝑺𝐛)]=𝐚[(𝐯𝑺)𝐛]+𝐚[𝐯(𝑺T)]𝐛.

Therefore,

[(𝐯𝐚)(𝑺𝐛)]=𝐚[{𝐯𝑺+𝐯(𝑺T)}𝐛]

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