allc (b) (tr C)I – CT

Advanced Engineering Mathematics
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ISBN:9780470458365
Author:Erwin Kreyszig
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Chapter2: Second-order Linear Odes
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Use indicial notation to show that

### Mathematical Expression Explanation

This section explains the partial derivative of a given function in the context of tensor calculus, specifically related to strain energy functions in continuum mechanics.

#### Expression:
\[
(b) \quad \frac{\partial I_1^c}{\partial \mathbf{C}} = (\text{tr} \, \mathbf{C}) \mathbf{I} - \mathbf{C}^T
\]

#### Explanation:
- **\(\frac{\partial I_1^c}{\partial \mathbf{C}}\)**: This represents the partial derivative of the first invariant \(I_1^c\) with respect to the tensor \(\mathbf{C}\).
  
- **\((\text{tr} \, \mathbf{C})\)**: This denotes the trace of the tensor \(\mathbf{C}\), i.e., the sum of the elements on its main diagonal.
  
- **\(\mathbf{I}\)**: Symbolizing the identity tensor, which is a matrix with ones on the diagonal and zeros elsewhere.
  
- **\(\mathbf{C}^T\)**: The transpose of tensor \(\mathbf{C}\), which flips the tensor over its diagonal.

In continuum mechanics, this equation can be used to relate the deformation gradient tensor \(\mathbf{C}\) to changes in strain energy, providing insights into the material behavior under various loading conditions.
Transcribed Image Text:### Mathematical Expression Explanation This section explains the partial derivative of a given function in the context of tensor calculus, specifically related to strain energy functions in continuum mechanics. #### Expression: \[ (b) \quad \frac{\partial I_1^c}{\partial \mathbf{C}} = (\text{tr} \, \mathbf{C}) \mathbf{I} - \mathbf{C}^T \] #### Explanation: - **\(\frac{\partial I_1^c}{\partial \mathbf{C}}\)**: This represents the partial derivative of the first invariant \(I_1^c\) with respect to the tensor \(\mathbf{C}\). - **\((\text{tr} \, \mathbf{C})\)**: This denotes the trace of the tensor \(\mathbf{C}\), i.e., the sum of the elements on its main diagonal. - **\(\mathbf{I}\)**: Symbolizing the identity tensor, which is a matrix with ones on the diagonal and zeros elsewhere. - **\(\mathbf{C}^T\)**: The transpose of tensor \(\mathbf{C}\), which flips the tensor over its diagonal. In continuum mechanics, this equation can be used to relate the deformation gradient tensor \(\mathbf{C}\) to changes in strain energy, providing insights into the material behavior under various loading conditions.
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