| 31. | In the case of stress tensor, and changes in volume are generalized to the volume multiplied by the strain tensor.
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| 32. | This can be interpreted as the stress tensor of the composite material minus the stresses carried by the reinforcement at yielding.
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| 33. | The formulas can be simply checked by substituting the reinforcement ratios in the brittle material stress tensor and calculating the invariants.
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| 34. | Let \ boldsymbol { S } _ { ( m ) } be an objective stress tensor in the initial configuration.
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| 35. | The "'electromagnetic stress energy tensor "'contains the classical Maxwell stress tensor that governs the electromagnetic interactions.
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| 36. | The above is a condition that the constitutive laws relating the deformation gradient to the first or second Piola Kirchhoff stress tensor.
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| 37. | In the absence of such a coupling, the viscous stress tensor will have only two independent parameters and will be symmetric.
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| 38. | It follows from the Maxwell stress tensor of classical electrodynamics that the radiation pressure p is related to the internal energy density u:
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| 39. | One set of such invariants are the principal stresses of the stress tensor, which are just the eigenvalues of the stress tensor.
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| 40. | One set of such invariants are the principal stresses of the stress tensor, which are just the eigenvalues of the stress tensor.
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