2017/09/19 Tuesday, September 19, 2017 8:44 AM
Trace of a second order tensor
Note: trace is a scalar CM_F17 Page 1 Note: trace is a scalar
Inner product of 2nd order tensors:
CM_F17 Page 2 Define a norm from inner product:
FYI: Other norms for tensors Vector-induced norm definition:
CM_F17 Page 3 Basically if we have a definition of a norm for a vector => from which we derive a norm for a 2nd order tensor.
This is a very good definition. If we use L2 norm for the vectors (
Then the norm of a 2nd order tensor with this definition is simply:
The inverse of a tensor:
CM_F17 Page 4 You already showed the following in your HW1:
Orthogonal tensors:
CM_F17 Page 5 Remember Q was an orthogonal tensor
CM_F17 Page 6 For an orthogonal tensor -> rows and columns are orthonormal (i.e. basis vectors of an orthonormal coordinate system)
Orthogonal tensors are nothing but:
1. Rotation (proper orthogonal (det T = 1). 2. (Rotation ?) + Reflection (improper orthogonal): (det T = -1)
CM_F17 Page 7 Examples:
CM_F17 Page 8 If T1, T2, ….. are are rotations
T = T1 T2 T3 … Is also a rotation (det T = 1 and T T = I)
Reflection: Example, reflection w.r.t. x2, x3 plane
CM_F17 Page 9 det T = -1 and T is orthogonal
For any improper orthogonal tensor we have ONE reflection + (possibly some rotations)
Some properties of orthogonal tensors
CM_F17 Page 10 CM_F17 Page 11 Higher order tensors
We will see: - Strain is a second order tensor - Stress is also a second order tensor - We know stress depends on strain (for linearized elasticity) stress is a linear function of strain:
CM_F17 Page 12 function of strain:
CM_F17 Page 13 CM_F17 Page 14 This is how a fourth order tensor components should transform (?)
Think about
Higher order generalization of dyadic product:
CM_F17 Page 15 You can show that it in fact is linear (-> is a tensor)
--- How about generalization of expanding a tensor in terms of its components:
CM_F17 Page 16 Generalization of components of a tensor:
--- Examples of expanding a tensor:
CM_F17 Page 17 Definition of polyads:
CM_F17 Page 18 Coordinate transformation rule for any order tensor:
CM_F17 Page 19