Tensor derivative (continuum mechanics)

Tensor derivative (continuum mechanics)

The derivatives of scalars, vectors, and second-order tensors with respect to second-order tensors are of considerable use in continuum mechanics. These derivatives are used in the theories of nonlinear elasticity and plasticity, particularly in the design of algorithms for numerical simulations. J. C. SImo and T. J. R. Hughes, 1998, Computational Inelasticity, Springer]

The directional derivative provides a systematic way of finding these derivatives. J. E. Marsden and T. J. R. Hughes, 2000, Mathematical Foundations of Elasticity, Dover.]

Derivatives with respect to vectors and second-order tensors

The definitions of directional derivatives for various situations are given below. It is assumed that the functions are sufficiently smooth that derivatives can be taken.

Derivatives of vector valued functions of vectors

Let mathbf{f}(mathbf{v}) be a vector valued function of the vector mathbf{v}. Then the derivative of mathbf{f}(mathbf{v}) with respect to mathbf{v} (or at mathbf{v}) in the direction mathbf{u} is the second order tensor defined as: frac{partial mathbf{f{partial mathbf{vcdotmathbf{u} = Dmathbf{f}(mathbf{v}) [mathbf{u}] = left [frac{d }{d alpha}~mathbf{f}(mathbf{v} + alpha~mathbf{u}) ight] _{alpha = 0}for all vectors mathbf{u}.

"Properties:"

1) If mathbf{f}(mathbf{v}) = mathbf{f}_1(mathbf{v}) + mathbf{f}_2(mathbf{v}) then frac{partial mathbf{f{partial mathbf{vcdotmathbf{u} = left(frac{partial mathbf{f}_1}{partial mathbf{v + frac{partial mathbf{f}_2}{partial mathbf{v ight)cdotmathbf{u}

2) If mathbf{f}(mathbf{v}) = mathbf{f}_1(mathbf{v}) imesmathbf{f}_2(mathbf{v}) then frac{partial mathbf{f{partial mathbf{vcdotmathbf{u} = left(frac{partial mathbf{f}_1}{partial mathbf{vcdotmathbf{u} ight) imesmathbf{f}_2(mathbf{v}) + mathbf{f}_1(mathbf{v}) imesleft(frac{partial mathbf{f}_2}{partial mathbf{vcdotmathbf{u} ight)

3) If mathbf{f}(mathbf{v}) = mathbf{f}_1(mathbf{f}_2(mathbf{v})) then frac{partial mathbf{f{partial mathbf{vcdotmathbf{u} = frac{partial mathbf{f}_1}{partial mathbf{f}_2}cdotleft(frac{partial mathbf{f}_2}{partial mathbf{vcdotmathbf{u} ight)

Derivatives of scalar valued functions of second-order tensors

Let f(oldsymbol{S}) be a real valued function of the second order tensor oldsymbol{S}. Then the derivative of f(oldsymbol{S}) with respect to oldsymbol{S} (or at oldsymbol{S}) in the directionoldsymbol{T} is the second order tensor defined as: frac{partial f}{partial oldsymbol{S:oldsymbol{T} = Df(oldsymbol{S}) [oldsymbol{T}] = left [frac{d }{d alpha}~f(oldsymbol{S} + alpha~oldsymbol{T}) ight] _{alpha = 0}for all second order tensors oldsymbol{T}.

"Properties:"

1) If f(oldsymbol{S}) = f_1(oldsymbol{S}) + f_2(oldsymbol{S}) then frac{partial f}{partial oldsymbol{S:oldsymbol{T} = left(frac{partial f_1}{partial oldsymbol{S + frac{partial f_2}{partial oldsymbol{S ight):oldsymbol{T}

2) If f(oldsymbol{S}) = f_1(oldsymbol{S})~ f_2(oldsymbol{S}) then frac{partial f}{partial oldsymbol{S:oldsymbol{T} = left(frac{partial f_1}{partial oldsymbol{S:oldsymbol{T} ight)~f_2(oldsymbol{S}) + f_1(oldsymbol{S})~left(frac{partial f_2}{partial oldsymbol{S:oldsymbol{T} ight)

3) If f(oldsymbol{S}) = f_1(f_2(oldsymbol{S})) then frac{partial f}{partial oldsymbol{S:oldsymbol{T} = frac{partial f_1}{partial f_2}~left(frac{partial f_2}{partial oldsymbol{S:oldsymbol{T} ight)

Derivatives of tensor valued functions of second-order tensors

Let oldsymbol{F}(oldsymbol{S}) be a second order tensor valued function of the second order tensor oldsymbol{S}. Then the derivative of oldsymbol{F}(oldsymbol{S}) with respect to oldsymbol{S} (or at oldsymbol{S}) in the direction oldsymbol{T} is the fourth order tensor defined as: frac{partial oldsymbol{F{partial oldsymbol{S:oldsymbol{T} = Doldsymbol{F}(oldsymbol{S}) [oldsymbol{T}] = left [frac{d }{d alpha}~oldsymbol{F}(oldsymbol{S} + alpha~oldsymbol{T}) ight] _{alpha = 0}for all second order tensors oldsymbol{T}.

"Properties:"

1) If oldsymbol{F}(oldsymbol{S}) = oldsymbol{F}_1(oldsymbol{S}) + oldsymbol{F}_2(oldsymbol{S}) then frac{partial oldsymbol{F{partial oldsymbol{S:oldsymbol{T} = left(frac{partial oldsymbol{F}_1}{partial oldsymbol{S + frac{partial oldsymbol{F}_2}{partial oldsymbol{S ight):oldsymbol{T}

2) If oldsymbol{F}(oldsymbol{S}) = oldsymbol{F}_1(oldsymbol{S})cdotoldsymbol{F}_2(oldsymbol{S}) then frac{partial oldsymbol{F{partial oldsymbol{S:oldsymbol{T} = left(frac{partial oldsymbol{F}_1}{partial oldsymbol{S:oldsymbol{T} ight)cdotoldsymbol{F}_2(oldsymbol{S}) + oldsymbol{F}_1(oldsymbol{S})cdotleft(frac{partial oldsymbol{F}_2}{partial oldsymbol{S:oldsymbol{T} ight)

3) If oldsymbol{F}(oldsymbol{S}) = oldsymbol{F}_1(oldsymbol{F}_2(oldsymbol{S})) then frac{partial oldsymbol{F{partial oldsymbol{S:oldsymbol{T} = frac{partial oldsymbol{F}_1}{partial oldsymbol{F}_2}:left(frac{partial oldsymbol{F}_2}{partial oldsymbol{S:oldsymbol{T} ight)

4) If f(oldsymbol{S}) = f_1(oldsymbol{F}_2(oldsymbol{S})) then frac{partial f}{partial oldsymbol{S:oldsymbol{T} = frac{partial f_1}{partial oldsymbol{F}_2}:left(frac{partial oldsymbol{F}_2}{partial oldsymbol{S:oldsymbol{T} ight)

Derivative of the determinant of a tensor

The derivative of the determinant of a second order tensor oldsymbol{A} is given by: frac{partial }{partial oldsymbol{Adet(oldsymbol{A}) = det(oldsymbol{A})~ [oldsymbol{A}^{-1}] ^T ~.In an orthonormal basis, the components of oldsymbol{A} can be written asa matrix mathbf{A}. In that case, the right hand side corresponds the cofactors of the matrix.

:

References

See also

* Tensor derivative
* Directional derivative


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