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Reference documentation for deal.II version 9.6.0
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Reference documentation for deal.II version 9.6.0
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#include <deal.II/base/config.h>#include <deal.II/base/ndarray.h>#include <deal.II/base/numbers.h>#include <deal.II/base/table_indices.h>#include <deal.II/base/template_constraints.h>#include <deal.II/base/tensor.h>#include <array>Go to the source code of this file.
Namespaces | |
| namespace | internal |
| namespace | internal::SymmetricTensorImplementation |
| namespace | internal::SymmetricTensorAccessors |
Enumerations | |
| enum struct | SymmetricTensorEigenvectorMethod { hybrid , ql_implicit_shifts , jacobi } |
Functions | |
| template<int dim, typename Number = double> | |
| DEAL_II_HOST constexpr SymmetricTensor< 2, dim, Number > | unit_symmetric_tensor () |
| template<int dim, typename Number = double> | |
| DEAL_II_HOST constexpr SymmetricTensor< 4, dim, Number > | deviator_tensor () |
| template<int dim, typename Number = double> | |
| DEAL_II_HOST constexpr SymmetricTensor< 4, dim, Number > | identity_tensor () |
| template<int dim, typename Number > | |
| DEAL_II_HOST constexpr SymmetricTensor< 2, dim, Number > | invert (const SymmetricTensor< 2, dim, Number > &) |
| template<int dim, typename Number > | |
| DEAL_II_HOST constexpr SymmetricTensor< 4, dim, Number > | invert (const SymmetricTensor< 4, dim, Number > &) |
| template<int dim2, typename Number > | |
| DEAL_II_HOST constexpr Number | trace (const SymmetricTensor< 2, dim2, Number > &) |
| template<int dim, typename Number > | |
| DEAL_II_HOST constexpr SymmetricTensor< 2, dim, Number > | deviator (const SymmetricTensor< 2, dim, Number > &) |
| template<int dim, typename Number > | |
| DEAL_II_HOST constexpr Number | determinant (const SymmetricTensor< 2, dim, Number > &) |
| DEAL_II_HOST constexpr TableIndices< 2 > | internal::SymmetricTensorAccessors::merge (const TableIndices< 2 > &previous_indices, const unsigned int new_index, const unsigned int position) |
| DEAL_II_HOST constexpr TableIndices< 4 > | internal::SymmetricTensorAccessors::merge (const TableIndices< 4 > &previous_indices, const unsigned int new_index, const unsigned int position) |
| template<int rank_, int dim, typename Number , typename OtherNumber > | |
| DEAL_II_HOST constexpr SymmetricTensor< rank_, dim, typename ProductType< Number, OtherNumber >::type > | operator+ (const SymmetricTensor< rank_, dim, Number > &left, const SymmetricTensor< rank_, dim, OtherNumber > &right) |
| template<int rank_, int dim, typename Number , typename OtherNumber > | |
| DEAL_II_HOST constexpr SymmetricTensor< rank_, dim, typename ProductType< Number, OtherNumber >::type > | operator- (const SymmetricTensor< rank_, dim, Number > &left, const SymmetricTensor< rank_, dim, OtherNumber > &right) |
| template<int rank_, int dim, typename Number , typename OtherNumber > | |
| DEAL_II_HOST constexpr Tensor< rank_, dim, typename ProductType< Number, OtherNumber >::type > | operator+ (const SymmetricTensor< rank_, dim, Number > &left, const Tensor< rank_, dim, OtherNumber > &right) |
| template<int rank_, int dim, typename Number , typename OtherNumber > | |
| DEAL_II_HOST constexpr Tensor< rank_, dim, typename ProductType< Number, OtherNumber >::type > | operator+ (const Tensor< rank_, dim, Number > &left, const SymmetricTensor< rank_, dim, OtherNumber > &right) |
| template<int rank_, int dim, typename Number , typename OtherNumber > | |
| DEAL_II_HOST constexpr Tensor< rank_, dim, typename ProductType< Number, OtherNumber >::type > | operator- (const SymmetricTensor< rank_, dim, Number > &left, const Tensor< rank_, dim, OtherNumber > &right) |
| template<int rank_, int dim, typename Number , typename OtherNumber > | |
| DEAL_II_HOST constexpr Tensor< rank_, dim, typename ProductType< Number, OtherNumber >::type > | operator- (const Tensor< rank_, dim, Number > &left, const SymmetricTensor< rank_, dim, OtherNumber > &right) |
| template<int dim, typename Number > | |
| DEAL_II_HOST constexpr Number | third_invariant (const SymmetricTensor< 2, dim, Number > &t) |
| template<int dim, typename Number > | |
| DEAL_II_HOST constexpr Number | trace (const SymmetricTensor< 2, dim, Number > &d) |
| template<int dim, typename Number > | |
| DEAL_II_HOST constexpr Number | first_invariant (const SymmetricTensor< 2, dim, Number > &t) |
| template<typename Number > | |
| DEAL_II_HOST constexpr Number | second_invariant (const SymmetricTensor< 2, 1, Number > &) |
| template<typename Number > | |
| DEAL_II_HOST constexpr Number | second_invariant (const SymmetricTensor< 2, 2, Number > &t) |
| template<typename Number > | |
| DEAL_II_HOST constexpr Number | second_invariant (const SymmetricTensor< 2, 3, Number > &t) |
| template<typename Number > | |
| std::array< Number, 1 > | eigenvalues (const SymmetricTensor< 2, 1, Number > &T) |
| template<typename Number > | |
| std::array< Number, 2 > | eigenvalues (const SymmetricTensor< 2, 2, Number > &T) |
| template<typename Number > | |
| std::array< Number, 3 > | eigenvalues (const SymmetricTensor< 2, 3, Number > &T) |
| template<int dim, typename Number > | |
| void | internal::SymmetricTensorImplementation::tridiagonalize (const ::SymmetricTensor< 2, dim, Number > &A, ::Tensor< 2, dim, Number > &Q, std::array< Number, dim > &d, std::array< Number, dim - 1 > &e) |
| template<int dim, typename Number > | |
| std::array< std::pair< Number, Tensor< 1, dim, Number > >, dim > | internal::SymmetricTensorImplementation::ql_implicit_shifts (const ::SymmetricTensor< 2, dim, Number > &A) |
| template<int dim, typename Number > | |
| std::array< std::pair< Number, Tensor< 1, dim, Number > >, dim > | internal::SymmetricTensorImplementation::jacobi (::SymmetricTensor< 2, dim, Number > A) |
| template<typename Number > | |
| std::array< std::pair< Number, Tensor< 1, 2, Number > >, 2 > | internal::SymmetricTensorImplementation::hybrid (const ::SymmetricTensor< 2, 2, Number > &A) |
| template<typename Number > | |
| std::array< std::pair< Number, Tensor< 1, 3, Number > >, 3 > | internal::SymmetricTensorImplementation::hybrid (const ::SymmetricTensor< 2, 3, Number > &A) |
| template<int dim, typename Number > | |
| std::array< std::pair< Number, Tensor< 1, dim, Number > >, std::integral_constant< int, dim >::value > | eigenvectors (const SymmetricTensor< 2, dim, Number > &T, const SymmetricTensorEigenvectorMethod method=SymmetricTensorEigenvectorMethod::ql_implicit_shifts) |
| template<int rank_, int dim, typename Number > | |
| DEAL_II_HOST constexpr SymmetricTensor< rank_, dim, Number > | transpose (const SymmetricTensor< rank_, dim, Number > &t) |
| template<int dim, typename Number > | |
| DEAL_II_HOST constexpr SymmetricTensor< 4, dim, Number > | outer_product (const SymmetricTensor< 2, dim, Number > &t1, const SymmetricTensor< 2, dim, Number > &t2) |
| template<int dim, typename Number > | |
| std::pair< SymmetricTensor< 2, dim, Number >, SymmetricTensor< 2, dim, Number > > | positive_negative_split (const SymmetricTensor< 2, dim, Number > &original_tensor) |
| template<int dim, typename Number > | |
| std::tuple< SymmetricTensor< 2, dim, Number >, SymmetricTensor< 2, dim, Number >, SymmetricTensor< 4, dim, Number >, SymmetricTensor< 4, dim, Number > > | positive_negative_projectors (const SymmetricTensor< 2, dim, Number > &original_tensor) |
| template<int dim, typename Number > | |
| DEAL_II_HOST constexpr SymmetricTensor< 2, dim, Number > | symmetrize (const Tensor< 2, dim, Number > &t) |
| template<int rank_, int dim, typename Number > | |
| DEAL_II_HOST constexpr SymmetricTensor< rank_, dim, Number > | operator* (const SymmetricTensor< rank_, dim, Number > &t, const Number &factor) |
| template<int rank_, int dim, typename Number > | |
| DEAL_II_HOST constexpr SymmetricTensor< rank_, dim, Number > | operator* (const Number &factor, const SymmetricTensor< rank_, dim, Number > &t) |
|
strong |
An enumeration for the algorithm to be employed when performing the computation of normalized eigenvectors and their corresponding eigenvalues by the eigenvalues() and eigenvectors() methods operating on SymmetricTensor objects.
The specialized algorithms utilized in computing the eigenvectors are presented in [131].
Definition at line 3068 of file symmetric_tensor.h.
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inlineconstexpr |
Return a unit symmetric tensor of rank 2, i.e., the \(\text{dim}\times\text{dim}\) identity matrix \(\mathbf I\). For example, if dim==2, then this matrix has the form
\[ I_{2\times 2} = \begin{pmatrix} 1 & 0 \\ 0 & 1 \end{pmatrix}. \]
Definition at line 3158 of file symmetric_tensor.h.
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inlineconstexpr |
Return the tensor of rank 4 that, when multiplied by a symmetric rank 2 tensor \(\mathbf T\) returns the deviator \(\text{dev}\ \mathbf T\). It is the operator representation of the linear deviator operator \(\mathbb P\), also known as the volumetric projection tensor, calculated as:
\begin{align*} \mathbb{P} &=\mathbb{S} -\frac{1}{\text{dim}} \mathbf I \otimes \mathbf I \\ \mathcal{P}_{ijkl} &= \frac 12 \left(\delta_{ik} \delta_{jl} + \delta_{il} \delta_{jk} \right) - \frac{1}{\text{dim}} \delta_{ij} \delta_{kl} \end{align*}
For every tensor T, there holds the identity deviator<dim,Number>(T) == deviator_tensor<dim,Number>() * T, up to numerical round-off.
\[ \text{dev}\mathbf T = \mathbb P : \mathbf T \]
\[ \frac{\partial \text{dev}\mathbf{T}}{\partial \mathbf T} = \mathbb P. \]
Definition at line 3186 of file symmetric_tensor.h.
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inlineconstexpr |
Return the fourth-order symmetric identity tensor \(\mathbb S\) which maps symmetric second-order tensors, such as \(\mathbf A\), to themselves.
\[ \mathbb S : \mathbf A = \mathbf A \]
Note that this tensor, even though it is the identity, has a somewhat funny form, and in particular does not only consist of zeros and ones. For example, for dim=2, the identity tensor has all zero entries except for
\[ \mathcal{S}_{0000} = \mathcal{S}_{1111} = 1 \]
\[ \mathcal{S}_{0101} = \mathcal{S}_{0110} = \mathcal{S}_{1001} = \mathcal{S}_{1010} = \frac 12. \]
In index notation, we can write the general form
\[ \mathcal{S}_{ijkl} = \frac 12 \left( \delta_{ik} \delta_{jl} + \delta_{il} \delta_{jk} \right). \]
To see why this factor of \(1 / 2\) is necessary, consider computing \(\mathbf A= \mathbb I : \mathbf B\). For the element \(A_{01}\) we have \(A_{01} = \mathcal{S}_{0100} B_{00} + \mathcal{S}_{0111} B_{11} + \mathcal{S}_{0101} B_{01} + \mathcal{S}_{0110} B_{10}\). On the other hand, we need to have \(A_{01} = B_{01}\), and symmetry implies \(B_{01}=B_{10}\), leading to \(A_{01} = (\mathcal{S}_{0101} + \mathcal{S}_{0110}) B_{01}\), or, again by symmetry, \(\mathcal{S}_{0101} = \mathcal{S}_{0110} = \frac 12\). Similar considerations hold for the three-dimensional case.
This issue is also explained in the introduction to step-44.
Definition at line 3215 of file symmetric_tensor.h.
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constexpr |
Invert a symmetric rank-2 tensor.
Definition at line 3250 of file symmetric_tensor.h.
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constexpr |
Invert a symmetric rank-4 tensor. Since symmetric rank-4 tensors are mappings from and to symmetric rank-2 tensors, they can have an inverse.
If a tensor is not invertible, then the result is unspecified, but will likely contain the results of a division by zero or a very small number at the very least.
Definition at line 3270 of file symmetric_tensor.h.
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inlineconstexpr |
Compute and return the trace of a tensor of rank 2, i.e. the sum of its diagonal entries. The trace is the first invariant of a rank-2 tensor.
\[ \text{tr} \mathbf A = \sum_i A_{ii} \]
|
inlineconstexpr |
Compute the deviator of a symmetric tensor, which is defined as \(\text{dev} \mathbf T = \mathbf T - \frac{1}{\text{dim}} \text{tr}\mathbf T \; \mathbf I\), where \(\mathbf I\) is the identity operator. This quantity equals the original tensor minus its contractive or dilative component and refers to the shear in, for example, elasticity.
Definition at line 3141 of file symmetric_tensor.h.
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inlineconstexpr |
Compute the determinant of a rank 2 symmetric tensor. The determinant is also commonly referred to as the third invariant of rank-2 tensors.
For a one-dimensional tensor, the determinant equals the only element and is therefore equivalent to the trace.
For greater notational simplicity, there is also a third_invariant() function that returns the determinant of a tensor.
Definition at line 2724 of file symmetric_tensor.h.
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inlineconstexpr |
Addition of two symmetric tensors of equal rank. The result is another SymmetricTensor that has a number type that is compatible with the operation.
If possible (e.g. when Number and OtherNumber are of the same type, or if the result of Number() + OtherNumber() is another Number), you should use operator+= instead since this does not require the creation of a temporary variable.
Definition at line 2618 of file symmetric_tensor.h.
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inlineconstexpr |
Subtraction of two symmetric tensors of equal rank. The result is another SymmetricTensor that has a number type that is compatible with the operation.
If possible (e.g. when Number and OtherNumber are of the same type, or if the result of Number() - OtherNumber() is another Number), you should use operator-= instead since this does not require the creation of a temporary variable.
Definition at line 2643 of file symmetric_tensor.h.
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constexpr |
Addition of a SymmetricTensor and a general Tensor of equal rank. The result is a general Tensor that has a number type that is compatible with the operation.
Definition at line 2663 of file symmetric_tensor.h.
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constexpr |
Addition of a general Tensor with a SymmetricTensor of equal rank. The result is a general Tensor that has a number type that is compatible with the operation.
Definition at line 2680 of file symmetric_tensor.h.
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constexpr |
Subtraction of a general Tensor from a SymmetricTensor of equal rank. The result is a general Tensor that has a number type that is compatible with the operation.
Definition at line 2697 of file symmetric_tensor.h.
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constexpr |
Subtraction of a SymmetricTensor from a general Tensor of equal rank. The result is a general Tensor that has a number type that is compatible with the operation.
Definition at line 2714 of file symmetric_tensor.h.
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constexpr |
Compute the determinant of a rank 2 symmetric tensor. This function therefore computes the same value as the determinant() functions and is only provided for greater notational simplicity (since there are also functions first_invariant() and second_invariant()).
\[ I_3 (\mathbf A) = III (\mathbf A) = \det (\mathbf A) \]
Definition at line 2764 of file symmetric_tensor.h.
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inlineconstexpr |
Definition at line 2773 of file symmetric_tensor.h.
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constexpr |
Compute the trace of a rank 2 symmetric tensor. This function therefore computes the same value as the trace() functions and is only provided for greater notational simplicity (since there are also functions second_invariant() and third_invariant()).
\[ I_1 (\mathbf A) = I (\mathbf A) = \text{tr} \mathbf A = \sum_i A_{ii} \]
Definition at line 2795 of file symmetric_tensor.h.
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constexpr |
Compute the second invariant of a tensor of rank 2. The second invariant of a tensor \(\mathbf A\) is defined as \(I_2 (\mathbf A) = II(\mathbf A) = \frac 12 \left[ (\text{tr} \mathbf A)^2 - \text{tr} (\mathbf{A}^2) \right]\).
For the kind of arguments to this function, i.e., a rank-2 tensor of size 1, the result is simply zero.
Definition at line 2814 of file symmetric_tensor.h.
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constexpr |
Compute the second invariant of a tensor of rank 2. The second invariant of a tensor \(\mathbf A\) is defined as \(I_2 (\mathbf A) = II(\mathbf A) = \frac 12 \left[ (\text{tr} \mathbf A)^2 - \text{tr} (\mathbf{A}^2) \right]\).
For the kind of arguments to this function, i.e., a symmetric rank-2 tensor of size 2, the result is (counting indices starting at one) \(I_2(\mathbf A) = II(\mathbf A) = \frac 12 \left[ (A_{11} + A_{22})^2 - (A_{11}^2+2 A_{12}^2+ A_{22}^2) \right] = A_{11} A_{22} - A_{12}^2\). As expected, for the \(2\times 2\) symmetric tensors this function handles, this equals the determinant of the tensor. (This is so because for \(2\times 2\) symmetric tensors, there really are only two invariants, so the second and third invariant are the same; the determinant is the third invariant.)
Definition at line 2841 of file symmetric_tensor.h.
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constexpr |
Compute the second invariant of a tensor of rank 2. The second invariant of a tensor \(\mathbf A\) is defined as \(I_2 (\mathbf A) = II(\mathbf A) = \frac 12 \left[ (\text{tr} \mathbf A)^2 - \text{tr} (\mathbf{A}^2) \right]\).
Definition at line 2858 of file symmetric_tensor.h.
| std::array< Number, 1 > eigenvalues | ( | const SymmetricTensor< 2, 1, Number > & | T | ) |
Return the eigenvalues of a symmetric \(1 \times 1\) tensor. The (single) entry of the tensor is, of course, equal to the (single) eigenvalue.
| std::array< Number, 2 > eigenvalues | ( | const SymmetricTensor< 2, 2, Number > & | T | ) |
Return the eigenvalues of a symmetric \(2\times 2\) tensor. The array of eigenvalues is sorted in descending order.
For \(2\times 2\) tensors, the eigenvalues of tensor \(\mathbf T\) are the roots of the characteristic polynomial \(0 = \lambda^2 - \lambda\;\text{tr}\mathbf{T} + \det \mathbf{T}\) as given by \(\lambda_1, \lambda_2 = \frac{1}{2} \left[ \text{tr} \mathbf{T} \pm \sqrt{(\text{tr} \mathbf{T})^2 - 4 \det \mathbf{T}} \right]\).
| std::array< Number, 3 > eigenvalues | ( | const SymmetricTensor< 2, 3, Number > & | T | ) |
Return the eigenvalues of a symmetric \(3\times 3\) tensor. The array of eigenvalues is sorted in descending order.
For \(3\times 3\) tensors, the eigenvalues of tensor \(\mathbf T\) are the roots of the characteristic polynomial \(0 = \lambda^3 - \lambda^2\;\text{tr}\mathbf T - \frac{1}{2} \lambda \left[\text{tr}(\mathbf{T}^2) - (\text{tr}\mathbf T)^2\right] - \det \mathbf T\).
| std::array< std::pair< Number, Tensor< 1, dim, Number > >, std::integral_constant< int, dim >::value > eigenvectors | ( | const SymmetricTensor< 2, dim, Number > & | T, |
| const SymmetricTensorEigenvectorMethod | method = SymmetricTensorEigenvectorMethod::ql_implicit_shifts ) |
Return the eigenvalues and eigenvectors of a real-valued rank-2 symmetric tensor \(\mathbf T\). The array of matched eigenvalue and eigenvector pairs is sorted in descending order (determined by the eigenvalues).
The specialized algorithms utilized in computing the eigenvectors are presented in [131].
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constexpr |
Return the transpose of the given symmetric tensor. Since we are working with symmetric objects, the transpose is of course the same as the original tensor. This function mainly exists for compatibility with the Tensor class.
Definition at line 3131 of file symmetric_tensor.h.
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inlineconstexpr |
Return the tensor of rank 4 that is the outer product of the two tensors given as arguments, i.e. the result \(\mathbb A = \mathbf{T}_1 \otimes \mathbf{T}_2\) satisfies \(\mathbb A : \mathbf B = (\mathbf{T}_2 : \mathbf B) \mathbf{T}_1\) for all symmetric tensors \(\mathbf B\). In index notation
\[ \mathcal{A}_{ijkl} = (T_1)_{ij} (T_2)_{kl} \]
For example, the deviator tensor \(\mathbb P = \mathbb I - \frac{1}{\text{dim}} \mathbf I \otimes \mathbf I\) can be computed as identity_tensor<dim>() - 1/d * outer_product (unit_symmetric_tensor<dim>(), unit_symmetric_tensor<dim>()), since the (double) contraction with the unit tensor yields the trace of a symmetric tensor ( \(\mathbf I : \mathbf B = \text{tr} \mathbf B\)).
Definition at line 3301 of file symmetric_tensor.h.
| std::pair< SymmetricTensor< 2, dim, Number >, SymmetricTensor< 2, dim, Number > > positive_negative_split | ( | const SymmetricTensor< 2, dim, Number > & | original_tensor | ) |
Perform a spectrum decomposition of a 2nd-order symmetric tensor original_tensor given as the input argument,
\[ \mathrm{original\_tensor} = \sum_i \lambda_i \, \boldsymbol{n}_i \otimes \boldsymbol{n}_i, \]
where \(\lambda_i\) is the eigenvalue, and \(\boldsymbol{n}_i\) is the corresponding eigenvector. The output is a pair of 2nd-order symmetric tensors. The first term in the pair is the positive part of the input tensor, and the second term in the pair is the negative part of the input tensor, that is,
\[ \mathrm{positive\_part\_tensor} = \sum_i \left<\lambda_i\right>_+ \boldsymbol{n}_i \otimes \boldsymbol{n}_i, \quad \mathrm{negative\_part\_tensor} = \sum_i \left<\lambda_i\right>_- \boldsymbol{n}_i \otimes \boldsymbol{n}_i, \]
where \(\left<\lambda_i\right>_+ = \mathrm{max}\{ \lambda_i, 0 \}\) and \(\left<\lambda_i\right>_- = \mathrm{min}\{ \lambda_i, 0 \}\). Obviously,
\[ \mathrm{positive\_part\_tensor} + \mathrm{negative\_part\_tensor} = \mathrm{original\_tensor}. \]
| [in] | original_tensor | The 2nd-order symmetric tensor to be split into the positive and negative parts |
Definition at line 3343 of file symmetric_tensor.h.
| std::tuple< SymmetricTensor< 2, dim, Number >, SymmetricTensor< 2, dim, Number >, SymmetricTensor< 4, dim, Number >, SymmetricTensor< 4, dim, Number > > positive_negative_projectors | ( | const SymmetricTensor< 2, dim, Number > & | original_tensor | ) |
This function is similar to the function positive_negative_split(). That is, perform a spectrum decomposition of a 2nd-order symmetric tensor original_tensor given as the input argument, and split it into a positive part and a negative part. Moreover, this function also provides the derivatives. Let \(\mathbf{A}\) represent the input 2nd-order symmetric tensor original_tensor, \(\mathbf{A}^+\) represent the positive part, and \(\mathbf{A}^-\) represent the negative part. Then, two fourth-order tensors are defined as
\[ \mathbb{P}^+ = \frac{\partial \mathbf{A}^+}{\partial \mathbf{A}}, \quad \mathbb{P}^- = \frac{\partial \mathbf{A}^-}{\partial \mathbf{A}}, \]
where \(\mathbb{P}^+\) is the positive projector and \(\mathbb{P}^-\) is the negative projector. These two fourth-order tensors satisfy the following properties:
\[ \mathbb{P}^+ : \mathbf{A} = \mathbf{A}^+, \quad \mathbb{P}^- : \mathbf{A} = \mathbf{A}^-. \]
Since \(\mathbb{P}^+\) and \(\mathbb{P}^-\) are 4th-order projectors,
\[ \mathbb{P}^+ : \mathbf{A}^+ = \mathbf{A}^+, \quad \mathbb{P}^- : \mathbf{A}^- = \mathbf{A}^-, \quad \mathbb{P}^+ : \mathbf{A}^- = \mathbb{P}^- : \mathbf{A}^+ = \mathbf{0}. \]
Lastly,
\[ \mathbb{P}^+ + \mathbb{P}^- = \mathbb{S}, \]
where \(\mathbb{S}\) is the fourth-order symmetric identity tensor Physics::Elasticity::StandardTensors< dim >::S. The output of this function is a tuple containing four terms. The first term is \(\mathbf{A}^+\), the second term is \(\mathbf{A}^-\), the third term is \(\mathbb{P}^+\), and the fourth term is \(\mathbb{P}^-\).
| [in] | original_tensor | The 2nd-order symmetric tensor to be split into the positive and negative parts |
Definition at line 3410 of file symmetric_tensor.h.
|
inlineconstexpr |
Return the symmetrized version of a full rank-2 tensor, i.e. \(\text{sym}\mathbf A = \frac 12 \left(\mathbf A + \mathbf{A}^T\right)\), as a symmetric rank-2 tensor. This is the version for general dimensions.
Definition at line 3534 of file symmetric_tensor.h.
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inlineconstexpr |
Multiplication of a symmetric tensor of general rank with a scalar from the right. This version of the operator is used if the scalar has the same data type as is used to store the elements of the symmetric tensor.
Definition at line 3559 of file symmetric_tensor.h.
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constexpr |
Multiplication of a symmetric tensor of general rank with a scalar from the left. This version of the operator is used if the scalar has the same data type as is used to store the elements of the symmetric tensor.
Definition at line 3577 of file symmetric_tensor.h.
1.11.0