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# CG
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## partial integration
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name in config: `partial_integration`
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### parameters:
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- none
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### description:
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Direct application of the distributional derivative of the dipolar source term to the test function. The resulting right hand side will have as many non-zero entries as the element containing the dipole has associated degrees of freedom (e.g. nodes for linear basis functions). For tetrahedral meshes, the partial integration approach is constant within each element.
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## vertex based monopolar venant
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name in config: `venant`
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### parameters:
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- todo
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### description:
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todo
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## patch based monopolar venant
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name in config: `patch_based_venant`
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### parameters:
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- todo
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### description:
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todo
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## spatial venant
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name in config: `spatial_venant`
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### parameters:
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- todo
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### description:
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todo
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## truncated spatial venant
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name in config: `truncated_spatial_venant`
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### parameters:
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- todo
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### description:
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todo
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## whitney
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name in config: `whitney`
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### parameters:
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- todo
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### description:
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todo
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## subtraction
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name in config: `subtraction`
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### parameters:
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- todo
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### description:
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todo
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# DG
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## partial integration
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name in config: `partial_integration`
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### parameters:
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- todo
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### description:
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todo
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## patch based monopolar venant
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name in config: `patch_based_venant`
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### parameters:
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- todo
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### description:
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todo
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## spatial venant
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name in config: `spatial_venant`
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### parameters:
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- todo
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### description:
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todo
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## subtraction
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name in config: `subtraction`
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### parameters:
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- todo
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### description:
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todo
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## localized subtraction
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name in config: `localized_subtraction`
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### parameters:
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- todo
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### description:
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todo
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# UDG
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## partial integration
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name in config: `partial_integration`
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### parameters:
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- todo
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### description:
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todo
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## monopolar venant
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name in config: `patch_based_venant`
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### parameters:
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- todo
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### description:
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todo
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# CutFEM
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## partial integration
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name in config: `partial_integration`
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### parameters:
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- todo
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### description:
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todo |
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\ No newline at end of file |