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Created with Raphaël 2.2.01Sep31Aug29282622211825Jul181716111093127Jun2518171310828May27262523221614131223Apr9824Mar2221191022Jan913Dec12109865328Nov151331Oct30Sep1664312Jul1185328Jun2714Feb24Jan32130Dec16Nov121196517Sep1318Jul30May25Apr2417159515Mar9825Feb2115987626Jan14121154120Dec1965325Nov2019161514124328Oct272625242321Reduce the eps for the FD to 1e-10Actually test FD with a 50-decimal-digits floating point typeRemove the public 'energy' method of the FD assemblerMore infrastructure for doing FD with a multiprecision typeAdd infrastructure to do FD approximations with a multiprecision number typeReplace 1.0 by T(1.0)Do not use the StructuredGridFactory for a YaspGridTest computing the Hessian of a fixed iterateMeasure the time needed to solve the quadratic minimization problemsOnly warn when energy increasesExport T as field_type[bugfix] Add missing skew part in finite-strain membrane energyAlso inject 'log'Implement mixed writing with a P3 basisMinor bugfix: Bit sets vor Dirichlet and Neumann vertices was too largeWork without numpyOutput files by the mixed FE code should start with 'mixed-'Don't abort when the order is not 2 -- simply warn and skipMonitor the overall energy of the quadratic subproblems[bugfix] Use setRhs to properly reset the rhs of a monotone multigrid stepMove mmgStep preprocess out of the solver iterationFix index bugMinor simplificationAllow public access to the basisFirst implementation of a mixed discretization for Cosserat continuaUse local installation of ADOL-C for the time beingRemove the default implementation using FD approximationTowards allowing FD using multi-precision number typesAdd (rudimentary) method to write mixed Cosserat configurationCompute Cosserat strain given only the gradient of the deformation, and the rotationImplement assignment from FieldVector<T,4>Implement projection onto normal space and the Weingarten mapUse Entity<0>::subEntities instead of Entity<0>::count, when available[bugfix] Projection onto the normal space of R^n was wrongNew GFE assembler using finite differences for gradient and Hesse matrixAvoid the conversion operator of FieldMatrix<,1,1>Avoid signed/unsigned warningUse Gauss-Seidel instead of IPOpt as the base solverTerminate when the _global_ correction drops below the limitevaluateDerivative: use the GramSchmidt-Solver to solve the rank-deficient systems