Connections
Acoustic pressure distribution¶
Acoustic pressure distribution in 3D¶
A script demonstrating the solution of the scalar Helmholtz equation for a situation inspired by the physical problem of WiFi propagation in an apartment¶
Vibro-acoustic problem 3D acoustic domain with 2D perforated deforming interface¶
Transient advection equation in 1D solved using discontinous galerkin method¶
Laplace equation (eg: temperature distribution) on a cube geometry with different boundary condition values on the cube sides¶
Each of the two equations describes a flow in one compartment of a porous medium¶
Laplace equation in 1D with a variable coefficient¶
Two Laplace equations with multiple linear combination constraints¶
A Laplace equation that models the flow of “dry water” around an obstacle shaped like a Citroen CX¶
Laplace equation with Dirichlet boundary conditions solved in a single patch NURBS domain using the isogeometric analysis (IGA) approach, using commands for interactive use¶
Example of solving Laplace’s equation on a block domain refined with level 1 hanging nodes¶
Laplace equation with shifted periodic BCs¶
Example explaining how to change Dirichlet boundary conditions depending on time¶
Laplace equation using the long syntax of keywords¶
Laplace equation with a field-dependent material parameter¶
Poisson equation with source term¶
Poisson equation solved in a single patch NURBS domain using the isogeometric analysis (IGA) approach¶
The Poisson equation with Neumann boundary conditions on a part of the boundary¶
Nonlinear Poisson’s equation example demonstrating the nonlinear diffusion and nonlinear volume force terms¶
Parallel assembling and solving of a Poisson’s equation, using commands for interactive use¶
Poisson equation¶
Transient Laplace equation with a localized power source and periodic boundary conditions¶
Laplace equation using the short syntax of keywords¶
Laplace equation with Dirichlet boundary conditions given by a sine function and constants¶
The transient advection-diffusion equation with a given divergence-free advection velocity¶
Transient heat equation with time-dependent source term, three different material domains and Newton type boundary condition loss term¶
Transient Laplace equation with non-constant initial conditions given by a function¶
Transient Laplace equation¶
Transient Laplace equation (heat equation) with non-constant initial conditions given by a function, using commands for interactive use¶
Compute homogenized elastic coefficients for a given heterogeneous linear elastic microstructure¶
Homogenized nonlinear hyperelastic material with evolving microstructure deformation in each macroscopic quadrature point¶
Homogenization of the Darcy flow in a thin porous layer¶
Compute homogenized elastic coefficients for a given microstructure¶
Nearly incompressible hyperelastic material model with active fibres¶
Inflation of a Mooney-Rivlin hyperelastic balloon¶
Compare various elastic materials w¶
Incompressible generalized Yeoh hyperelastic material model¶
Nearly incompressible Mooney-Rivlin hyperelastic material model¶
Incompressible Mooney-Rivlin hyperelastic material model¶
Compressible Mooney-Rivlin hyperelastic material model¶
Porous nearly incompressible hyperelastic material with fluid perfusion¶
Dispersion analysis of a heterogeneous finite scale periodic cell¶
Elastic contact planes simulating an indentation test¶
Elastic contact sphere simulating an indentation test¶
Linear elasticity with linear combination constraints and periodic boundary conditions¶
The linear elastodynamics solution of an iron plate impact problem¶
The linear elastodynamics solution of an iron plate impact problem with identification of material parameters from simulated measurement data¶
Diametrically point loaded 2-D disk¶
Diametrically point loaded 2-D disk with postprocessing¶
Diametrically point loaded 2-D disk with nodal stress calculation¶
Diametrically point loaded 2-D disk with postprocessing and probes¶
Diametrically point loaded 2-D disk, using commands for interactive use¶
Linear elasticity with given displacements¶
Time-dependent linear elasticity with a simple damping¶
Linear elasticity solved in a single patch NURBS domain using the isogeometric analysis (IGA) approach¶
Linear elasticity example using the imperative API¶
This example shows how to use the post_process_hook to probe the output data¶
Linear elasticity with pressure traction load on a surface and constrained to one-dimensional motion¶
Nearly incompressible linear elasticity in mixed displacement-pressure formulation with comments¶
Linear viscoelasticity with pressure traction load on a surface and constrained to one-dimensional motion¶
Example demonstrating how a linear elastic term can be used to solve an elasticity problem with a material nonlinearity¶
A linear elastic beam loaded with a continuous force¶
Modal analysis of a linear elastic block in 2D or 3D¶
Modal analysis of a wheel set¶
Linear elasticity with multi node linear combination constraints¶
The linear elasticity of two discs connected using multi-point constraints¶
Linear elasticity with nodal linear combination constraints¶
Linear elasticity with a given prestress in one subdomain and a (pre)strain fibre reinforcement in the other¶
The linear elastodynamics of an elastic body loaded by a given base motion¶
Bending of a long thin cantilever beam, declarative problem description¶
Bending of a long thin cantilever beam, imperative problem description¶
An example demonstrating the usage of the truss elements in 2D¶
An example demonstrating the usage of the truss structural elements in 3D¶
Contact of two elastic bodies with a penalty function for enforcing the contact constraints¶
Live plot demonstration¶
Plot the convergence of eigenvalues (or corresponding frequencies) of an eigenvalue problem to an analytical solution, when applying the uniform mesh refinement¶
Biot problem - deformable porous medium¶
Biot problem - deformable porous medium with the no-penetration boundary condition on a boundary region¶
Biot problem - deformable porous medium with the no-penetration boundary condition on a boundary region enforced using Lagrange multipliers¶
Parallel assembling and solving of a Biot problem (deformable porous medium), using commands for interactive use¶
Biot problem - deformable porous medium with a no-penetration boundary condition imposed in the weak sense on a boundary region, using the short syntax of keywords¶
Piezo-elasticity problem - linear elastic material with piezoelectric effects¶
Piezo-elasticity problem - homogenization of a piezoelectric linear elastic matrix with embedded metalic electrodes, see [1] for details¶
The linear elastodynamics of a piezoelectric body loaded by a given base motion¶
First solve the stationary electric conduction problem¶
Thermo-elasticity with a given temperature distribution¶
Thermo-elasticity with a computed temperature demonstrating equation sequence solver¶
Navier-Stokes equations for incompressible fluid flow¶
Navier-Stokes equations for incompressible fluid flow in 2D¶
Navier-Stokes equations for incompressible fluid flow in 2D solved in a single patch NURBS domain using the isogeometric analysis (IGA) approach¶
Stabilized Navier-Stokes problem with grad-div, SUPG and PSPG stabilization solved by a custom Oseen solver¶
Stokes equations for incompressible fluid flow¶
Incompressible Stokes flow with Navier (slip) boundary conditions, flow driven by a moving wall and a small diffusion for stabilization¶
Acoustic band gaps in a strongly heterogeneous elastic body, detected using homogenization techniques¶
Acoustic band gaps in a strongly heterogeneous elastic body with a rigid inclusion, detected using homogenization techniques¶
Boron atom with 1 electron¶
Hydrogen atom¶
Quantum oscillator¶
Quantum potential well¶