Demo problem: Bending of a 3D non-symmetric cantilever beam made of incompressible material

In this tutorial we demonstrate the solution of a 3D solid mechanics problem: the large-amplitude bending deformation of a non-symmetric cantilever beam made of incompressible Mooney-Rivlin material.

Here is an animation of the beam's deformation. In its undeformed configuration, the beam is straight and its cross-section is given by a quarter circle. The beam is loaded by an increasing gravitational body force, acting in the negative $ y$-direction, while its left end (at $ z=0 $) is held fixed. Because of its non-symmetric cross-section, the beam's downward bending deformation is accompanied by a sideways deflection.

Animation of the beam's bending deformation.

Note how the automatic mesh adaptation refines the mesh in the region of strongest bending.

The mesh

We use multiple inheritance to upgrade the already-existing refineable "quarter tube mesh" to a solid mesh. Following a call to the constructor of the underlying meshes, we set the nodes' Lagrangian coordinates to their current Eulerian positions to make the initial configuration stress-free.

/// Simple quarter tube mesh upgraded to become a solid mesh
template<class ELEMENT>
public virtual RefineableQuarterTubeMesh<ELEMENT>,
public virtual SolidMesh
/// \short Constructor:
RefineableElasticQuarterTubeMesh(GeomObject* wall_pt,
const Vector<double>& xi_lo,
const double& fract_mid,
const Vector<double>& xi_hi,
const unsigned& nlayer,
TimeStepper* time_stepper_pt=
&Mesh::Default_TimeStepper) :
//Assign the Lagrangian coordinates
/// Empty Destructor

Global parameters and functions

As usual, we define a namespace, Global_Physical_Variables, to define the problem parameters: the length of the cantilever beam, $ L $, a (pointer to) a strain energy function, the constitutive parameters $ C_1 $ and $ C_2 $ for the Mooney-Rivlin strain energy function, and a (pointer to) a constitutive equation. Finally, we define the gravitational body force which acts in the negative $ y$-direction.

/// Global variables
namespace Global_Physical_Variables
/// Length of beam
double L=10.0;
/// Pointer to strain energy function
StrainEnergyFunction* Strain_energy_function_pt=0;
/// First "Mooney Rivlin" coefficient
double C1=1.3;
/// Second "Mooney Rivlin" coefficient
double C2=1.3;
/// Pointer to constitutive law
ConstitutiveLaw* Constitutive_law_pt=0;
/// Non-dim gravity
double Gravity=0.0;
/// Non-dimensional gravity as body force
void gravity(const double& time,
const Vector<double> &xi,
Vector<double> &b)
} //end namespace

The driver code

If the code is executed without command line arguments we perform a single simulation. We start by creating the strain energy function and pass it to the constructor of the strain-energy-based constitutive equation. We then build the problem object, using oomph-lib's large-displacement Taylor-Hood solid mechanics elements which are based on a continuous-pressure/displacement formulation.

/// Driver for 3D cantilever beam loaded by gravity
int main(int argc, char* argv[])
// Run main demo code if no command line arguments are specified
if (argc==1)
// Create incompressible Mooney Rivlin strain energy function
new MooneyRivlin(&Global_Physical_Variables::C1,
// Define a constitutive law (based on strain energy function)
new IsotropicStrainEnergyFunctionConstitutiveLaw(
//Set up the problem with continous pressure/displacement

We document the initial configuration before starting a parameter study in which the magnitude of the gravitational body force is increased in small steps:

// Doc solution
// Initial values for parameter values
//Parameter incrementation
unsigned nstep=10;
double g_increment=5.0e-4;
for(unsigned i=0;i<nstep;i++)
// Increment load
// Solve the problem with Newton's method, allowing
// up to max_adapt mesh adaptations after every solve.
unsigned max_adapt=1;
// Doc solution
} // end main demo code

If the code is executed with a non-zero number of command line arguments, it performs a large number of additional self tests that we will not discuss here. See the driver code for details.

The problem class

The problem class contains the usual member functions. No action is required before the mesh adaptation; we overload the function Problem::actions_after_adapt() to pin the redundant solid pressure degrees of freedom afterwards.

/// Problem class for the 3D cantilever "beam" structure.
template<class ELEMENT>
class CantileverProblem : public Problem
/// Constructor:
/// Update function (empty)
/// Update function (empty)
/// Actions before adapt. Empty
/// Actions after adapt
// Pin the redundant solid pressures (if any)
/// Doc the solution
void doc_solution();

We overload the Problem::mesh_pt() function to return a pointer to the specific mesh used in this problem:

/// Access function for the mesh

The private member data stores a DocInfo object in which we will store the name of the output directory.

/// DocInfo object for output
DocInfo Doc_info;

The problem constructor

We start by creating the GeomObject that defines the curvilinear boundary of the beam: a circular cylinder of unit radius.

/// Constructor:
template<class ELEMENT>
// Create geometric object that defines curvilinear boundary of
// beam: Elliptical tube with half axes = radius = 1.0
double radius=1.0;
GeomObject* wall_pt=new EllipticalTube(radius,radius);
// Bounding Lagrangian coordinates
Vector<double> xi_lo(2);
Vector<double> xi_hi(2);

We build the mesh, using six axial layers of elements, before creating an error estimator and specifying the error targets for the adaptive mesh refinement.

// # of layers
unsigned nlayer=6;
//Radial divider is located half-way along the circumference
double frac_mid=0.5;
//Now create the mesh
// Set error estimator
mesh_pt())->spatial_error_estimator_pt()=new Z2ErrorEstimator;
// Error targets for adaptive refinement

We complete the build of the elements by specifying the constitutive equation and the body force. We check that the element is based on a pressure/displacement formulation, and, if so, select an incompressible formulation. (This check is only required because the self-tests not shown here also include cases in which the problem is solved using a displacement-based formulation with compressible elasticity; see also the section How to enforce incompressibility below).

// Complete build of elements
unsigned n_element=mesh_pt()->nelement();
for(unsigned i=0;i<n_element;i++)
// Cast to a solid element
ELEMENT *el_pt = dynamic_cast<ELEMENT*>(mesh_pt()->element_pt(i));
// Set the constitutive law
el_pt->constitutive_law_pt() =
// Set the body force
el_pt->body_force_fct_pt() = Global_Physical_Variables::gravity;
// Material is incompressble: Use incompressible displacement/pressure
// formulation (if the element is pressure based, that is!)
PVDEquationsWithPressure<3>* cast_el_pt =
if (cast_el_pt!=0)
} // done build of elements

We fix the position of all nodes at the left end of the beam (on boundary 0) and pin any redundant solid pressures.

// Pin the left boundary (boundary 0) in all directions
unsigned b=0;
unsigned n_side = mesh_pt()->nboundary_node(b);
//Loop over the nodes
for(unsigned i=0;i<n_side;i++)
// Pin the redundant solid pressures (if any)

Finally, we assign the equation numbers and define the output directory.

//Assign equation numbers
// Prepare output directory
} //end of constructor


The post-processing function doc_solution() simply outputs the shape of the deformed beam.

/// Doc the solution
template<class ELEMENT>
ofstream some_file;
char filename[100];
// Number of plot points
unsigned n_plot = 5;
// Output shape of deformed body
// Increment label for output files
} //end doc

Comments and exercises

How to enforce incompressibility

We stress that the imposition of incompressibility must be requested explicitly via the element's member function incompressible(). Mathematically, incompressibility is enforced via a Lagrange multiplier which manifests itself physically as the pressure. Incompressibility can therefore only be enforced for elements that employ the pressure-displacement formulation of the principle of virtual displacements. This is why we the Problem constructor checked if the element is derived from the PVDEquationsWithPressure class before setting the element's incompressible flag to true.

As usual, oomph-lib provides self-tests that assess if the enforcement incompressibility (or the lack thereof) is consistent:

You should experiment with different combinations of constitutive laws and element types to familiarise yourself with these.

Source files for this tutorial

PDF file

A pdf version of this document is available.