# Beam Elements (TYPE3)

Radioss uses a shear beam theory or Timoshenko formulation for its beam elements.

- No cross-section deformation in its plane.
- No cross-section warping out of its plane.

With these assumptions, transverse shear is taken into account.

This formulation can degenerate into a standard Euler-Bernoulli formulation (the cross section remains normal to the beam axis). This choice is under user control.

## Local Coordinate System

The properties describing a beam element are all defined in a local coordinate system.

This coordinate system can be seen in Figure 1. Nodes 1 and 2 of the element are used to define the local X axis, with the origin at node 1. The local Y axis is defined using node 3, which lies in the local XY plane, along with nodes 1 and 2. The Z axis is determined from the vector cross product of the positive X and Y axes.

In case Node 3 is not defined, Nodes 1 and 2 of the element are used to define the local X axis, with the origin at node 1. Local XY plane is defined using local X axis and Global Z axis (or Global Y axis, if local X is parallel to global Z). The local Y axis is determined from the vector cross product of the positive Z and X axes.

The local Y direction is first defined at time $t=0$ and its position is updated at each cycle, taking into account the rotation of the X axis. The Z axis is always orthogonal to the X and Y axes.

## Beam Element Geometry

- $A$
- Cross section area
- ${I}_{x}$
- Area moment of inertia of cross section about local x axis
- ${I}_{y}$
- Area moment of inertia of cross section about local y axis
- ${I}_{z}$
- Area moment of inertia of cross section about local z axis

The area moments of inertia about the y and z axes are concerned with bending. They can be calculated using the relationships:

The area moment of inertia about the x axis concerns torsion. This is simply the summation of the previous two moments of Ontario:

## Minimum Time Step

The minimum time step for a beam element is determined using the following relation:

Where,

$c$ is the speed of sound: $\sqrt{E/\rho}$

$a=\mathrm{min}\left(1,\frac{1}{\sqrt{\frac{L}{\frac{b}{12}+\frac{12\left(1+\upsilon \right)}{5}}}}\right)\cdot {F}_{1}$

${F}_{1}=\sqrt{1+2{d}^{2}}-\sqrt{2}d$

$b=\frac{A{L}^{2}}{\mathrm{max}\left({I}_{y},{I}_{z}\right)}$

$d=\mathrm{max}({d}_{m},{d}_{f})$

## Beam Element Behavior

- Membrane or axial deformation
- Torsion
- Bending about the z axis
- Bending about the y axis

### Membrane Behavior

The force rate vector for an element is calculated using the relation:

- $E$
- Elastic modulus
- $l$
- Beam element length
- ${\upsilon}_{x}$
- Nodal velocity in x direction

With the force rate equation, the force vector is determined using explicit time integration:

### Torsion

The moment rate vector is computed by:

- $G$
- Modulus of rigidity
- ${\dot{\theta}}_{x}$
- Angular rotation rate

The moment about the X axis is found by explicit time integration:

### Bending About Z-axis

Two vector fields must be solved for forces and moments. The rate equations are:

Where,

${\varphi}_{y}=\frac{144\left(1+v\right){I}_{z}}{5A{l}^{2}}$ ,

$\upsilon $ is the Poisson's ratio.

The factor ${\varphi}_{y}$ takes into account transverse shear.

The time integration for both is:

### Bending About Y-axis

The rate equations are:

Where, ${\Phi}_{z}=\frac{144\left(1+\nu \right){I}_{y}}{5A{l}^{2}}$ .

Like bending about the Z axis, the factor ${\Phi}_{z}$ introduces transverse shear.

With the time integration, the expression is:

## Material Properties

- Elastic
- Elasto-plastic

### Elastic Behavior

The elastic beam is defined using material LAW1 which is a simple linear material law.

The cross-section of a beam is defined by its area $A$ and three area moments of inertia ${I}_{x}$ , ${I}_{y}$ and ${I}_{z}$ .

An elastic beam can be defined with these four parameters. For accuracy and stability, the following limitations should be respected:

### Elasto-plastic Behavior

A global plasticity model is used.

The main assumption is that the beam cross section is full and rectangular. Optimal relations between sections and section inertia are:

However, this model also returns good results for the circular or ellipsoidal cross-section. For tubular or H cross-sections, plasticity will be approximated.

Recommendations:

### Global Beam Plasticity

The elasto-plastic beam element is defined using material LAW2:

The increment of plastic strain is:

The equivalent strain rate is derived from the total energy rate:

Yield stress:

If ${\sigma}_{eq}>{\sigma}_{y}$ , you perform a radial return on the yield surface:

and for $i$ = x, y, z:

## Inertia Computation

The computational method of inertia for some kinds of elements as beam is particular as the inertia has to be transferred to the extremities of the beam. The nodal inertias are computed in function of the material density $\rho $ , the cross-section area $S$ , the element length $L$ and the moments of inertia ${I}_{xx},\text{\hspace{0.17em}}{I}_{yy}\text{\hspace{0.17em}},{I}_{zz}$ :