14.3. BEAM3 - 2-D Elastic Beam

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Matrix or VectorShape FunctionsIntegration Points
Stiffness and Mass Matrices; and Thermal and Pressure Load Vector (Equation 12–4) and (Equation 12–5)None
Stress Stiffness Matrix(Equation 12–5)None
Load TypeDistribution
Element TemperatureLinear thru thickness and along length
Nodal TemperatureConstant thru thickness, linear along length
Pressure Linear along length

14.3.1. Element Matrices and Load Vectors

The element stiffness matrix in element coordinates is (Przemieniecki(28)):

(14–1)

where:

A = cross-section area (input as AREA on R command)
E = Young's modulus (input as EX on MP command)
L = element length
I = moment of inertia (input as IZZ on R command)
G = shear modulus (input as GXY on MP command)
Fs = shear deflection constant (input as SHEARZ on R command)

The consistent element mass matrix (LUMPM,OFF) in element coordinates is (Yokoyama(167)):

(14–2)

where:

ρ = density (input as DENS on MP command)
m = added mass per unit length (input as ADDMAS on R command)
εin = prestrain (input as ISTRN on R command)

The lumped element mass matrix (LUMPM,ON) in element coordinates is:

(14–3)

The element pressure load vector in element coordinates is:

(14–4)

For uniform lateral pressure,

(14–5)

(14–6)

(14–7)

where:

P = uniform applied pressure (units = force/length) (input on SFE command)

Other standard formulas (Roark(48)) for P1 through P6 are used for linearly varying loads, partially loaded elements, and point loads.

14.3.2. Stress Calculation

The centroidal stress at end i is:

(14–8)

where:

Fx,i = axial force (output as FORCE)

The bending stress is

(14–9)

where:

Mi = moment at end i
t = thickness of beam in element y direction (input as HEIGHT on R command)

The presumption has been made that the cross-section is symmetric.

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