Objective

To determine the stress–strain state of a beam fixed at both ends under the uniformly distributed load, concentrated axial and transverse forces, and a bending moment.

Reference

S. Timoshenko, Resistance des materiaux, t.1, Paris, Eyrolles, 1976, p. 26. M. Courtand et P. Lebelle, Formulaire du beton arme, t.2, Paris, Eyrolles, 1976, p. 219.

Problem statement

To determine the vertical displacement Z, the axial force N, and the bending moment M at mid-span of the beam (point G), as well as the horizontal reaction H at the left end (point A).

Design model

A beam fixed at both ends is subjected to:
– a uniformly distributed load P acting over the entire span length l;
– co-directional concentrated axial forces F1 and F2, located at a distance of 0.3l from the left and right ends, respectively;
– a concentrated transverse force F, located at a distance of 0.3l from the right end;
– a concentrated bending moment C, located at a distance of 0.3l from the left end.

Initial geometry of analytical model

Initial geometry of analytical model

Initial geometry of FE model

Initial geometry of FE model

Geometry

Beam length L = 1 m
Moment of inertia J = 1,7 * 10-8 m4

Material properties

Modulus of elasticity Å = 2,0 * 1011 Pa
Poisson's ratio ν = 0,2

Loads

Uniformly distributed load Ð = 24 kN/m;
Concentrated force F1 = 30 kN;
Concentrated force F2 = 10 kN;
Concentrated force F = 20 kN;
Concentrated bending moment C = 3 kN.


Output data

Vertical displacements, Z (m)

Vertical displacements, Z (m)

Diagram of axial forces, N (N)

Diagram of axial forces, N (N)

Diagram of bending moment, M (kN*m)

Diagram of bending moment, M (kN*m)

Comparison of calculation results

Parameter Analytical solution LIRA-FEM Error, %
Vertical displacement Z (point G) (m) -4,9023·10-2 -4,9023·10-2 0
Axial force N (point G) (N): -6000,0 -6000,0 0
Bending moment M (point G) (kN*m) -2800,0 -2800,0 0
Horizontal reaction H (point A) (N) 24000,0 24000,0 0

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