Bending a Cantilever Beam under a Concentrated Load

Let us consider a cantilevered beam of length L, loaded with the force P at the right-hand end. The beam cross-section is a rectangle of width b and height h.

Bending of a Cantilever Beam under a Concentrated Load

Sought is the maximum beam deflection.
Assume P = 825 N, L = 0.5 m, b = 0.05 m, h = 0.02 m.
Material characteristics assume default values: the Young's modulus E = 2.1E+011 Pa, Poisson's ratio ν = 0.28.
The left-hand end of the beam is fixed, and the right-hand end is subjected to the load amount P, directed vertically downward.

Bending of a Cantilever Beam under a Concentrated Load, the finite element model with applied loads and restraints

The finite element model with applied loads and restraints

The analytical solution appears as:

w = ( P . L3 ) /  ( 3 . E . J ) =  4.9107E-003 m

where P – is the force, L – the beam length, E – the material Young's modulus, J = b . h3 / 12 - the moment of inertia.

After carrying out calculation with the help of AutoFEM, the following results are obtained:

Table 1.Parameters of the finite element mesh

Finite Element Type

Number of Nodes

Number of Finite Elements

quadratic tetrahedron

1017

3593

Table 2. Result "Displacement, magnitude"*

Numerical Solution
Displacement w*, m

Analytical Solution
Displacement w, m

Error δ =100%* |w* - w| / |w|

4.8792E-003

4.9107E-003

0.64

Bending of a Cantilever Beam under a Concentrated Load, Result "Displacement, magnitude" of finite element analysis

Dependence of the relative error on the number of finite elements

Conclusions:

The relative error of the numerical solution compared to the analytical solution is equal to 0.64% for quadratic finite elements.

*The results of numerical tests depend on the finite element mesh and may differ slightly from those given in the table.

 

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