Natural Vibration Frequencies of a Cantilever Beam

Given is a cantilevered beam of length L with a rectangular cross-section of width b and height h.

Natural Vibration Frequencies of a Cantilever Beam

Sought are the three natural frequencies of the beam.
Assume L = 0.5 m, b = 0.05 m, h = 0.02 m.
The material properties are:  Young's modulus E = 2.1E+011 , Poisson's ratio ν = 0.28, the density ρ = 7800 kg / m3.

Natural Vibration Frequencies of a Cantilever Beam, the finite element model with restraints

The finite element model with restraints

The analytical solution appears as:

,

where fi - natural frequencies, E – the material Young's modulus, J – the moment of inertia, ρ – the material density, F – the area of the cross section, L – the beam length, ki - the factor that depends on the vibration mode ( k1 = 1.875, k2 = 4.694, k3 = 7.855 ).

The results are as follows*:

Table 1. Parameters of finite element mesh

Finite Element Type

Number of nodes

Number of finite elements

quadratic tetrahedron

395

906

Table 2. Result "Frequency"*

 

Numerical solution
Frequency fi*, Hz

Analytical solution
Frequency fi, Hz

Error δ = 100%*| fi* - fi| / | fi |

1

67.307

First mode of natural vibration of a cantilever beam

67.0

0.46

2

418.736

Second mode of natural vibration of a cantilever beam

420.2

0.35

3

1157.75

Third mode of natural vibration of a cantilever beam

1176.7

1.61

 

Conclusion:

The relative error of the numerical solution compared to the analytical solution is equal to 0,4-1.6% for the first and third forms when using quadratic finite elements and it grows with the increase in the form number.

*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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