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Typology: Lecture notes
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Problem Description:
Nomenclature:
L =5m Length of beam
b =0.5m Cross Section Base
h =0.5m Cross Section Height
E =7* Young’s Modulus of Aluminum
= 0.35 Poisson’s Ratio of Aluminum =2700 Density of Aluminum
Moment of Inertia
In this module, we will introduce the ANSYS Mechanical APDL Vibration Analysis Type. This
uses the Modal solution method. This tutorial will explore the free vibration of a cantilever
beam modeled with 1D BEAM elements and we will extract the natural frequencies and mode
shapes at these frequencies.
Theory
Natural Frequency
Using Euler-Bernoulli Beam Theory we find:
(10.1)
Normal Mode solution to the above equation is:
(10.2)
This makes equation 10.1:
(10.3)
Solution for displacement is:
(10.4)
Where:
(10.5)
Geometry
Opening ANSYS Mechanical APDL
Preferences
Key points
Since we will be using 1D Elements, our goal is to model the length of the beam.
Line
The resulting graphic should be as shown:
Real Constants and Material Properties
Now we will dimension our beam.
Now we must specify Young’s Modulus, Poisson’s Ratio and Density
2
6
7
8
The resulting graphic should be as shown:
ANSYS numbers nodes from the left extreme to the right extreme and then numbers from left to
right.
Displacement
The resulting graphic should look as shown below:
Solution
Analysis Type
The graphics area should look as below:
You can repeat these steps to view the other mode shapes produced by different frequencies.
6
5
Results
The percent error (%E) in our model can be defined as:
( )
Frequency Theoretical 2 Elements 10 Elements 500 Elements
16.45 16.427 16.419 16.
103.09 102.56 101.73 101.
288.6 338.91 279.86 279.
565.67 907.38 535.21 534.
935.09 N/A 859.22 857.
1396.895 N/A 1242.2 1236.
With an unreasonably coarse mesh, ANSYS only allows you to extract a certain amount of modes. This is shown with the 2 elements where ANSYS only calculated the first four translational frequencies and first 2 torsional frequencies. Since the theory section uses approximations to calculate the natural frequencies, the theoretical answer is not precise. As mesh is refined, our analysis shows that the answers converge to the solution. This again can be seen as ANSYS does not provide natural frequencies if the mesh is too coarse.