VM-LSDYNA-SOLVE-045
VM-LSDYNA-SOLVE-045
Fundamental Frequency of a Square Plate with Opening
Overview
| Reference: | Blevins, R. J. (1979). Formula for natural frequency and mode shape. Van Nostrand Reinhold Company Inc., p.274, table 11-8, case 2. |
| Analysis Type(s): | Implicit Vibration Analysis |
| Element Type(s): | 3D Hexahedral and Tetrahedral Elements |
| Input Files: | Link to Input Files Download Page |
Test Case
This test case models the vibration of a clamped squared plate with a central opening. The objective is to validate the fundamental natural frequency of the structure. The thin square plate has a length of 1.0 m, a circular opening diameter of 0.1 m, and thickness of 0.01 m. The outer surface of the plate is clamped, while the inner surface (opening) is free to move. Figure 160 illustrates the domain geometry, main dimensions and boundary conditions.
The following table lists the material and geometric properties. The units for the current test case follow the International System of Units.
| Material Properties | Geometric Properties |
|---|---|
|
Young's modulus (E) = 2 ⋅ 1011 Pa Poisson's ratio (ν) = 0.3 Density (ρ) = 7850 kg/m3 |
Plate length (l) = 1.0 m Opening radius (r) = 0.1 m Thickness (h) = 0.01 m |
Considering a thin flat square plate of homogeneous, linear elastic material, the mode
shapes and natural frequencies are characterized by two integer indices,
i and j. The mode indices i
and j represent the number of nodal lines in the length directions of a
square plate. The natural frequency of the plate can be calculated as:
(15) |
where is a dimensionless parameter,
is the plate length,
is the plate thickness,
is the mass per unit area,
is the Young's modulus, and
is the Poisson's ratio. The parameter
is a function of the mode indices i and
j, the Poisson's ratio, the ratio between the opening diameter and
plate length, and the boundary conditions of the outer and inner surfaces. The mass per unit
area
is calculated as the product of the material density ρ and the plate
thickness
. For a clamped condition,
= 0.3, and
= 0.2, the dimensionless parameters
= 35.7. Therefore, the natural frequency for the first mode, also known as
fundamental frequency, is 43.39 Hz.
Analysis Assumptions and Modeling Notes
One part is defined to represent the square plate with opening, being meshed with 3D hexahedral and tetrahedral elements with sizes of 0.01 m (length directions) and 0.00125 m (thickness direction). The plate elements use a constant stress solid element formulation (*SECTION_SOLID with ELFORM=1) and an elastic material card (*MAT_ELASTIC) with a density of 7850 kg/m3, a Young's modulus of 2 ⋅ 1011 Pa, and a Poisson's ratio of 0.3. The nodes corresponding to the outer surface of the plate are grouped using *SET_NODE_LIST, and the keyword *BOUNDARY_SPC_SET is used to define the constraint of this node set (translational and rotational constraint about the three axes). The keywords *CONTROL_IMPLICIT_GENERAL (IMFLAG=1), *CONTROL_IMPLICIT_DYNAMICS (IMASS=0), and *CONTROL_IMPLICIT_EIGENVALUE (NEIG=1) are used to activate the implicit eigenvalue, static analysis with one eigenvalue to be extracted.
Results Comparison
The square plate configuration for the first mode is shown in the figure below. The visualization of the first mode is performed by reading the d3eigv file, generated for the modal analysis.
To quantify the error between the theoretical and LS-DYNA results, the fundamental frequency of the square plate with opening and its relative error is calculated and shown in the following table. This comparison verifies the excellent agreement between the fundamental frequencies.
| Results | Target | LS-DYNA Solver | Error (%) |
|---|---|---|---|
| Fundamental Frequency, f11 (Hz) | 43.39 | 43.10 | -0.67 |


