Products: Abaqus/Standard Abaqus/Explicit
This example illustrates the use of Abaqus/Standard and Abaqus/Explicit to model the response of beam elements with circular cross-sections to a planar linearly increasing wave.
The results obtained using Abaqus are compared with those determined theoretically using the equations of Hicks.
Simulating the response of submerged structures of simple geometric shapes to various underwater explosions constitutes an important part of the validation of any fluid-structure interaction code.
To validate the incident wave loading feature, several beams of increasing diameter are subjected to the same incident wave load, athwartships. From Hicks we have expressions describing the actual load on the beam in terms of the cross-sectional area of the beam and the response as a function of the beam's structural mass and the entrained fluid mass. Therefore, the acceleration of a rigid mass is
The loading of immersed beams in Abaqus is achieved using incident wave loading. In this test an unconnected array of eight beam elements is subjected to a plane wave incident at 90° from the plane of the array. The amplitude of the wave is linearly increasing, providing a uniform pressure gradient. The beams have identical structural properties, but their wetted cross-sections vary from 0.3 m to 35.0 m. Consequently, the loads generated on the elements due to the incident wave will vary, and the responses will vary due to the different entrained fluid masses. Both Abaqus/Standard and Abaqus/Explicit are tested.
The acceleration results from Abaqus/Standard and Abaqus/Explicit are summarized in Table 1.14.16–1. The results agree closely with the theory.
Hicks, A. N., “The Theory of Explosion Induced Hull Whipping,” Naval Construction Research Establishment, Dunfermline, Fife, Scotland, Report NCRE/R579, March 1972.
Table 1.14.16–1 Finite element results.
![]() | A | B | ![]() | Theoretical Acceleration (Component) | Abaqus/Standard Acceleration (Component) | Abaqus/Explicit Acceleration (Component) |
---|---|---|---|---|---|---|
0.3 | 579.6 | 3.262e4 | 1.777e–2 | 8.17e–9 | 8.17e–9 | 8.17e–9 |
1.0 | 6440.0 | 3.555e4 | 1.811e–1 | 8.33e–8 | 8.33e–8 | 8.33e–8 |
3.0 | 5.796e4 | 6.131e4 | 9.453e–1 | 4.35e–8 | 4.35e–8 | 4.35e–8 |
5.0 | 1.610e5 | 1.128e5 | 1.427 | 6.56e–7 | 6.56e–7 | 6.56e–7 |
7.0 | 3.155e5 | 1.901e5 | 1.660 | 7.63e–7 | 7.63e–7 | 7.63e–7 |
9.0 | 5.216e5 | 2.931e5 | 1.779 | 8.18e–7 | 8.18e–7 | 8.18e–7 |
17.0 | 1.861e6 | 9.629e5 | 1.933 | 8.89e–7 | 8.89e–7 | 8.89e–7 |
35.0 | 7.889e6 | 3.977e5 | 1.9837 | 9.12e–7 | 9.12e–7 | 9.12e–7 |