3.6.14 Acoustic submodeling

Products: ABAQUS/Standard  ABAQUS/Explicit  

Elements tested

AC2D3    AC2D4    AC2D4R    AC2D6    AC2D8   

AC3D4    AC3D6    AC3D8    AC3D8R    AC3D10    AC3D15    AC3D20   

ACAX3    ACAX4    ACAX4R    ACAX6    ACAX8   

Features tested

The submodeling capability is applied to an acoustic model of a duct. The global model is represented by either 20 linear elements or 10 quadratic elements along the lengthwise direction of the duct. An absorbing boundary condition is applied at one end of the duct; loads are applied to the other end. The submodel models the part of the duct close to the absorbing end and has a finer mesh than the global model. The driven nodes of the submodel lie along the global model element boundaries. Two-dimensional, three-dimensional, and axisymmetric models are tested for the driven nodes' acoustic pressure; the *STEADY STATE DYNAMICS, DIRECT and *DYNAMIC procedures are used in ABAQUS/Standard, and the *DYNAMIC, EXPLICIT procedure is used in ABAQUS/Explicit. The transient simulations are performed for period of time long enough to allow the wave to propagate past the end of the duct. Each element type used in the global model can be tested against each other element type of similar dimensionality in the submodel.

Problem description

Model:

The two-dimensional and axisymmetric global models have dimensions of 1.0 × 10.0, and the three-dimensional global models have dimensions of 1.0 × 10.0 × 1.0. In the two- and three-dimensional cases the submodel covers the end of the duct from 8.5 to 10; the axisymmetric submodel is from 8.0 to 10.0.

Material:

Bulk modulus of acoustic medium1.42176 × 105
Density1.293

Boundary conditions:

In the global linear models the bottom surface is subjected to acoustic pressures of 1.0 at the corner nodes; in the ABAQUS/Standard global quadratic models consistent loads corresponding to a uniform acoustic pressure load are applied. In the submodel analyses the boundary conditions are driven by the results from the global models.

Loading:

The top of the acoustic medium has an impedance boundary condition with the proportionality factors between pressure and displacement equal to 2.3323 × 10–3.

Results and discussion

The amplitudes of acoustic pressures and their phases are correctly identified in the global analysis file output and applied at the driven nodes in the submodel analysis.

Input files

ABAQUS/Standard input files

Global analyses:


pgca3afd.inp

ACAX3 elements.

pgca4afd.inp

ACAX4 elements.

pgca6afd.inp

ACAX6 elements.

pgca8afd.inp

ACAX8 elements.

pgc23afd.inp

AC2D3 elements.

pgc24afd.inp

AC2D4 elements.

pgc26afd.inp

AC2D6 elements.

pgc28afd.inp

AC2D8 elements.

pgc34afd.inp

AC3D4 elements.

pgc36afd.inp

AC3D6 elements.

pgc38afd.inp

AC3D8 elements.

pgc3aafd.inp

AC3D10 elements.

pgc3fafd.inp

AC3D15 elements.

pgc3kafd.inp

AC3D20 elements.

submodelacoust_gd_acax4_std.inp

ACAX4 elements; global *DYNAMIC analysis.

submodelacoust_gd_ac2d4_std.inp

AC2D4 elements; global *DYNAMIC analysis.

submodelacoust_gd_ac3d8_std.inp

AC3D8 elements; global *DYNAMIC analysis.

Submodel analyses:


psca3af1.inp

ACAX3 elements.

psca4af1.inp

ACAX4 elements.

psca6af1.inp

ACAX6 elements.

psca8af1.inp

ACAX8 elements.

psc23af1.inp

AC2D3 elements.

psc24af1.inp

AC2D4 elements.

psc26af1.inp

AC2D6 elements.

psc28af1.inp

AC2D8 elements.

psc34af1.inp

AC3D4 elements.

psc36af1.inp

AC3D6 elements.

psc38af1.inp

AC3D8 elements.

psc3aaf1.inp

AC3D10 elements.

psc3faf1.inp

AC3D15 elements.

psc3kaf1.inp

AC3D20 elements.

submodelacoust_sd_acax4_std.inp

ACAX4 elements; submodel *DYNAMIC analysis.

submodelacoust_sd_ac2d4_std.inp

AC2D4 elements; submodel *DYNAMIC analysis.

submodelacoust_sd_ac3d8_std.inp

AC3D8 elements; submodel *DYNAMIC analysis.