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The test problem is a structural model of a car windscreen. <ref name="meerbergen2007"/> | The test problem is a structural model of a car windscreen. <ref name="meerbergen2007"/> | ||
This is a 3D problem discretized with <math>7564</math> nodes and <math>5400</math> linear hexahedral elements (3 layers of <math>60 \times 30</math> elements). | This is a 3D problem discretized with <math>7564</math> nodes and <math>5400</math> linear hexahedral elements (3 layers of <math>60 \times 30</math> elements). | ||
The mesh is shown in | The mesh is shown in Fig. 1. | ||
The material is glass with the following properties: | The material is glass with the following properties: | ||
The [[wikipedia:Young's_modulus|Young modulus]] is <math>7\times10^{10}\mathrm{N}/\mathrm{m}^2</math>, the density is <math>2490 \mathrm{kg}/\mathrm{m}^3</math>, and the [[wikipedia:Poisson's_ratio|Poisson ratio]] is <math>0.23</math>. The natural damping is <math>10\%</math>, i.e. <math>\gamma=0.1</math>. | The [[wikipedia:Young's_modulus|Young modulus]] is <math>7\times10^{10}\mathrm{N}/\mathrm{m}^2</math>, the density is <math>2490 \mathrm{kg}/\mathrm{m}^3</math>, and the [[wikipedia:Poisson's_ratio|Poisson ratio]] is <math>0.23</math>. The natural damping is <math>10\%</math>, i.e. <math>\gamma=0.1</math>. | ||
Revision as of 10:25, 14 April 2022
Description
This is an example for a model in the frequency domain of the form
where represents a unit point load in one unknown of the state vector. is a symmetric positive-definite matrix and where is symmetric positive semi-definite.
The test problem is a structural model of a car windscreen. [1] This is a 3D problem discretized with nodes and linear hexahedral elements (3 layers of elements). The mesh is shown in Fig. 1. The material is glass with the following properties: The Young modulus is , the density is , and the Poisson ratio is . The natural damping is , i.e. . The structural boundaries are free (free-free boundary conditions). The windscreen is subjected to a point force applied on a corner. The goal of the model reduction is the fast evaluation of . Model reduction is used as a fast linear solver for a sequence of parametrized linear systems.
The discretized problem has dimension . The goal is to estimate for . In order to generate the plots, the frequency range was discretized as with .
Fig. 1 shows the mesh of the car windscreen and Fig. 2 the frequency response .
Origin
This benchmark is part of the Oberwolfach Benchmark Collection[2]; No. 38886.
Data
Download matrices in the Matrix Market format:
- Windscreen-dim1e4-windscreen.tar.gz (21.5 MB)
The archive contains files windscreen.K, windscreen.M and windscreen.B representing , and accordingly.
Dimensions
System structure:
with .
System dimensions:
, , .
Citation
To cite this benchmark, use the following references:
- For the benchmark itself and its data:
- Oberwolfach Benchmark Collection, Windscreen. hosted at MORwiki - Model Order Reduction Wiki, 2018. http://modelreduction.org/index.php/Windscreen
@MISC{morwiki_windscreen,
author = {{Oberwolfach Benchmark Collection}},
title = {Windscreen},
howpublished = {hosted at {MORwiki} -- Model Order Reduction Wiki},
url = {http://modelreduction.org/index.php/Windscreen},
year = 20XX
}
- For the background on the benchmark:
@article{Mee07,
author = {K. Meerbergen},
title = {Fast frequency response computation for {R}ayleigh damping},
journal = {International Journal for Numerical Methods in Engineering},
volume = {73},
number = {1},
pages = {96--106},
year = {2007},
doi = {10.1002/nme.2058},
}
References
- ↑ K. Meerbergen, Fast frequency response computation for Rayleigh damping, International Journal for Numerical Methods in Engineering, 73(1): 96--106, 2007.
- ↑ J.G. Korvink, E.B. Rudnyi, Oberwolfach Benchmark Collection, In: Dimension Reduction of Large-Scale Systems, Lecture Notes in Computational Science and Engineering, vol 45: 311--315, 2005.

