Seminar talk, 18 September 2024: Difference between revisions
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We present general case for <math>n=1</math> and several systems for <math>n=2</math> and <math>3</math>. The key is that the Riemann invariant at the microscale is the "flux" rather than "density". It allows for exact solutions of several 1D problems: "smoothing" of shocks and "sharpening" of rarefaction waves into shocks due to microscale <math>x</math>- and <math>t</math>-dependencies, flows in piecewise homogeneous media. It also allows formulating an upscaling algorithm based on the analytical solutions and its invariant properties. | We present general case for <math>n=1</math> and several systems for <math>n=2</math> and <math>3</math>. The key is that the Riemann invariant at the microscale is the "flux" rather than "density". It allows for exact solutions of several 1D problems: "smoothing" of shocks and "sharpening" of rarefaction waves into shocks due to microscale <math>x</math>- and <math>t</math>-dependencies, flows in piecewise homogeneous media. It also allows formulating an upscaling algorithm based on the analytical solutions and its invariant properties. | ||
| video = | | video = | ||
| slides = | | slides = [[Media:Moscow_Osja_240918.pdf|Moscow_Osja_240918.pdf]] | ||
| references = [[Media:f(s,x)_exact_upscaling_240918.pdf|f(s,x)_exact_upscaling_240918.pdf]] | | references = [[Media:f(s,x)_exact_upscaling_240918.pdf|f(s,x)_exact_upscaling_240918.pdf]] | ||
| 79YY-MM-DD = 7975-90-81 | | 79YY-MM-DD = 7975-90-81 | ||
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Revision as of 13:50, 18 September 2024
Speaker: Pavel Bedrikovetsky
Title: Exact solutions and upscaling in conservation law systems
Abstract:
Numerous transport processes in nature and industry are described by conservation law systems , . This corresponds to upper scale, like rock or core scale in porous media, column length in chemical engineering, or multi-block scale in city transport. The micro heterogeneity at lower scales introduces - or -dependencies into the large-scale conservation law system, like or . Often, numerical micro-scale modelling highly exceeds the available computational facilities in terms of calculation time or memory. The problem is a proper upscaling: how to "average" the micro-scale -dependent to calculate the upper-scale flux ?
We present general case for and several systems for and . The key is that the Riemann invariant at the microscale is the "flux" rather than "density". It allows for exact solutions of several 1D problems: "smoothing" of shocks and "sharpening" of rarefaction waves into shocks due to microscale - and -dependencies, flows in piecewise homogeneous media. It also allows formulating an upscaling algorithm based on the analytical solutions and its invariant properties.
Slides: Moscow_Osja_240918.pdf
References:
f(s,x)_exact_upscaling_240918.pdf