Numerical investigation to the full URE equations via predictor-corrector scheme

We produce the modified Rusanov (mR) method for the full ultra-relativistic Euler (URE) model. This system describes the flow of an ideal fluid of pressure <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi mathvariant="sans-serif">p</mml:mi> </mml:math> , spatial part <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi mathvariant="sans-serif">u</mml:mi> <mml:mo>∈</mml:mo> <mml:msup> <mml:mrow> <mml:mi mathvariant="double-struck">R</mml:mi> </mml:mrow> <mml:mrow> <mml:mn>3</mml:mn> </mml:mrow> </mml:msup> </mml:math> of the dimensionless four-velocity and particle density <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi mathvariant="sans-serif">n</mml:mi> </mml:math> . The nonlinear system in question is purely hyperbolic. The mR method is formulated as predictor and corrector phases. The predictor is based on the parameter of control <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mo stretchy="false">(</mml:mo> <mml:mrow> <mml:msubsup> <mml:mrow> <mml:mi>α</mml:mi> </mml:mrow> <mml:mrow> <mml:mi>i</mml:mi> <mml:mo>+</mml:mo> <mml:mn>1</mml:mn> <mml:mo>/</mml:mo> <mml:mn>2</mml:mn> </mml:mrow> <mml:mrow> <mml:mi>n</mml:mi> </mml:mrow> </mml:msubsup> </mml:mrow> <mml:mo stretchy="false">)</mml:mo> </mml:mrow> </mml:math> , which is accountable for this scheme’s numerical diffusion. The balance conservation equation is reinstated by the corrector phase. Without utilizing Riemann problem solvers, the approach has the ability to compute the numerical flow that’s closest to the solution’s actually state. In the numerical simulation the results acquired via the mR method are compared with the Rusanov, the Lax-Friedrichs methods and reference solution with 10000 grid points calculated employing classical Rusanov. This numerical study confirms the effectiveness of the mR scheme. The mR technique can also be implemented to solve numerous other applied science models.

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Journal
Journal of low frequency noise, vibration and active control
Published
2025-03-17
DOI
https://doi.org/10.1177/14613484251325442
Primary Topic
Computational Fluid Dynamics and Aerodynamics
Type
article
Field-Weighted Citation Impact
0.00

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article

Numerical investigation to the full URE equations via predictor-corrector scheme

Mahmoud A. E. Abdelrahman, A.F. Alsarhan, H. G. Abdelwahed, Kamel Mohamed
Journal of low frequency noise, vibration and active control
Computational Fluid Dynamics and Aerodynamics
article

Numerical investigation to the full URE equations via predictor-corrector scheme

Mahmoud A. E. Abdelrahman, A.F. Alsarhan, H. G. Abdelwahed, Kamel Mohamed
article en

Abstract

We produce the modified Rusanov (mR) method for the full ultra-relativistic Euler (URE) model. This system describes the flow of an ideal fluid of pressure <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi mathvariant="sans-serif">p</mml:mi> </mml:math> , spatial part <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi mathvariant="sans-serif">u</mml:mi> <mml:mo>∈</mml:mo> <mml:msup> <mml:mrow> <mml:mi mathvariant="double-struck">R</mml:mi> </mml:mrow> <mml:mrow> <mml:mn>3</mml:mn> </mml:mrow> </mml:msup> </mml:math> of the dimensionless four-velocity and particle density <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mi mathvariant="sans-serif">n</mml:mi> </mml:math> . The nonlinear system in question is purely hyperbolic. The mR method is formulated as predictor and corrector phases. The predictor is based on the parameter of control <mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" overflow="scroll"> <mml:mrow> <mml:mo stretchy="false">(</mml:mo> <mml:mrow> <mml:msubsup> <mml:mrow> <mml:mi>α</mml:mi> </mml:mrow> <mml:mrow> <mml:mi>i</mml:mi> <mml:mo>+</mml:mo> <mml:mn>1</mml:mn> <mml:mo>/</mml:mo> <mml:mn>2</mml:mn> </mml:mrow> <mml:mrow> <mml:mi>n</mml:mi> </mml:mrow> </mml:msubsup> </mml:mrow> <mml:mo stretchy="false">)</mml:mo> </mml:mrow> </mml:math> , which is accountable for this scheme’s numerical diffusion. The balance conservation equation is reinstated by the corrector phase. Without utilizing Riemann problem solvers, the approach has the ability to compute the numerical flow that’s closest to the solution’s actually state. In the numerical simulation the results acquired via the mR method are compared with the Rusanov, the Lax-Friedrichs methods and reference solution with 10000 grid points calculated employing classical Rusanov. This numerical study confirms the effectiveness of the mR scheme. The mR technique can also be implemented to solve numerous other applied science models.

Journal of low frequency noise, vibration and active controlVol. 44(3)
Prince Sattam Bin Abdulaziz University (SA), Mansoura University (EG), South Valley University (EG), Taibah University (SA), New Valley University
Deanship of Scientific Research, Prince Sattam bin Abdulaziz University
Openalex Percentile: Top 94%
Computational Fluid Dynamics and Aerodynamics
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