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๐—”๐—ป๐—ฎ๐—น๐˜†๐˜€๐—ถ๐˜€ ๐—ผ๐—ณ ๐—ณ๐˜‚๐—ฒ๐—น ๐˜€๐—น๐—ผ๐˜€๐—ต๐—ถ๐—ป๐—ด ๐—ถ๐—ป๐˜€๐—ถ๐—ฑ๐—ฒ ๐—ฎ ๐—ณ๐˜‚๐—ฒ๐—น ๐˜๐—ฎ๐—ป๐—ธ ๐—ฑ๐˜‚๐—ฟ๐—ถ๐—ป๐—ด ๐—ฏ๐—ฟ๐—ฎ๐—ธ๐—ถ๐—ป๐—ด, ๐˜๐˜‚๐—ฟ๐—ป๐—ถ๐—ป๐—ด, ๐—ฎ๐—ป๐—ฑ ๐˜๐—ผ๐—ฟ๐˜€๐—ถ๐—ผ๐—ป๐—ฎ๐—น ๐—บ๐—ผ๐˜๐—ถ๐—ผ๐—ป

Fuel sloshing is one of the critical challenges in vehicle dynamics, directly influencing ๐˜ด๐˜ต๐˜ข๐˜ฃ๐˜ช๐˜ญ๐˜ช๐˜ต๐˜บ, ๐˜ฑ๐˜ณ๐˜ฆ๐˜ด๐˜ด๐˜ถ๐˜ณ๐˜ฆ ๐˜ง๐˜ญ๐˜ถ๐˜ค๐˜ต๐˜ถ๐˜ข๐˜ต๐˜ช๐˜ฐ๐˜ฏ๐˜ด, and ๐˜ด๐˜ต๐˜ณ๐˜ถ๐˜ค๐˜ต๐˜ถ๐˜ณ๐˜ข๐˜ญ ๐˜ญ๐˜ฐ๐˜ข๐˜ฅ๐˜ด.

Fuel sloshing is one of the critical challenges in vehicle dynamics, directly influencing ๐˜ด๐˜ต๐˜ข๐˜ฃ๐˜ช๐˜ญ๐˜ช๐˜ต๐˜บ, ๐˜ฑ๐˜ณ๐˜ฆ๐˜ด๐˜ด๐˜ถ๐˜ณ๐˜ฆ ๐˜ง๐˜ญ๐˜ถ๐˜ค๐˜ต๐˜ถ๐˜ข๐˜ต๐˜ช๐˜ฐ๐˜ฏ๐˜ด, ๐˜ด๐˜ต๐˜ณ๐˜ถ๐˜ค๐˜ต๐˜ถ๐˜ณ๐˜ข๐˜ญ ๐˜ญ๐˜ฐ๐˜ข๐˜ฅ๐˜ด, ๐˜ข๐˜ฏ๐˜ฅ ๐˜ง๐˜ถ๐˜ฆ๐˜ญ ๐˜ฅ๐˜ฆ๐˜ญ๐˜ช๐˜ท๐˜ฆ๐˜ณ๐˜บ ๐˜ฑ๐˜ฆ๐˜ณ๐˜ง๐˜ฐ๐˜ณ๐˜ฎ๐˜ข๐˜ฏ๐˜ค๐˜ฆ ๐˜ฅ๐˜ถ๐˜ณ๐˜ช๐˜ฏ๐˜จ ๐˜ข๐˜จ๐˜จ๐˜ณ๐˜ฆ๐˜ด๐˜ด๐˜ช๐˜ท๐˜ฆ ๐˜ฎ๐˜ข๐˜ฏ๐˜ฆ๐˜ถ๐˜ท๐˜ฆ๐˜ณ๐˜ด.

This study presents a detailed ๐—–๐—ผ๐—บ๐—ฝ๐˜‚๐˜๐—ฎ๐˜๐—ถ๐—ผ๐—ป๐—ฎ๐—น ๐—™๐—น๐˜‚๐—ถ๐—ฑ ๐——๐˜†๐—ป๐—ฎ๐—บ๐—ถ๐—ฐ๐˜€ (๐—–๐—™๐——) investigation on the influence of porous media in controlling fuel sloshing behavior inside a moving fuel tank under dynamic operating conditions.

This work presents a comprehensive CFD investigation of the influence of porous media on fuel sloshing behavior in a fuel-carrying tank under dynamic vehicle maneuvers, including sudden braking, turning, and twisting conditions:

โ€ข Initial vehicle speed: 22 m/s
โ€ข Complete braking within: 3 seconds
โ€ข Turning & torsional motion range: 8ยฐโ€“10ยฐ

The fluid flow behavior within the tank is modeled by solving the Navierโ€“Stokes and continuity equations, ensuring accurate prediction of momentum and mass conservation throughout the computational domain. These governing equations provide detailed insights into the transient velocity and pressure distributions generated during vehicle motion.

To capture the multiphase interaction between fuel and air, the ๐—ฉ๐—ผ๐—น๐˜‚๐—บ๐—ฒ ๐—ผ๐—ณ ๐—™๐—น๐˜‚๐—ถ๐—ฑ (๐—ฉ๐—ข๐—™) method is employed for precise tracking of the fluid interface and phase distribution over time. This approach enables accurate simulation of the sloshing dynamics under complex operating conditions.

Furthermore, the porous medium effects are modeled using the Darcyโ€“Forchheimer approach, where pressure losses are represented through viscous and inertial resistance components.

The Darcy coefficient accounts for viscous dissipation dominant at low flow velocities, whereas the Forchheimer coefficient captures nonlinear inertial effects arising at higher velocities due to flow acceleration, eddies, and localized turbulence within the porous structure.

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