Sep 2026· The Physics of Fluids· Vol 38· 0 citations· 37 references
Abstract
The self-starting of a hyperloop pod, characterized by the transition from a choked to an unchoked flow state during acceleration, can substantially reduce aerodynamic drag. This study develops a quasi-one-dimensional inviscid theoretical model to elucidate the underlying self-starting mechanism. The model describes the propagation of compression waves and the frontal normal shock wave (FNSW) ahead of the pod and provides analytical solutions for the coupled velocity, temperature, and pressure fields within the disturbed region. Furthermore, numerical simulations are conducted using a two-dimensional axisymmetric model with an overset mesh technique. The SST k–ω URANS-based numerical model is validated against wind tunnel experimental data and published three-dimensional simulation results. The present theoretical predictions are cross-validated against the numerical results, showing a maximum deviation of 2.8% for the FNSW. The results indicate that self-starting is governed primarily by the relative distance between the pod and the FNSW. Within the investigated range, acceleration mainly affects the rate of flow field and aerodynamic drag evolution but does not determine whether self-starting occurs. Under the uniform acceleration assumptions, self-starting is achieved only when the blockage ratio, defined as the maximum pod cross-sectional area divided by the tube cross-sectional area, is below 0.21. This conditional threshold provides guidance for pod–tube dimensional matching and aerodynamic safety.
Downburst events generate extreme near-surface winds over a considerable area, posing significant threats to structures. The existing empirical models usually model the vertical and radial steady-state profiles of the downburst separately based on empirical equations. However, these models are difficult to consider the...
Cong-Jie Shang, Yu-Long Bao, Yong-Le Li· The Physics of Fluids· 0 citations
While accurate description of the internal structure of strong shock layers is beyond the scope of the Navier–Stokes equations [2, 4, 18, 30], continuum equations may still be used to describe weak shock layers at low Mach numbers. The present work extends the steady laminar base flow model of [11] and the two-dime...
This paper presents a multi-domain model for simulating direct current (DC) arcs by coupling thermal, fluid dynamics, and electromagnetic field equations. The magnetohydrodynamics (MHD) equations are first simplified to derive a two-dimensional (2D) axisymmetric model. The model is then discretized and implemented in M...
Vinod Kumar Maddineni, Rahul Reddy Devarapally, Nihar Panchal et al.· IEEE/IAS Industrial and Comm...· 0 citations
To obtain a better understanding and prediction of the limit-cycle oscillation (LCO) response characteristics of the F-16 aircraft, time-accurate, high-fidelity, unsteady Reynolds-averaged Navier–Stokes (URANS) numerical simulations coupled with a NASTRAN-generated finite-element method structural modal model were perf...
Sergey L. Kernazhitskiy, R. Spinetti· AIAA Journal· 0 citations
The self-starting behavior of vertical-axis wind turbines is strongly influenced by the development of vortical structures along the span. However, a fully coupled high-fidelity three-dimensional analysis of this process requires substantial computational resources. This study presents a computationally efficient, span...
Faisal Muhammad, Basel Ismail, Muhammad Saif Ullah Khalid· 0 citations
Abstract Content of image described in text. An improved model for two-dimensional wind-driven water waves is developed by incorporating both wind pressure and tangential viscous stress. These aerodynamic forces are determined via numerical simulations of turbulent flow over a slowly moving, wavy boundary, and are vali...