Starting a Convergent–Divergent Nozzle with a Busemann Diffuser

Abstract The problem of starting a convergent–divergent nozzle with a Busemann diffuser that provides a given air heating is solved. The starting simulates the nozzle acceleration in still air to a certain supersonic Mach number. The influence of viscosity on the diffuser flow is numerically investigated. The modeling is performed based on the two-dimensional non-stationary Navier−Stokes equations and the Godunov−Kolgan finite-difference scheme, adapted for calculating axisymmetric viscous gas flows. It is shown that starting the nozzle does not make it possible to obtain steady-state isentropic flow in form of a centered compression wave in the Busemann diffuser. The growth of the viscous layer leads to the formation of a system of inclined and normal shock waves moving upstream and creating zones of subsonic flow in the diffuser. The approach to the Busemann solution is not guaranteed to be reached even in the case of inviscid gas.

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Publication Details

Journal
Fluid Dynamics
Published
2026-09-21
DOI
https://doi.org/10.1134/s0015462826606170
Primary Topic
Point processes and geometric inequalities
Type
article
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article

Starting a Convergent–Divergent Nozzle with a Busemann Diffuser

Yu. V. Tunik
Fluid Dynamics
Point processes and geometric inequalities
article

Starting a Convergent–Divergent Nozzle with a Busemann Diffuser

Yu. V. Tunik
article en

Abstract

Abstract The problem of starting a convergent–divergent nozzle with a Busemann diffuser that provides a given air heating is solved. The starting simulates the nozzle acceleration in still air to a certain supersonic Mach number. The influence of viscosity on the diffuser flow is numerically investigated. The modeling is performed based on the two-dimensional non-stationary Navier−Stokes equations and the Godunov−Kolgan finite-difference scheme, adapted for calculating axisymmetric viscous gas flows. It is shown that starting the nozzle does not make it possible to obtain steady-state isentropic flow in form of a centered compression wave in the Busemann diffuser. The growth of the viscous layer leads to the formation of a system of inclined and normal shock waves moving upstream and creating zones of subsonic flow in the diffuser. The approach to the Busemann solution is not guaranteed to be reached even in the case of inviscid gas.

Fluid DynamicsVol. 61(5)
Lomonosov Moscow State University (RU)
Openalex Percentile: Top 6%
Point processes and geometric inequalities
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Starting a Convergent–Divergent Nozzle with a Busemann Diffuser — Yu. V. Tunik · Fluid Dynamics (2026) | TGRS Research Map | TGRS