Abstract

Numerical studies of the aerodynamic characteristics of the coaxial main rotor of the Kamov Ka-32 helicopter in steep descent modes, including the area of the vortex ring state (VRS) modes, have been performed. Used in this paper is an original free vortex wake model of the rotor developed by the authors. The angles of attack of the rotor αR = 30 – 90° and the rate of descent in the range of Vy = 0–30 m/s are considered. The calculations have been carried out under the condition of a fixed time-average thrust of the rotor. The visualization of the rotor wake shapes the flow structures using streamlines, and the flow velocities have been received and analyzed. The VRS boundaries in “Vx–Vy” coordinates have been constructed. The criteria used in this paper are: rotor thrust and torque pulsations, rise of rotor torque and induced velocity relative to the hovering mode. The results of the calculations are compared with the experimental and calculated data of other authors, and a satisfactory match has been obtained. The new results presented in this paper can supplement the existing experience of experimental and numerical research in this field.

Highlights

  • The steep descent modes belong to the most complex helicopter flight modes

  • These effects are related to the specifics of the main rotor aerodynamics in the vortex ring state (VRS) modes

  • One of the most specific features of the VRS modes is the structure of the flow around the rotor

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Summary

Introduction

The steep descent modes belong to the most complex helicopter flight modes. This is due to the possible falling of the helicopter in the area of the VRS modes of the main rotor. In various flight tests, when a helicopter enters the area of the VRS modes, the following features have been noted: a loss of altitude, an increase in the required power, a high level of vibrations, irregular flywheel movement of the blades and a temporary loss of control of the helicopter. These effects are related to the specifics of the main rotor aerodynamics in the VRS modes

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