On the Use of Pressure Distributions to Model the Hydrodynamics of Air-Cushion Vehicles and Surface-Effect Ships

1993 ◽  
Vol 105 (2) ◽  
pp. 69-89 ◽  
Author(s):  
LAWRENCE J. DOCTORS
1963 ◽  
Vol 67 (636) ◽  
pp. 755-756 ◽  
Author(s):  
A. E. Bingham

The phrase “Air-Cushioned Vehicle” describes the complete range of vehicles which obtain some or all of their support from a free pressurised cushion of air contained between the vehicle and the ground.Vickers’ interest in air cushion vehicles stems directly from the basic work carried out on the Hovercraft—one type of air cushion vehicle—by Mr. C. S. Cockerell and the initiative and encouragement displayed by the N.R.D.C. through its subsidiary Hovercraft Development Ltd.


2012 ◽  
Vol 152-154 ◽  
pp. 560-567 ◽  
Author(s):  
Ahmed S. Sowayan ◽  
Khalid A. Alsaif

A model for compressible Air Cushion Vehicles (ACV) is presented. In this model the compressible Bernoulli's equation and the Newton's second law of motion are used to predict the dynamic behavior of the heave response of the ACV in both time and frequency domains. The mass flow rate inside the air cushion of this model is assumed to be constant. The self excited response and the cushion pressure of the ACV is calculated to understand the behavior of the system in order to assist in the design stage of such systems. It is shown in this study that the mass flow rate and the length of the vehicle's skirt are the most significant parameters which control the steady state behavior of the self excited oscillations of the ACV. An equation to predict the transient time of the oscillatory response or the settling time in terms of the system parameters of the ACV is developed. Based on the developed equations, the optimum parameters of the ACV that lead to minimum settling time are obtained.


1989 ◽  
Author(s):  
PETER INCH ◽  
MARK PRENTICE ◽  
CAROL LEWIS

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