Non-linear axisymmetric potential flow boundary model for partially cavitating high speed bodies
원문보기
IPC분류정보
국가/구분
United States(US) Patent
등록
국제특허분류(IPC7판)
G06G-007/48
G06G-007/50
출원번호
US-0874306
(2001-06-07)
발명자
/ 주소
Varghese, Abraham N.
Uhlman, James S.
출원인 / 주소
The United States of America as represented by the Secretary of the Navy
인용정보
피인용 횟수 :
3인용 특허 :
2
초록▼
A method for calculating parameters about an axisymmetric body in a cavity is provided. The user provides data describing the body, a cavity estimate, and convergence tolerances. Boundary element panels are distributed along the body and the estimated cavity. Matrices are initialized for each panel
A method for calculating parameters about an axisymmetric body in a cavity is provided. The user provides data describing the body, a cavity estimate, and convergence tolerances. Boundary element panels are distributed along the body and the estimated cavity. Matrices are initialized for each panel using disturbance potentials and boundary values. Disturbance potential matrices are formulated for each panel using disturbance potential equations and boundary conditions. The initialized matrices and the formulated matrices are solved for each boundary panel to obtain panel sources, dipoles and cavitation numbers. Forces and velocities are computed giving velocity and drag components. The cavity shape is updated by moving each panel in accordance with the calculated values. The method then tests for convergence against a tolerance, and iterates until convergence is achieved. Upon completion, parameters of interest and the cavity shape are provided. This invention also allows determiniation of cavity shape for a cavitation number.
대표청구항▼
1. A method for calculating parameters for an axisymmetric partially cavitating body having a cavitator located at the foremost end, said method comprising the steps of:receiving system parameter data including geometric data describing the axisymmetric body, a convergence tolerance, and an initial
1. A method for calculating parameters for an axisymmetric partially cavitating body having a cavitator located at the foremost end, said method comprising the steps of:receiving system parameter data including geometric data describing the axisymmetric body, a convergence tolerance, and an initial cavity shape including an endplate height, an endplate location, and a cavity length; initially distributing boundary element panels along the initial cavity shape, endplate and the axisymmetric body aft of the endplate; initializing matrices for each boundary element panel using the disturbance potentials at the boundary element panels and known boundary values; formulating disturbance potential matrices for each boundary element panel utilizing disturbance potential equations and no net flux boundary conditions; solving initialized matrices and formulated disturbance potential matrices for each boundary panel to obtain unknown panel sources, unknown dipoles and unknown cavitation numbers; computing forces and velocities at each panel from the panel sources, dipoles and cavitation numbers to obtain velocity components, pressure drag, viscous drag, and base drag; updating the cavity by moving each panel in accordance with the calculated forces and velocities and the boundary conditions; testing for convergence by comparing the movement of each panel against the convergence tolerance; iterating said steps of initializing matrices, formulating matrices, solving formulated matrices, computing forces and velocities, updating the cavity and testing for convergence when said test for convergence indicates that movement of at least one panel exceeds the convergence tolerance; computing parameters of interest when said test for convergence indicates that movement of all panels is within the convergence tolerance; and outputting the location of the cavity and the computed parameters. 2. The method of claim 1 wherein the step of computing parameters of interest comprises computing the pressure drag, the viscous drag, the base drag, the total drag, the cavitation number, the cavity length, the maximum cavity radius, and the cavity length to maximum radius location.3. The method of claim 2 wherein the output results step further includes outputting the cavity's disturbance potential, disturbance potential gradient, and pressure coefficient.4. The method of claim 3 wherein the output results step further comprises outputting all system parameter data, panel locations, and cavitation numbers for each iteration.5. The method of claim 1 wherein the updating the cavity step comprises the steps of:calculating the rotation of a boundary element panel necessary for satisfying the no flow boundary condition for a panel of interest starting with the boundary element panel closest to the cavitator; shifting the aft most point of the panel of interest in the radial direction for satisfying the calculated rotation; moving the foremost point of the next aftward panel to the same radius as the shifted aft most point of the panel of interest; and continuing calculating, shifting and moving for each panel foremost to aft most until the panel adjacent to the endplate is updated. 6. The method of claim 1 wherein the convergence tolerance comprises a maximum radial displacement for each panel.7. A method for calculating cavity length for an axisymmetric partially cavitating body having a cavitator located at the foremost end, said method comprising the steps of:receiving system parameter data including geometric data describing the axisymmetric body, a cavitation number, a convergence tolerance, a cavitation number tolerance, and an initial cavity shape including an endplate height, an endplate location, and a cavity length; initially distributing boundary element panels along the initial cavity shape, endplate and the axisymmetric body aft of the endplate; initializing matrices for each boundary element panel using the disturbance potentials at the boundary element panels utilizing known boundary values; formulating disturbance potential matrices for each boundary element panel utilizing disturbance potential equations and no net flux boundary conditions; solving initialized matrices and formulated disturbance potential matrices for each boundary panel to obtain unknown panel sources, unknown dipoles and unknown cavitation numbers; computing forces and velocities at each panel from the panel sources, dipoles and cavitation numbers to obtain velocity components, pressure drag, viscous drag, and base drag; updating the cavity by moving each panel in accordance with the calculated forces and velocities and the boundary conditions; testing for convergence by comparing the movement of each panel against the convergence tolerance; iterating said steps of initializing matrices, formulating matrices, solving formulated matrices, computing forces and velocities, updating the cavity and testing for convergence when said test for convergence indicates that movement of at least one panel exceeds the convergence tolerance; computing a current cavity and a current cavitation number when said test for convergence indicates that movement of all said panels are within the convergence tolerance; indicating cavitation number convergence when said current cavitation number is within the cavitation number tolerance from the received cavitation number; increasing said cavity length to provide a new cavity length when said current cavitation number is less than said received cavitation number beyond the cavitation number tolerance; decreasing said cavity length to provide a new cavity length when said current cavitation number is greater than said received cavitation number beyond the cavitation number tolerance; iterating the steps of initially distributing, initializing matrices, formulating disturbance potential matrices, solving initialized matrices and formulated disturbance potential matrices, computing forces and velocities, updating the cavity, testing for convergence, iterating, and computing a current cavity and a current cavitation number using said new cavity length when cavitation number convergence is not indicated; computing parameters of interest when cavitation number convergence is indicated; and outputting the location of the cavity and the computed parameters. 8. The method of claim 7 wherein the step of computing parameters of interest comprises computing the pressure drag, the viscous drag, the base drag, the total drag, the maximum cavity radius, and the cavity length to maximum radius location.9. The method of claim 8 wherein the output results step further includes outputting the cavity's disturbance potential, disturbance potential gradient, and pressure coefficient.10. The method of claim 9 wherein the output results step further comprises outputting all system parameter data, panel locations, and cavitation numbers for each iteration.11. The method of claim 7 wherein the updating the cavity step comprises the steps of:calculating the rotation of a boundary element panel necessary for satisfying the no flow boundary condition for a panel of interest starting with the boundary element panel closest to the cavitator; shifting the aft most point of the panel of interest in the radial direction for satisfying the calculated rotation; moving the foremost point of the next aftward panel to the same radius as the shifted aft most point of the panel of interest; and continuing calculating, shifting and moving for each panel foremost to aft most until the panel adjacent to the endplate is updated. 12. The method of claim 7 wherein the convergence tolerance comprises a maximum radial displacement for each panel.
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이 특허에 인용된 특허 (2)
Ruffa Anthony A., Acoustical cavitation suppressor for flow fields.
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