TY - JOUR
T1 - An “Add-On” Analysis of Large Open Circularcylindrical Cavities
AU - Kastner, Raphael
AU - Twig, Yigal
N1 - Funding Information:
Manuscript received July 20, 1992; revised August 9, 1993. This work was supported in part by the Israel Academy of the Sciences and Humanities under contract no. 45/89-3. The authors are with the Department of Electrical Engineering, Physical Electronics. Tel Aviv University, Tel Aviv 69978, Israel. IEEE Log Number 9215653.
PY - 1994/2
Y1 - 1994/2
N2 - The add-on method utilizes previously acquired solutions for subproblems, comprising portions of a scatterer, as a part of the analysis. The process of adding the remainder of the solution is a relatively efficient one, assuming that the initial stage of the subproblem has been performed. The “add on” method is based on two basic principles: A. Superposition is used to break up the unknown current into two components, the first one being a readily computable solution to a simple short circuited problem, and the second one is excited by a current source over the aperture area, and is the only one requiring computation. B. A gradual algorithm is used for the computation of the second current component for many subproblems. Principle A leads to a purely algebraic algorithm of principle B, with no integral operators. In this work, this formulation is extended to the cylindrical case. In this case, the aperture region is a portion of a circle complementing the circular conducting shell, thus it shrinks as the conductor increases in size and no truncation is needed. The short circuit current for the closed circular cylinder is computed rapidly using the FFT. The cylindrical problem is solved for large cylinders in three ways: 1. A direct Moment Method solution, 2. A direct spatial decomposition solution based on the MoM matrix and invoking the matrix partitioning technique, 3. The cylindrical add-on scheme. All solutions are identical, however, the computational advantage of the add-on technique is quite apparent, as seen from the analysis of the operation count as well as from numerical examples.
AB - The add-on method utilizes previously acquired solutions for subproblems, comprising portions of a scatterer, as a part of the analysis. The process of adding the remainder of the solution is a relatively efficient one, assuming that the initial stage of the subproblem has been performed. The “add on” method is based on two basic principles: A. Superposition is used to break up the unknown current into two components, the first one being a readily computable solution to a simple short circuited problem, and the second one is excited by a current source over the aperture area, and is the only one requiring computation. B. A gradual algorithm is used for the computation of the second current component for many subproblems. Principle A leads to a purely algebraic algorithm of principle B, with no integral operators. In this work, this formulation is extended to the cylindrical case. In this case, the aperture region is a portion of a circle complementing the circular conducting shell, thus it shrinks as the conductor increases in size and no truncation is needed. The short circuit current for the closed circular cylinder is computed rapidly using the FFT. The cylindrical problem is solved for large cylinders in three ways: 1. A direct Moment Method solution, 2. A direct spatial decomposition solution based on the MoM matrix and invoking the matrix partitioning technique, 3. The cylindrical add-on scheme. All solutions are identical, however, the computational advantage of the add-on technique is quite apparent, as seen from the analysis of the operation count as well as from numerical examples.
UR - http://www.scopus.com/inward/record.url?scp=0028368611&partnerID=8YFLogxK
U2 - 10.1109/8.277220
DO - 10.1109/8.277220
M3 - ???researchoutput.researchoutputtypes.contributiontojournal.article???
AN - SCOPUS:0028368611
SN - 0018-926X
VL - 42
SP - 255
EP - 260
JO - IEEE Transactions on Antennas and Propagation
JF - IEEE Transactions on Antennas and Propagation
IS - 2
ER -