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Acceleration of the Multi-Level Fast Multipole Algorithm using Double Interpolation Technique

이중 보간 기법을 이용한 MLFMA 가속기법

  • Yun, Dal-Jae (Advanced Instrumentation Institute, Korea Research Institute of Standards and Science) ;
  • Kim, Hyung-Ju (Radio Resource Research Group, Electronics and Telecommunications Research Institute) ;
  • Lee, Jae-In (School of Electrical Engineering, Korea Advanced Institute of Science and Technology) ;
  • Yang, Seong-Jun (School of Electrical Engineering, Korea Advanced Institute of Science and Technology) ;
  • Yang, Woo-Yong (Naval MFR Team, Hanwha Systems) ;
  • Bae, Jun-Woo (Naval MFR Team, Hanwha Systems) ;
  • Myung, Noh-Hoon (School of Electrical Engineering, Korea Advanced Institute of Science and Technology)
  • 윤달재 (한국표준과학연구원 첨단측정장비연구소) ;
  • 김형주 (한국전자통신연구원 전파자원연구그룹) ;
  • 이재인 (한국과학기술원 전기 및 전자공학부) ;
  • 양성준 (한국과학기술원 전기 및 전자공학부) ;
  • 양우용 (한화시스템(주) 해상MFR팀) ;
  • 배준우 (한화시스템(주) 해상MFR팀) ;
  • 명로훈 (한국과학기술원 전기 및 전자공학부)
  • Received : 2018.11.29
  • Accepted : 2019.04.26
  • Published : 2019.06.05

Abstract

This paper proposes an acceleration of the multi-level fast multipole algorithm(MLFMA) by using a double interpolation method. The MLFMA has been primarily used to conduct scattering analysis of electrically large targets, e.g. stealth aircraft. In the MLFMA, radiation functions of each basis functions are first precomputed, and then aggregated. After transfer calculations for the aggregations, each interaction is disaggregated, and then received in the testing function. The key idea of the proposed method is to decrease the sampling rates of the radiation and receiving functions. The computational complexity of the unit sphere integration in terms of the testing functions is thus highly alleviated. The remaining insufficient sampling rate is then complemented by using additional interpolation. We demonstrate the performance of the proposed method through radar cross-section(RCS) calculations for realistic aircraft.

Keywords

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Fig. 1. Flow chart of the matrix vector product calculations in MLFMA

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Fig. 2. Flow chart of the MVP calculations in the proposed MLFMA

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Fig. 3. Target geometry of the canonical flare CAD model

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Fig. 4. The monostatic RCS of the flare CAD model

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Fig. 5. The number of iterations for the flare CAD model

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Fig. 6. Target geometry of the B-2 stealth CAD model

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Fig. 7. The monostatic RCS of the B-2 stealth CAD model

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Fig. 8. The number of iterations for the B-2 stealth CAD model

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Fig. 9. The number of iterations as a function of the number of basis in the unit sphere CAD model

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Fig. 10. The computation time per iteration as a function of the number of basis in the unit sphere CAD model

Table 1. The computational complexity improvements of the reference and proposed MLFMA

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Table 2. The average number of iterations and total computation time of the reference and proposed MLFMA in the flare simulation

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Table 3. The average number of iterations and total computation time of the reference and proposed MLFMA in the B-2 stealth simulation

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Table 4. The NRMSD value, average number of iterations, and total computation time of the proposed MLFMA in terms of S' value

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Table 5. The computation time per iteration of the reference and proposed MLFMA

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