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The Outstanding Excellences of Interactive Energy Density Topology Change Method

Received: 3 March 2024     Accepted: 18 March 2024     Published: 2 April 2024
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Abstract

It has not been solved that the fruits, vegetables, strawberries, cells, blood and a bottle of liquor are damaged, broken during transportation. It is the greatest factor in this situation that there is a danger vibration frequency band where these are easy to scratch and are prone to death. If there are eigen frequencies within this danger frequency band, it needs that those eigen frequencies within this danger frequency band are moved out of the band. In the former paper, it was shown difficult to apply the existing topology optimization methods using homogenization method or density method to control plural eigen frequencies for solving this problem. Therefore in the former paper, it was proposed the so called “Interactive Energy Density Topology (IEDT) change method” that is a new high precision and high efficiency method for controlling plural eigen frequencies simultaneously referring to the kinetic and the strain energy density distributions. Here it is discussed more about the IEDT change method and show that it is sometimes difficult for the traditional methods to get solutions because especially in the dynamic problem, eigen frequencies may go up or down depending on its size even if reinforcement or hall for change topology is applied at the same location. But with the proposed IEDT change method, always it can be realized because the proposed method has wider solution spaces than the traditional one. Lastly, it is shown that this IEDT method is also very effective to reduce the integral value of response curve by frequency.

Published in International Journal of Mechanical Engineering and Applications (Volume 12, Issue 2)
DOI 10.11648/j.ijmea.20241202.11
Page(s) 37-49
Creative Commons

This is an Open Access article, distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution and reproduction in any medium or format, provided the original work is properly cited.

Copyright

Copyright © The Author(s), 2024. Published by Science Publishing Group

Keywords

IEDT Change Method, Frequency Response, Topology Optimization, Density Method, Index of Generalized Eigen Frequency, Kinetic Energy Density, Strain Energy Density, Danger Frequency Band

References
[1] Sasaki, T., Yang, Y., Hagiwara, I., Proposition of a New High Speed and High Efficiency Control Method for Plural Eigen Frequencies by Change Topology, International Journal of Mechanical Engineering and Applications 10(6), 2022-11, pp. 135-143.
[2] Sasaki, T., Hagiwara, I., Proposition of an energy density topology change method for plural eigen frequencies control, Transactions of the JSME (in Japanese), Vol. 89, No. 927 (2023),
[3] Bendsoe, M. P. and Kikuchi, N., Generating Optimal Topologies in Structural Design using a Homogenization method, Computer Methods in Applied Mechanics and Engineering, 71, (1988), pp. 197-224.
[4] Suzuki, K. and Kikuchi, N., A homogenization method for shape and topology optimization, Computer Methods in Applied Mechanics and Engineering, Volume 93, (1991), pp. 291-318.
[5] Ma, Z. D., Kikuchi, N., Cheng, H. C. and Hagiwara, I., Development of Structural Optimization Method for Vibration Reduction (1st Report, Structural Optimization Theory Using the Homogenization Method), JSME Series C, Vol. 59, No. 562 (1993-6), pp. 1730-1736 (in Japanese).
[6] Tenek, L. H., Hagiwara, I., Static and Vibrational Shape and Topology Optimization Using Homogenization and Mathematical Programming. Computer Methods in Applied Mechanics and Engineering, 109, (1993) pp. 143-154.
[7] Torigaki, T., Hagiwara, I., Kitagawa, Y., Ueda, M., Ma, Z. D., Kikuchi, N., Development and Application of a Shape-Topology Optimization System Using a Homogenization Method, SAE International Congress and Exposition. (1994-3).
[8] Ma, Z. D., Kikuchi, N., Hagiwara, I., Torigaki, T., Development of Structural Optimization Method for Vibration Reduction, (2nd Report, An Improved Algorithm for the Optimization Problem), JSME Series C, Vol. 60, No. 577 (1994-9), pp. 3018-3024 (in Japanese).
[9] Ma, Z. D., Kikuchi, N., Cheng, H. C., Hagiwara, I., Topological Optimization Technique for Free Vibration Problems, ASME Journal of Applied Mechanics, Vol. 62 (1995-3), pp. 201-207.
[10] Hassani B., Hinton, E., A review of homogenization and topology optimization I—homogenization theory for media with periodic structure, Computers & Structures, Volume 69, Issue 6, December 1998, pp. 707-717.
[11] Allaire, G., Cavallina, L., Miyake, N., Oka, T., Yachimura, T., The Homogenization Method for Topology Optimization of Structures: Old and New, JOURNAL FREE ACCESS, 2019 Volume 25 Issue 2 Pages 75-146.
[12] Tenek, L. H., Hagiwara, I., Optimal plate and shell topologies using thickness distribution or homogenization, Computer Methods in Applied Mechanics and Engineering, Vol. 115 Nos. 1 & 2 (1994), pp. 111-124.
[13] Fujii, D., Suzuki, K., Otsubo, H., Filtering method for topology optimization analysis using optimality criteria method, The Architectural Institute of Japan's Journal of Structural and Construction Engineering, No. 543(2001), pp. 105-112(in Japanese).
[14] Kishida, M., Kurahashi, T., Consideration on numerical parameters in density update equation used in the density base topology optimization, Bulletin of the Japan Society for Computational Methods in Engineering, Vol. 21, Paper No. 03-211218 (2021), pp. 17-26 (in Japanese).
[15] Nishio, Y., Liu, Y., Ono, N., Boundary shape identification method for density based topology optimization, Transactions of the JSME (in Japanese), Vol. 88, No. 914 (2022),
[16] Mike, J. D., Powell, A., Direct search optimization method that models the objective and constraint functions by linear interpolation”, Proc. Sixth Workshop on Optimization and Numerical Analysis, Vol. 275, pp. 51-67, Kluwer Academic Publishers, Dordrecht, NL, 1994.
[17] COMSOL Multiphysics® v. 5. 5.
[18] Kozukue, W., Hagiwara, I., Vehicle Interior Noise Reduction Analysis Using Sound Pressure Level Integral Sensitivity, JSME, series C, Vol. 59, No. 568 (1993-12), pp. 3845-3851 (in Japanese).
[19] Kozukue, W., Hagiwara, I., Vehicle Interior Noise Reduction Analysis Using Sound Pressure Level Integral Sensitivity, JSME, series C, Vol. 61, No. 586 (1995-7), pp. 2746-2752 (in Japanese).
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  • APA Style

    Yang, Y., Sasaki, T., Abe, A., Hagiwara, I. (2024). The Outstanding Excellences of Interactive Energy Density Topology Change Method. International Journal of Mechanical Engineering and Applications, 12(2), 37-49. https://doi.org/10.11648/j.ijmea.20241202.11

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    ACS Style

    Yang, Y.; Sasaki, T.; Abe, A.; Hagiwara, I. The Outstanding Excellences of Interactive Energy Density Topology Change Method. Int. J. Mech. Eng. Appl. 2024, 12(2), 37-49. doi: 10.11648/j.ijmea.20241202.11

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    AMA Style

    Yang Y, Sasaki T, Abe A, Hagiwara I. The Outstanding Excellences of Interactive Energy Density Topology Change Method. Int J Mech Eng Appl. 2024;12(2):37-49. doi: 10.11648/j.ijmea.20241202.11

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  • @article{10.11648/j.ijmea.20241202.11,
      author = {Yang Yang and Toshie Sasaki and Aya Abe and Ichiro Hagiwara},
      title = {The Outstanding Excellences of Interactive Energy Density Topology Change Method
    },
      journal = {International Journal of Mechanical Engineering and Applications},
      volume = {12},
      number = {2},
      pages = {37-49},
      doi = {10.11648/j.ijmea.20241202.11},
      url = {https://doi.org/10.11648/j.ijmea.20241202.11},
      eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ijmea.20241202.11},
      abstract = {It has not been solved that the fruits, vegetables, strawberries, cells, blood and a bottle of liquor are damaged, broken during transportation. It is the greatest factor in this situation that there is a danger vibration frequency band where these are easy to scratch and are prone to death. If there are eigen frequencies within this danger frequency band, it needs that those eigen frequencies within this danger frequency band are moved out of the band. In the former paper, it was shown difficult to apply the existing topology optimization methods using homogenization method or density method to control plural eigen frequencies for solving this problem. Therefore in the former paper, it was proposed the so called “Interactive Energy Density Topology (IEDT) change method” that is a new high precision and high efficiency method for controlling plural eigen frequencies simultaneously referring to the kinetic and the strain energy density distributions. Here it is discussed more about the IEDT change method and show that it is sometimes difficult for the traditional methods to get solutions because especially in the dynamic problem, eigen frequencies may go up or down depending on its size even if reinforcement or hall for change topology is applied at the same location. But with the proposed IEDT change method, always it can be realized because the proposed method has wider solution spaces than the traditional one. Lastly, it is shown that this IEDT method is also very effective to reduce the integral value of response curve by frequency.
    },
     year = {2024}
    }
    

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  • TY  - JOUR
    T1  - The Outstanding Excellences of Interactive Energy Density Topology Change Method
    
    AU  - Yang Yang
    AU  - Toshie Sasaki
    AU  - Aya Abe
    AU  - Ichiro Hagiwara
    Y1  - 2024/04/02
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    DO  - 10.11648/j.ijmea.20241202.11
    T2  - International Journal of Mechanical Engineering and Applications
    JF  - International Journal of Mechanical Engineering and Applications
    JO  - International Journal of Mechanical Engineering and Applications
    SP  - 37
    EP  - 49
    PB  - Science Publishing Group
    SN  - 2330-0248
    UR  - https://doi.org/10.11648/j.ijmea.20241202.11
    AB  - It has not been solved that the fruits, vegetables, strawberries, cells, blood and a bottle of liquor are damaged, broken during transportation. It is the greatest factor in this situation that there is a danger vibration frequency band where these are easy to scratch and are prone to death. If there are eigen frequencies within this danger frequency band, it needs that those eigen frequencies within this danger frequency band are moved out of the band. In the former paper, it was shown difficult to apply the existing topology optimization methods using homogenization method or density method to control plural eigen frequencies for solving this problem. Therefore in the former paper, it was proposed the so called “Interactive Energy Density Topology (IEDT) change method” that is a new high precision and high efficiency method for controlling plural eigen frequencies simultaneously referring to the kinetic and the strain energy density distributions. Here it is discussed more about the IEDT change method and show that it is sometimes difficult for the traditional methods to get solutions because especially in the dynamic problem, eigen frequencies may go up or down depending on its size even if reinforcement or hall for change topology is applied at the same location. But with the proposed IEDT change method, always it can be realized because the proposed method has wider solution spaces than the traditional one. Lastly, it is shown that this IEDT method is also very effective to reduce the integral value of response curve by frequency.
    
    VL  - 12
    IS  - 2
    ER  - 

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