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Publications","issue":"1","license":[{"start":{"date-parts":[[2018,1,1]],"date-time":"2018-01-01T00:00:00Z","timestamp":1514764800000},"content-version":"tdm","delay-in-days":0,"URL":"https:\/\/journals.sagepub.com\/page\/policies\/text-and-data-mining-license"}],"content-domain":{"domain":["journals.sagepub.com"],"crossmark-restriction":true},"short-container-title":["Advances in Mechanical Engineering"],"published-print":{"date-parts":[[2018,1]]},"abstract":"<jats:p> In general, eccentric gravity machinery is a rotation mechanism with eccentric pendulum mechanism, which can be used to convert continuously kinetic energy generated by gravity energy to electric energy. However, a stable rotated velocity of the eccentric gravity machinery is difficult to be achieved only using gravity energy. In this article, a stable velocity control system applied to eccentric gravity machinery is proposed. The dynamic characteristic of eccentric gravity machinery is analyzed and its mathematical model is established, which is used to design the controller. A stable running velocity of the eccentric gravity machinery can be operated by the controlled servomotor. Due to disturbances being periodic, repetitive controller is installed to velocity control loop. The stability performance and control performance of the repetitive control system are discussed. The iterative algorithm of the repetitive control is executed by a digital signal processor TI TMS320C32 floating-point processor. Simulated and experimental results are reported to verify the performance of the proposed eccentric gravity machinery control system. <\/jats:p>","DOI":"10.1177\/1687814017751782","type":"journal-article","created":{"date-parts":[[2018,1,13]],"date-time":"2018-01-13T07:31:37Z","timestamp":1515828697000},"update-policy":"https:\/\/doi.org\/10.1177\/sage-journals-update-policy","source":"Crossref","is-referenced-by-count":0,"title":["Modeling and stabilization of eccentric gravity machinery"],"prefix":"10.1177","volume":"10","author":[{"ORCID":"https:\/\/orcid.org\/0000-0002-5317-3998","authenticated-orcid":false,"given":"Wu-Sung","family":"Yao","sequence":"first","affiliation":[{"name":"Department of Mechanical and Automation Engineering, National Kaohsiung First University of Science and Technology, Kaohsiung City, Taiwan"}]}],"member":"179","published-online":{"date-parts":[[2018,1,12]]},"reference":[{"key":"bibr1-1687814017751782","doi-asserted-by":"publisher","DOI":"10.1109\/87.865849"},{"key":"bibr2-1687814017751782","doi-asserted-by":"publisher","DOI":"10.1109\/28.833781"},{"key":"bibr3-1687814017751782","doi-asserted-by":"publisher","DOI":"10.1177\/1077546310384002"},{"key":"bibr4-1687814017751782","doi-asserted-by":"publisher","DOI":"10.1243\/09596518JSCE222"},{"key":"bibr5-1687814017751782","first-page":"311","volume":"42","author":"Zhao J","year":"2014","journal-title":"Control Intell 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Journal of Mechanical Engineering","issue":"19","content-domain":{"domain":[],"crossmark-restriction":false},"short-container-title":["Journal of Mechanical Engineering"],"published-print":{"date-parts":[[2019]]},"DOI":"10.3901\/jme.2019.19.028","type":"journal-article","created":{"date-parts":[[2020,1,18]],"date-time":"2020-01-18T21:53:36Z","timestamp":1579384416000},"page":"28","source":"Crossref","is-referenced-by-count":1,"title":["Operational Modal Identification for Rotating Machinery under Environment Excitation"],"prefix":"10.3901","volume":"55","author":[{"given":"LI","family":"Qihang","sequence":"first","affiliation":[]},{"given":"CHU","family":"Fulei","sequence":"first","affiliation":[]}],"member":"2265","container-title":["Journal of Mechanical 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Two different swirlers with flat and fillet sleeve structures (SWA and SWB) were adopted under fully confined and unconfined conditions for comparison. The velocity field characteristics were measured by 2D Particle Image Velocimetry (PIV), while the flame macrostructures were obtained by CH* chemiluminescence imaging. Distinctively, different types of flame shapes and flow field patterns were observed under fully confined and unconfined conditions and an evident transition of flow field topology from nonreacting to reacting cases related to the Coanda effect was only found in the SWB cases. The results show that the confined flames have a larger expansion angle than the unconfined, and the LBO limits (\u03d5LBO) shift to much higher equivalence ratios corresponding to better stability performance. Additionally, the \u03d5LBO characteristics present a slight difference between the SWA and SWB cases, and the Reynolds number (Re) also has a limited effect. Thus, wall confinement is a dominant factor that affects the flame topology and \u03d5LBO which should be considered in practical gas turbine applications.<\/jats:p>","DOI":"10.33737\/gpps21-tc-137","type":"proceedings-article","created":{"date-parts":[[2022,5,16]],"date-time":"2022-05-16T08:55:40Z","timestamp":1652691340000},"source":"Crossref","is-referenced-by-count":0,"title":["Effects Of Wall Confinement On The Flame Topology And Lean Blowout Characteristics In A Partially Premixed Single Swirl Gas Turbine Model Combustor"],"prefix":"10.33737","author":[{"name":"Key Laboratory for Power Machinery and Engineering of MOE, School of Mechanical Engineering, Shanghai Jiao Tong University","sequence":"first","affiliation":[]},{"given":"Xiaoxiang","family":"Shi","sequence":"first","affiliation":[]},{"given":"Zundi","family":"Liu","sequence":"additional","affiliation":[]},{"name":"Key Laboratory for Power Machinery and Engineering of MOE, School of Mechanical Engineering, Shanghai Jiao Tong University","sequence":"additional","affiliation":[]},{"given":"Zhongya","family":"Xi","sequence":"additional","affiliation":[]},{"name":"Key Laboratory for Power Machinery and Engineering of MOE, School of Mechanical Engineering, Shanghai Jiao Tong University","sequence":"additional","affiliation":[]},{"given":"Xiaoyuan","family":"Yang","sequence":"additional","affiliation":[]},{"name":"Key Laboratory for Power Machinery and Engineering of MOE, School of Mechanical Engineering, Shanghai Jiao Tong University","sequence":"additional","affiliation":[]},{"given":"Tianyou","family":"Lian","sequence":"additional","affiliation":[]},{"name":"Key Laboratory for Power Machinery and Engineering of MOE, School of Mechanical Engineering, Shanghai Jiao Tong University","sequence":"additional","affiliation":[]},{"given":"Vladimir","family":"Dulin","sequence":"additional","affiliation":[]},{"name":"Kutateladze Institute of Thermophysics, Novosibirsk 630090, Russia","sequence":"additional","affiliation":[]},{"given":"Leonid","family":"Chikishev","sequence":"additional","affiliation":[]},{"name":"Kutateladze Institute of Thermophysics, Novosibirsk 630090, Russia","sequence":"additional","affiliation":[]},{"given":"Dmitriy","family":"Markovich","sequence":"additional","affiliation":[]},{"name":"Kutateladze Institute of Thermophysics, Novosibirsk 630090, Russia","sequence":"additional","affiliation":[]},{"given":"Yuyang","family":"Li","sequence":"additional","affiliation":[]},{"name":"Kutateladze Institute of Thermophysics, Novosibirsk 630090, Russia","sequence":"additional","affiliation":[]}],"member":"19395","published-online":{"date-parts":[[2022,4,12]]},"event":{"name":"GPPS Xi'an21","acronym":"GPPS-TC-2021"},"container-title":["Proceedings of Global Power &amp; Propulsion Society"],"deposited":{"date-parts":[[2022,5,16]],"date-time":"2022-05-16T08:55:42Z","timestamp":1652691342000},"score":21.094614,"resource":{"primary":{"URL":"https:\/\/gpps.global\/wp-content\/uploads\/2022\/01\/GPPS-TC-2021_paper_137.pdf"}},"issued":{"date-parts":[[2022,4,12]]},"references-count":0,"URL":"https:\/\/doi.org\/10.33737\/gpps21-tc-137","ISSN":["2504-4400"],"issn-type":[{"type":"print","value":"2504-4400"}],"published":{"date-parts":[[2022,4,12]]}}],"items-per-page":20,"query":{"start-index":0,"search-terms":"Mechanical+engineering+and+machinery"}}}