Lorentz-Dirac方程式之限制條件
| dc.citation.epage | =O66-1 | en_US |
| dc.citation.spage | 61 | en_US |
| dc.citation.volume | 3 | en_US |
| dc.contributor.author | 鄭國順 | zh_TW |
| dc.contributor.author | K.S.Cheng | en_US |
| dc.date.accessioned | 2017-10-06T06:22:49Z | |
| dc.date.available | 2017-10-06T06:22:49Z | |
| dc.date.issued | 1977-09 | en_US |
| dc.description.abstract | Baylis and Hushilt pointed out that the Lorentz-Dirac equation with the usual constraint(ẍμ(τ)→0 as τ→∞) for physical solution, may permit two or more solutions to some problems. We impose another constriant to make the physical solution unique. | en_US |
| dc.identifier.journal | 交通大學學報 | zh_TW |
| dc.identifier.journal | The Journal of National Chiao Tung University | en_US |
| dc.identifier.uri | https://ir.lib.nycu.edu.tw/handle/11536/137594 | |
| dc.language.iso | en_US | en_US |
| dc.publisher | 交大學刊編輯委員會 | zh_TW |
| dc.title | Lorentz-Dirac方程式之限制條件 | zh_TW |
| dc.title | Constraints of the Lorentz-Dirac Equation | en_US |
| dc.type | Campus Publications | en_US |