Please use this identifier to cite or link to this item:
https://open.uns.ac.rs/handle/123456789/13101
DC Field | Value | Language |
---|---|---|
dc.contributor.author | Vujanović B. | en |
dc.date.accessioned | 2020-03-03T14:51:03Z | - |
dc.date.available | 2020-03-03T14:51:03Z | - |
dc.date.issued | 1981-01-01 | en |
dc.identifier.issn | 00207225 | en |
dc.identifier.uri | https://open.uns.ac.rs/handle/123456789/13101 | - |
dc.description.abstract | This paper exhibits a method of integrating Hamilton's canonical equations of motion by supposing that one component of the momentum vector can be represented as a field depending on time, generalized coordinates and the rest of the components of the momentum vector. The motion of a conservative or nonconservative dynamical system can be determined by purely algebraic operations if a complete solution of a quasi-linear partial differential equation is known. The method is knually suitable for initial and boundary value problems. © 1981. | en |
dc.relation.ispartof | International Journal of Engineering Science | en |
dc.title | On the integration of the nonconservative Hamilton's dynamical equations | en |
dc.type | Journal/Magazine Article | en |
dc.identifier.doi | 10.1016/0020-7225(81)90164-6 | en |
dc.identifier.scopus | 2-s2.0-0019659196 | en |
dc.identifier.url | https://api.elsevier.com/content/abstract/scopus_id/0019659196 | en |
dc.relation.lastpage | 1747 | en |
dc.relation.firstpage | 1739 | en |
dc.relation.issue | 12 | en |
dc.relation.volume | 19 | en |
item.grantfulltext | none | - |
item.fulltext | No Fulltext | - |
Appears in Collections: | FTN Publikacije/Publications |
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