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dc.contributor.authorDean Karnopp
dc.date.accessioned2017-05-08T23:04:35Z
dc.date.available2017-05-08T23:04:35Z
dc.date.copyrightMarch, 1978
dc.date.issued1978
dc.identifier.issn0022-0434
dc.identifier.otherJDSMAA-26049#70_1.pdf
dc.identifier.urihttp://yetl.yabesh.ir/yetl/handle/yetl/90919
dc.description.abstractThe unification that bond graph methods bring to the representation of mechanical, electrical, magnetic, and chemical kinetic systems is not completely achieved for fluid flow systems except in the special case of high pressure hydraulic systems. This is because power in fluid systems is not merely the product of two variables such as pressure and volume flow rate, but rather contains components due to the convection of internal and kinetic energy. Using a Lagrangian description rather than the more usual Eulerian description, however, normal bond graph elements succeed in representing fluid and thermal interactions. The approach leads to novel ways of simulating systems in which convection is important. Variable transport delay and dispersion are handled in a way preserving physical intuition since fixed quantities of matter are followed through the system.
dc.publisherThe American Society of Mechanical Engineers (ASME)
dc.titleA Bond Graph Modeling Philosophy for Thermofluid Systems
dc.typeJournal Paper
dc.journal.volume100
dc.journal.issue1
dc.journal.titleJournal of Dynamic Systems, Measurement, and Control
dc.identifier.doi10.1115/1.3426342
dc.journal.fristpage70
dc.journal.lastpage75
dc.identifier.eissn1528-9028
dc.treeJournal of Dynamic Systems, Measurement, and Control:;1978:;volume( 100 ):;issue: 001
dc.contenttypeFulltext


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