Super-transport of energy in ultra-short processes: implications to heat transfer, fluid dynamics and quantum mechanics

dc.contributor.authorKulish, V.V.
dc.date.accessioned2014-12-03T08:40:31Z
dc.date.available2014-12-03T08:40:31Z
dc.date.issued2008
dc.description.abstractPaper presented at the 6th International Conference on Heat Transfer, Fluid Mechanics and Thermodynamics, South Africa, 30 June - 2 July, 2008.en_US
dc.description.abstractThe paradox of instantaneous propagation of energy is intrinsic to the classical models of energy transport. This paradox becomes well-pronounced during ultra-short processes. To remove the paradox, phase-lagged models of energy transport have been proposed. The analysis of the solutions to the phaselagged energy equations suggests that when the characteristic time of the process is much less than the lag time, the wave mode of transport becomes the main mechanism of energy transfer. In ultra-short heat transfer processes, the wave transport is manifested by an apparent increase (three-four orders of magnitude) of the thermal conductivity of the transporting medium. In viscous fluid flow, in addition, an apparent decrease of viscosity occurs, so that the liquid behaves as superfluid even at high temperatures. It has been demonstrated that the lag time is inversely proportional to the temperature. Thus the life span of the supertransport phenomena should significantly increase at low temperatures, which is consistent with observing superfluids at lower temperatures for long periods of time. From the quantum physics standpoint, the energy transporting waves can be viewed as narrow wave packets, whose wave functions describe the superfluid state of the liquid. This may provide an alternative explanation of the phenomenon of superfluidity: the Bose-Einstein condensation may not be needed for superfluidity to occur. From the phase-lagged model of energy transport, it follows that the Schrödinger equation is but a zero-time-lag approximation. Hence, the phase-lagged Schrödinger equation must be used to describe ultra-short quantum interactions. It is suggested that the finiteness of Planck’s constant and the finiteness of the speed of energy propagation are not independent. This circumstance may shed some light on the understanding of processes that took place in the beginning of our Universe.en_US
dc.description.librarianvk2014en_US
dc.format.extent18 pagesen_US
dc.format.mediumPDFen_US
dc.identifier.citationKulish, VV 2008, Super-transport of energy in ultra-short processes: implications to heat transfer, fluid dynamics and quantum mechanics, Paper presented to the 6th International Conference on Heat Transfer, Fluid Mechanics and Thermodynamics, South Africa, 30 June - 2 July 2008.en_US
dc.identifier.isbn9781868546916
dc.identifier.urihttp://hdl.handle.net/2263/42770
dc.language.isoenen_US
dc.publisherInternational Conference on Heat Transfer, Fluid Mechanics and Thermodynamicsen_US
dc.relation.ispartofHEFAT 2008en_US
dc.rightsUniversity of Pretoriaen_US
dc.subjectSuper transport of energyen_US
dc.subjectUltra short processesen_US
dc.subjectHeat transferen_US
dc.subjectFluid dynamicsen_US
dc.subjectQuantum mechanicsen_US
dc.subjectPhase lagged models of energy transporten_US
dc.subjectWave mode of transporten_US
dc.subjectThermal conductivityen_US
dc.subjectViscous fluid flowen_US
dc.subjectSuper fluiden_US
dc.subjectNarrow wave pocketsen_US
dc.subjectSuperfluid stateen_US
dc.subjectBose-Einstein condensationen_US
dc.subjectSchrödinger equationen_US
dc.subjectUltra-short quantum interactionsen_US
dc.subjectPlanck’s constanten_US
dc.titleSuper-transport of energy in ultra-short processes: implications to heat transfer, fluid dynamics and quantum mechanicsen_US
dc.typePresentationen_US

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