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The orientational-correlation time intercept in liquids
We propose a theory for the zero viscosity (η) or infinite temperature (T) intercept (τ0) in the much used quasihydrodynamic expression τ2=τ0+(const)(η/T) for the second rank orientational correlation time (τ2). Whereas we associate the (η/T) term with the integral over the torque–torque correlation...
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Published in: | The Journal of chemical physics 1986-01, Vol.84 (1), p.385-390 |
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Main Authors: | , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | We propose a theory for the zero viscosity (η) or infinite temperature (T) intercept (τ0) in the much used quasihydrodynamic expression τ2=τ0+(const)(η/T) for the second rank orientational correlation time (τ2). Whereas we associate the (η/T) term with the integral over the torque–torque correlation function, we attribute the origin of τ0 to the integral over the cross-correlation function between torques and kinetic or convective terms. We are unable to evaluate the time dependence of this cross-correlation function exactly, but if a Gaussian form is assumed, a negative value is obtained for τ0. Experimentally, τ0 is sometimes positive and sometimes negative, which suggests that a monotonic form for the time dependence of the cross-correlation function might be inadequate. Because we have not been able to evaluate this cross-correlation function our explanation must still be considered a conjecture. |
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ISSN: | 0021-9606 1089-7690 |
DOI: | 10.1063/1.450148 |