Titlebook: Van der Waals Forces and Shielding Effects; P. Diehl,E. Fluck,R. Kosfeld Conference proceedings 1975 Springer-Verlag Berlin · Heidelberg 1

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,σw in Dense Media,ith densities up to 300 amagats. Streever and Carr [.], and Hunt and Carr [.] report .. = -0.43 ppm/amagat at 25 °C. More recently, working with greater precision, Kanegsberg, Pass and Carr [.] found a distinct non-linearity, requiring a third virial term σ.. They also found a distinct temperature d

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,19F σw Studies, his co-workers has alsready been discussed in sections on the repulsion effect (section 7.2), the . parameter (section 9.6) and the temperature dependence of σ. (section 11.2). In the present chapter we will therefore only tabulate the experimental data.

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On the Required Molecular Parameters and Physical Constants,t without systematic errors; one will find that the temperature measured tends to depend on the amount of liquid in the thermocouple tube and on whether this tube is spun or not. The likely causes of these effects are temperature gradients over the sample (if the dewared insert is not of a countercu

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Conference proceedings 1975ther and even from one nu­ clear site to another in the same solute molecule. No referencing technique, however cleverly devised, will be capable of eliminating the Ow contribution from the other, presumedly more interesting contributions. It appeared quite recently that mathematical trickery by the

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干涉

The Physical Nature of the Field , and of the Associated Excitation Energy,In the foregoing several methods were described to evaluate the time-averaged square of the electric field as experienced by the solute. It is perhaps useful to stress that not only the . of evaluating . are different, but that in fact fields of quite different nature are evaluated with various methods.

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Van der Waals Forces and Shielding Effects978-3-642-66176-1Series ISSN 0170-5989