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3, the magnitude of the T derivative of βΔw(r) above 100°C is less than ∼1/4 of that evaluated from the T variation from 25 to 100°C. From the thermodynamic point of view, however, it is legitimate to analyze the dependence of βΔw(r) on 1/T, rather than on T itself, and the 1/T derivative is less distinct below and above 100 °C than the T derivative. In the present paper, we compare βΔw(r) at a super-or subcritical temperature directly with that at a moderate temperature. Although this comparison is not thermodynamically systematic, it is helpful when a semiempirical model is to be developed for the aggregation of nonpolar solutes. The comparison is also useful from the operational point of view since the temperature elevation from 25 to 100°C is operationally much easier than the variation from 100°C to a supercritical temperature.
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3 at a fixed temperature of 400°C.
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0343983077
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note
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The linear dependence of βΔw(r) on the density ρ seen in Figure 3 is valid in the contact region expressed as 3.4 Å ≲ r ≲ 4.1 Å. The linearity is illustrated only at r = 3.7 Å for brevity.
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98
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3 is not large enough to cause a statistically significant change in βΔw(r).
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99
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0343983069
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note
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Our arguments are actually valid within the framework of the transition state theory.
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