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Since the dipole moment is small, CO is categorized as nonpolar.
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When the solvent density is low enough, the density derivative of βΔμ at constant temperature has the same sign as ∫d x {1-exp[-βv (x)] }, where x is the solvent configuration relative to the solute and v (x) is the solute-solvent interaction. The excluded volume region, where v (x) is very large, always makes a positive contribution to the density derivative of βΔμ. The density derivative is reduced by the attractive (negative) portion of v (x), and is not necessarily positive at low temperatures. In Table I and Fig. 2, the density derivative of βΔμ of a polar solute is negative at 400°C in the low-density region. In other words, 400°C is not high enough in the sense that the contribution from the attractive part of the solute-solvent interaction is not overwhelmed by that from the repulsive part. It should be noted that the attractive contribution is more sensitive to the temperature variation than the repulsive contribution and that the repulsive contribution dominates at a high enough temperature.
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It is a rather rough statement that the density corresponding to the minimum βΔμ is larger when the solute-water interaction is stronger. Indeed, the interaction strength is not a uniquely definable concept, but expresses the "intuitive feeling" about the molecule.
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22944446353
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3 when the extrapolation to 400°C is performed. In this view, the extrapolated βΔW at 400°C is in good agreement with the corresponding βΔW value given by Figs. 5 and 8.
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