Thermodynamics of the hydration of non-polar substances

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Fältnamn	Indikatorer	Metadata
000		01584naa a2200313 4500
001		oai:DiVA.org:ri-26325
003		SwePub
008		161208s1998 \| \|\|\|\|\|\|\|\|\|\|\|000 \|\|eng\|
024	7	a https://urn.kb.se/resolve?urn=urn:nbn:se:ri:diva-263252 URI
040		a (SwePub)ri
041		a engb eng
042		9 SwePub
072	7	a ref2 swepub-contenttype
072	7	a art2 swepub-publicationtype
100	1	a Mancera, RL4 aut
245	1 0	a Thermodynamics of the hydration of non-polar substances
264	1	c 1998
338		a print2 rdacarrier
500		a A1190
520		a We re-examine the numerical value and physical significance of TS , the temperature where the entropy of transfer Δ WLCP fitting function. It is concluded that the interpretation of TS as the temperature where hydration ceases cannot be sustained. As previously reported [R.L. Baldwin, N. Muller, Proc. Natl. Acad. Sci. USA, 89 (1992) 7110], hydration must vanish at a temperature T1 >TS, where its experimental manifestation, i.e., ΔWL CP, is zero. We discuss the concept of water relaxation around a non-polar solute molecule and its relation to the hydration process.
653		a Hydrophobic effect
653		a Aqueous solutions
653		a Protein folding.
700	1	a Kronberg, Bu RISE,YKI – Ytkemiska institutet4 aut
700	1	a Costas, M4 aut
700	1	a Silveston, R4 aut
710	2	a RISEb YKI – Ytkemiska institutet4 org
773	0	t Biophysical Chemistryg 70, s. 57-63q 70<57-63x 0301-4622x 1873-4200
856	4 8	u https://urn.kb.se/resolve?urn=urn:nbn:se:ri:diva-26325

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