TY - JOUR
T1 - Solvent accessibility in folded proteins. Studies of hydrogen exchange in trypsin
AU - Woodward, C. K.
AU - Ellis, Lynda B
AU - Rosenberg, A.
N1 - Copyright:
Copyright 2004 Elsevier B.V., All rights reserved.
PY - 1975
Y1 - 1975
N2 - In a native protein, the exchange of a peptide amide proton with solvent occurs by one of two pathways, either directly from the folded protein, or via unfolding, the exchange taking place from the unfolded protein. From the thermal unfolding rate constants, the contribution of unfolding to the overall kinetics as a function of solvent and temperature was determined. Exchange involving unfolding of the protein is characterized by a high activation energy, in the range of 50 to 60 Cal per mol. The activation energy (E[app]) of the rates of exchange directly from the folded protein is approximately 20 to 25 Cal/mol. Because for the protein transfer step, E[app] is approximately 20 Cal per mol, the activation energy for any contributing protein conformational process(es) is approximately equal to 5 Cal/mol. Most, if not all, of the peptide amide protons in a folded protein can exchange directly with solvent without the protein unfolding. The number of 'slowly' exchanging protons at a given condition of pH and temperature is not related to a discrete structural unit, but rather to the distribution of observed rates within the broader distribution of actual rates. The large attenuation of hydrogen exchange rates in folded proteins, resulting in a distribution of first order rates over 6 orders of magnitude, is primarily due to the effects of restricted solvent accessibility of labile protons in the three dimensional structure. Any protein conformational process, such as protein fluctuations, invoked to explain the solvent accessibility must be of low activation energy and attenuated by ethanol and other cosolvents.
AB - In a native protein, the exchange of a peptide amide proton with solvent occurs by one of two pathways, either directly from the folded protein, or via unfolding, the exchange taking place from the unfolded protein. From the thermal unfolding rate constants, the contribution of unfolding to the overall kinetics as a function of solvent and temperature was determined. Exchange involving unfolding of the protein is characterized by a high activation energy, in the range of 50 to 60 Cal per mol. The activation energy (E[app]) of the rates of exchange directly from the folded protein is approximately 20 to 25 Cal/mol. Because for the protein transfer step, E[app] is approximately 20 Cal per mol, the activation energy for any contributing protein conformational process(es) is approximately equal to 5 Cal/mol. Most, if not all, of the peptide amide protons in a folded protein can exchange directly with solvent without the protein unfolding. The number of 'slowly' exchanging protons at a given condition of pH and temperature is not related to a discrete structural unit, but rather to the distribution of observed rates within the broader distribution of actual rates. The large attenuation of hydrogen exchange rates in folded proteins, resulting in a distribution of first order rates over 6 orders of magnitude, is primarily due to the effects of restricted solvent accessibility of labile protons in the three dimensional structure. Any protein conformational process, such as protein fluctuations, invoked to explain the solvent accessibility must be of low activation energy and attenuated by ethanol and other cosolvents.
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M3 - Article
C2 - 234428
AN - SCOPUS:0016651412
SN - 0021-9258
VL - 250
SP - 432
EP - 439
JO - Journal of Biological Chemistry
JF - Journal of Biological Chemistry
IS - 2
ER -