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Chemical Protein Unfolding – A Simple Cooperative Model
[Image: see text] Chemical unfolding with guanidineHCl or urea is a common method to study the conformational stability of proteins. The analysis of unfolding isotherms is usually performed with an empirical linear extrapolation method (LEM). A large positive free energy is assigned to the native pr...
Autores principales: | , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
American Chemical Society
2023
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Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10561279/ https://www.ncbi.nlm.nih.gov/pubmed/37735883 http://dx.doi.org/10.1021/acs.jpcb.3c03558 |
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author | Seelig, Joachim Seelig, Anna |
author_facet | Seelig, Joachim Seelig, Anna |
author_sort | Seelig, Joachim |
collection | PubMed |
description | [Image: see text] Chemical unfolding with guanidineHCl or urea is a common method to study the conformational stability of proteins. The analysis of unfolding isotherms is usually performed with an empirical linear extrapolation method (LEM). A large positive free energy is assigned to the native protein, which is usually considered to be a minimum of the free energy. The method thus contradicts common expectations. Here, we present a multistate cooperative model that addresses specifically the binding of the denaturant to the protein and the cooperativity of the protein unfolding equilibrium. The model is based on a molecular statistical–mechanical partition function of the ensemble, but simple solutions for the calculation of the binding isotherm and the associated free energy are presented. The model is applied to 23 published unfolding isotherms of small and large proteins. For a given denaturant, the binding constant depends on temperature and pH but shows little protein specificity. Chemical unfolding is less cooperative than thermal unfolding. The cooperativity parameter σ is at least 2 orders of magnitude larger than that of thermal unfolding. The multistate cooperative model predicts zero free energy for the native protein, which becomes strongly negative beyond the midpoint concentration of unfolding. The free energy to unfold a cooperative unit corresponds exactly to the diffusive energy of the denaturant concentration gradient necessary for unfolding. The temperature dependence of unfolding isotherms yields the denaturant-induced unfolding entropy and, in turn, the unfolding enthalpy. The multistate cooperative model provides molecular insight and is as simple to apply as the LEM but avoids the conceptual difficulties of the latter. |
format | Online Article Text |
id | pubmed-10561279 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2023 |
publisher | American Chemical Society |
record_format | MEDLINE/PubMed |
spelling | pubmed-105612792023-10-10 Chemical Protein Unfolding – A Simple Cooperative Model Seelig, Joachim Seelig, Anna J Phys Chem B [Image: see text] Chemical unfolding with guanidineHCl or urea is a common method to study the conformational stability of proteins. The analysis of unfolding isotherms is usually performed with an empirical linear extrapolation method (LEM). A large positive free energy is assigned to the native protein, which is usually considered to be a minimum of the free energy. The method thus contradicts common expectations. Here, we present a multistate cooperative model that addresses specifically the binding of the denaturant to the protein and the cooperativity of the protein unfolding equilibrium. The model is based on a molecular statistical–mechanical partition function of the ensemble, but simple solutions for the calculation of the binding isotherm and the associated free energy are presented. The model is applied to 23 published unfolding isotherms of small and large proteins. For a given denaturant, the binding constant depends on temperature and pH but shows little protein specificity. Chemical unfolding is less cooperative than thermal unfolding. The cooperativity parameter σ is at least 2 orders of magnitude larger than that of thermal unfolding. The multistate cooperative model predicts zero free energy for the native protein, which becomes strongly negative beyond the midpoint concentration of unfolding. The free energy to unfold a cooperative unit corresponds exactly to the diffusive energy of the denaturant concentration gradient necessary for unfolding. The temperature dependence of unfolding isotherms yields the denaturant-induced unfolding entropy and, in turn, the unfolding enthalpy. The multistate cooperative model provides molecular insight and is as simple to apply as the LEM but avoids the conceptual difficulties of the latter. American Chemical Society 2023-09-22 /pmc/articles/PMC10561279/ /pubmed/37735883 http://dx.doi.org/10.1021/acs.jpcb.3c03558 Text en © 2023 The Authors. Published by American Chemical Society https://creativecommons.org/licenses/by/4.0/Permits the broadest form of re-use including for commercial purposes, provided that author attribution and integrity are maintained (https://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Seelig, Joachim Seelig, Anna Chemical Protein Unfolding – A Simple Cooperative Model |
title | Chemical Protein
Unfolding – A Simple Cooperative
Model |
title_full | Chemical Protein
Unfolding – A Simple Cooperative
Model |
title_fullStr | Chemical Protein
Unfolding – A Simple Cooperative
Model |
title_full_unstemmed | Chemical Protein
Unfolding – A Simple Cooperative
Model |
title_short | Chemical Protein
Unfolding – A Simple Cooperative
Model |
title_sort | chemical protein
unfolding – a simple cooperative
model |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC10561279/ https://www.ncbi.nlm.nih.gov/pubmed/37735883 http://dx.doi.org/10.1021/acs.jpcb.3c03558 |
work_keys_str_mv | AT seeligjoachim chemicalproteinunfoldingasimplecooperativemodel AT seeliganna chemicalproteinunfoldingasimplecooperativemodel |