Literature DB >> 22006304

Physical limits of cells and proteomes.

Ken A Dill1, Kingshuk Ghosh, Jeremy D Schmit.   

Abstract

What are the physical limits to cell behavior? Often, the physical limitations can be dominated by the proteome, the cell's complement of proteins. We combine known protein sizes, stabilities, and rates of folding and diffusion, with the known protein-length distributions P(N) of proteomes (Escherichia coli, yeast, and worm), to formulate distributions and scaling relationships in order to address questions of cell physics. Why do mesophilic cells die around 50 °C? How can the maximal growth-rate temperature (around 37 °C) occur so close to the cell-death temperature? The model shows that the cell's death temperature coincides with a denaturation catastrophe of its proteome. The reason cells can function so well just a few degrees below their death temperature is because proteome denaturation is so cooperative. Why are cells so dense-packed with protein molecules (about 20% by volume)? Cells are packed at a density that maximizes biochemical reaction rates. At lower densities, proteins collide too rarely. At higher densities, proteins diffuse too slowly through the crowded cell. What limits cell sizes and growth rates? Cell growth is limited by rates of protein synthesis, by the folding rates of its slowest proteins, and--for large cells--by the rates of its protein diffusion. Useful insights into cell physics may be obtainable from scaling laws that encapsulate information from protein knowledge bases.

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Year:  2011        PMID: 22006304      PMCID: PMC3207669          DOI: 10.1073/pnas.1114477108

Source DB:  PubMed          Journal:  Proc Natl Acad Sci U S A        ISSN: 0027-8424            Impact factor:   11.205


  59 in total

1.  Roles of native topology and chain-length scaling in protein folding: a simulation study with a Go-like model.

Authors:  N Koga; S Takada
Journal:  J Mol Biol       Date:  2001-10-12       Impact factor: 5.469

2.  Electrostatic contributions to the stability of a thermophilic cold shock protein.

Authors:  Huan-Xiang Zhou; Feng Dong
Journal:  Biophys J       Date:  2003-04       Impact factor: 4.033

Review 3.  Protein folding and misfolding.

Authors:  Christopher M Dobson
Journal:  Nature       Date:  2003-12-18       Impact factor: 49.962

4.  An electrostatic basis for the stability of thermophilic proteins.

Authors:  Brian N Dominy; Hervé Minoux; Charles L Brooks
Journal:  Proteins       Date:  2004-10-01

Review 5.  Hyperthermic biology and cancer therapies: a hypothesis for the "Lance Armstrong effect".

Authors:  Donald S Coffey; Robert H Getzenberg; Theodore L DeWeese
Journal:  JAMA       Date:  2006-07-26       Impact factor: 56.272

6.  Electrostatic interactions contribute to reduced heat capacity change of unfolding in a thermophilic ribosomal protein l30e.

Authors:  Chi-Fung Lee; Mark D Allen; Mark Bycroft; Kam-Bo Wong
Journal:  J Mol Biol       Date:  2005-04-29       Impact factor: 5.469

7.  The stability of salt bridges at high temperatures: implications for hyperthermophilic proteins.

Authors:  A H Elcock
Journal:  J Mol Biol       Date:  1998-11-27       Impact factor: 5.469

8.  How do thermophilic proteins and proteomes withstand high temperature?

Authors:  Lucas Sawle; Kingshuk Ghosh
Journal:  Biophys J       Date:  2011-07-06       Impact factor: 4.033

9.  Temperature of egg incubation determines sex in Alligator mississippiensis.

Authors:  M W Ferguson; T Joanen
Journal:  Nature       Date:  1982-04-29       Impact factor: 49.962

10.  Mistranslation-induced protein misfolding as a dominant constraint on coding-sequence evolution.

Authors:  D Allan Drummond; Claus O Wilke
Journal:  Cell       Date:  2008-07-25       Impact factor: 41.582

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  98 in total

1.  Profile of Ken A. Dill.

Authors:  Sujata Gupta
Journal:  Proc Natl Acad Sci U S A       Date:  2012-02-06       Impact factor: 11.205

2.  Optimal macromolecular density in the cell.

Authors:  Alexei Vazquez
Journal:  Proc Natl Acad Sci U S A       Date:  2012-02-17       Impact factor: 11.205

3.  Chain length determines the folding rates of RNA.

Authors:  Changbong Hyeon; D Thirumalai
Journal:  Biophys J       Date:  2012-02-07       Impact factor: 4.033

4.  A thermodynamic definition of protein domains.

Authors:  Lauren L Porter; George D Rose
Journal:  Proc Natl Acad Sci U S A       Date:  2012-05-25       Impact factor: 11.205

5.  Temperature is a key factor in Micromonas-virus interactions.

Authors:  David Demory; Laure Arsenieff; Nathalie Simon; Christophe Six; Fabienne Rigaut-Jalabert; Dominique Marie; Pei Ge; Estelle Bigeard; Stéphan Jacquet; Antoine Sciandra; Olivier Bernard; Sophie Rabouille; Anne-Claire Baudoux
Journal:  ISME J       Date:  2017-01-13       Impact factor: 10.302

6.  Ionic imbalance, in addition to molecular crowding, abates cytoskeletal dynamics and vesicle motility during hypertonic stress.

Authors:  Paula Nunes; Isabelle Roth; Paolo Meda; Eric Féraille; Dennis Brown; Udo Hasler
Journal:  Proc Natl Acad Sci U S A       Date:  2015-06-04       Impact factor: 11.205

7.  Diffusion within the cytoplasm: a mesoscale model of interacting macromolecules.

Authors:  Fabio Trovato; Valentina Tozzini
Journal:  Biophys J       Date:  2014-12-02       Impact factor: 4.033

Review 8.  Variation in transcriptome size: are we getting the message?

Authors:  Jeremy E Coate; Jeff J Doyle
Journal:  Chromosoma       Date:  2014-11-26       Impact factor: 4.316

9.  Thermal performance across levels of biological organization.

Authors:  Enrico L Rezende; Francisco Bozinovic
Journal:  Philos Trans R Soc Lond B Biol Sci       Date:  2019-06-17       Impact factor: 6.237

10.  Ribosomes are optimized for autocatalytic production.

Authors:  Shlomi Reuveni; Måns Ehrenberg; Johan Paulsson
Journal:  Nature       Date:  2017-07-19       Impact factor: 49.962

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