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Fast Folding Dynamics of Proteins

Proteins are polymers (or "chains") of amino acids, usually from dozens to hundreds of amino acids long. If DNA is the code for life, then proteins are life: they provide structure (collagen in the skin, for example), mobility (in muscle fibers), and as enzymes, they keep the engines of life going. Remarkably, as Christian Anfinsen showed many decades ago, the unique sequence of amino acids of each protein encodes its three-dimensional structure. Although chaperonins (other proteins!) have evolved to help misfolded or large unwieldy proteins escape from incorrectly folded "traps", proteins are not meticulously assembled - they can do the assembly job by-and-large by themselves.

How proteins fold and misfold is of great medical interest, as many diseases originate from proteins not doing their job correctly, often because of a mutation (a single amino acid that has been substituted by a different one because of an error in the DNA coding for the protein). Young-onset Alzheimer's disease and sickle cell anemia are but two of thousands of examples of such protein diseases. For this reason, how proteins fold - or fail to fold - is a subject of great current interest. The forces that hold proteins together or structure them, such as hydrophobicity, hydrogen bonding, van der Waals contacts, or salt bridges, are less simple and less directional than chemical bonds, and have complicated the development of protein folding models and experiments to test them.

Some of these diseases involve the aggregation of many proteins into sheet-like structures (beta sheets), first proposed by Linus Pauling in the 1930s. It is usually thought that these sheets require nucleation (a certain minimum size must form before the continue to grow spontaneously). Whether nucleation is needed or not, we have shown in a paper in J. Am. Chem. Soc. that pieces of this sheet-like structure exist in unfolded proteins at elevated temperature (say a 102 degree fever!), predisposing even the individual protein towards the formation of beta sheets.

Many years ago, Cyrus Levinthal stated that proteins cannot fold by randomly trying out all possible conformations, or shapes. It would simply take too long. In fact, proteins turn out to be extremely efficient at folding. We have engineered proteins in our lab that can fold in a matter of microseconds. While protein folding in textbooks has been treated as an ordinary chemical reaction, with unfolded and folded states separated by a free energy barrier, it appears that some proteins can fold downhill without such barriers. It appears that the mutations necessary to improve folding and eliminate the barrier are often detrimental to the function of the protein. Evolution has to simultaneously optimize both a protein's function and its ability to fold, and a compromise may be necessary between these two aspects of a protein.

In our experiments, we unfold wild-type and genetically engineered proteins by cooling to low temperatures (cold denaturation). Folding is then initiated by laser-jumping the temperature of the aqueous protein sample back up in a few nanoseconds. Alternatively, temperature-jump initiated unfolding may also be studied by taking folded proteins and jumping them up. Fluorescence lifetime detection tells us about the environment near amino acids such as tryptophan, the time evolution of fluorescence wavelength tells us about solvation, and the time evolution of infrared spectra tells us about the formation of hydrogen bonds and secondary structure. More details can be found in the clickable highlights of some recent publications shown below, or in the papers in the reference section of this website.

 

 

 

 

 

Publication Highlights

 

Feng Liu and Martin Gruebele, J. Mol. Biol. 370, 574-584 (2007)
Copyright © 2007 Elsevier B.V.

 

R.F. Service. Science 273:29-30 (1996)
Copyright © 1996 by the American Association for the Advancement of Science
http://www.sciencemag.org/cgi/content/summary/273/5271/29

R.M. Ballew, et. al. PNAS 93:5759-5764 (1996)
Copyright © 1996 by the National Academy of Sciences
http://www.pnas.org/cgi/content/abstract/93/12/5759

 

 

H. Ma and M. Gruebele. PNAS 102:2283-2287 (2005)
Copyright © 2005 by the National Academy of Sciences
http://www.pnas.org/cgi/content/full/102/7/2283

 

W. Yang and M. Gruebele. Nature 423:193-197 (2003)
Copyright © 2003 Nature Publishing Group
http://www.nature.com/nature/archive/IssueYear2003.html

 

 

W. Yang and M. Gruebele. Biophysical Journal 87:596-608 (2004)
Copyright © 2004 by the Biophysical Society
http://www.biophysj.org/cgi/content/abstract/87/1/596

 

E. K. Wilson. Chemical & Engineering News 82:35-40 (2004)
Copyright © 2004 American Chemical Society
http://pubs.acs.org/cen/coverstory/8239/8239computers.html

W. Yang et. al. J. Mol. Biol. 336:241-251 (2004)
Copyright © 2004 Elsevier B.V. All rights reserved.
http://www.elsevier.com/wps/find/journaldescription.cws_home/622890/description#description

 

W.Yang and M. Gruebele. JACS 126:7758-7759 (2004)
Copyright © 2004 American Chemical Society
http://pubs.acs.org/cgi-bin/article.cgi/jacsat/2004/126/i25/abs/ja0493751.html

 

PNAS link

W.A.Eaton. PNAS 96:5897-5899 (1999)
Copyright © 1999 by the National Academy of Sciences
http://www.pnas.org/cgi/content/full/96/11/5897

J. Sabelko, et. al. PNAS 96:6031-6036 (1999)
Copyright © 1999 by the National Academy of Sciences
http://www.pnas.org/cgi/content/full/96/11/6031

 

C. D. Snow, et. al. Nature 420:102-107 (2002)
Copyright © 2002 Nature Publishing Group
http://www.nature.com/cgi-taf/DynaPage.taf?file=/nature/journal/v420/n6911/abs/nature01160_fs.html

 

 


Nanosecond Temperature-Jump Apparatus

Rapid (<7ns) temperature-jumps in aqueous protein solutions are achieved by heating the protein solution with nanosecond infrared laser pulses. These heating pulses are created by Raman shifting the fundamental of a nanosecond Nd:YAG laser (1064 nm) in a hydrogen cell to produce 1.9 micrometer wavelength laser pulses, which are absorbed by water. Protein folding is then monitored in real time by collecting laser induced fluorescence from the protein's tryptophan residues once every 14 ns, or by collecting infrared light in the 1500-1800 inverse centimeter frequency range transmitted through the protein sample.


 

Simultaneous Detection of Fluorescence Lifetime and Dispersed Fluorescence

In addition to obtaining fluorescence lifetimes and integrated fluorescence intensities by collecting individual fluorescence transients, we can also simultaneously collect wavelength resolved emission spectra every 200 ns. Time resolved emission spectra can provide complimentary information about the solvent exposure of fluorescent chromophores.


Data Collection Scheme
Key:
LG LT - light guide lifetime
LG DF - light guide dispersed fluorescence
IRF - instrument response function
UV - UV probe beam produced by tripling the output of a Ti:Saph laser
IR - IR (1540 nm) heating pulse produced by Raman shifting the Nd:YAG fundamental
PMT - photomultiplier tube

The temperature jump experiment.

 

Group members Sharlene Denos, Feng Liu, and Seung Joong Kim in the wet lab.

   
     
   
     
 
Gruebele Group
University of Illinois at Urbana-Champaign
A214 Chemical and Life Sciences Lab
600 S Mathews Avenue RAL 29A
Urbana, Illinois 61801, USA

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University of Illinois

  Funding for this research is currently provided by the NSF, ACS, NASA, HFSP, IBM and UIUC.