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CHANNELS, RECEPTORS, AND ELECTRICAL SIGNALING |
1 Syracuse University
2 Texas A&M
3 Oxford University
* To whom correspondence should be addressed. E-mail: lmovilea{at}physics.syr.edu.
Submitted on December 3, 2004
Revised on December 26, 2004
Accepted on 23 May 2005
| Abstract |
|---|
-helical peptides between the bulk aqueous phase and the transmembrane
-barrel of the
-hemolysin (
HL) protein pore at the single-molecule level. The experimental kinetic data suggest a two-barrier, single-well free energy diagram for peptide transit through the
HL pore. This free energy profile is strongly voltage- and peptide length-dependent. We used the Woodhull-Eyring formalism to rationalize the values measured for the association and dissociation rate constants kon and koff, and to separate koff into individual rate constants for exit through each of the openings of the protein pore. The kinetic rate constants kon, koffcis and kofftrans decreased with the length of the peptide. At high transmembrane potentials, the alanine-based peptides, which include bulky lysine side chains, bind more strongly (formation constants Kf ~tens of M-1 than highly flexible poly(ethylene glycol)s (Kf ~ M-1)to the lumen of the
HL protein pore. In contrast, at zero transmembrane potential, the peptides bind weakly to the lumen of the
HL, and the binding decreases with the peptide length, similar to PEGs. The binding is enhanced at increased transmembrane potentials because
G= -
FV/RT predominates with the peptides. We suggest that the
HL protein may serve as a robust and versatile model for examining the interactions between positively charged signal peptides and a
-barrel pore.
Key Words: Driving force, Folding, Free energy barrier, Transmembrane pore, alfa-helical peptide, beta-barrel
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