Characterization of the folding and unfolding reactions of a small beta-barrel protein of novel topology, the MTCP1 oncogene product P13

Citation
C. Roumestand et al., Characterization of the folding and unfolding reactions of a small beta-barrel protein of novel topology, the MTCP1 oncogene product P13, J MOL BIOL, 312(1), 2001, pp. 247-259
Citations number
33
Categorie Soggetti
Molecular Biology & Genetics
Journal title
JOURNAL OF MOLECULAR BIOLOGY
ISSN journal
00222836 → ACNP
Volume
312
Issue
1
Year of publication
2001
Pages
247 - 259
Database
ISI
SICI code
0022-2836(20010907)312:1<247:COTFAU>2.0.ZU;2-Y
Abstract
The equilibrium and kinetic folding properties of a small oncogene product, P13(MTCP1), of novel topology have been investigated using perturbation by guanidine hydrochloride and observation by fluorescence, circular dichrois m and two-dimensional heteronuclear NMR spectroscopy. The structure of P13( MTCP1) is comprised of a canonical filled beta -barrel, although the topolo gy of the structure is absolutely unique, rendering the folding properties of this protein of great interest. Equilibrium measurements of the intrinsi c fluorescence emission spectrum, the fluorescence decay, the circular dich roism spectrum and the N-15-H-1 heteronuclear single quantum coherence (HSQ C) correlation spectrum as a function of increasing concentrations of denat urant showed no evidence for the population of any equilibrium intermediate s, although negative amplitudes on the blue edge of the tryptophan emission and loss of intensity of the native HSQC correlation peaks were indicative of increased conformational dynamics at low denaturant concentrations. The free energy and cooperativity of unfolding as observed by fluorescence and circular dichroism were in relatively good agreement, also consistent with a two-state transition. Kinetics measurements of the fluorescence emission as a function of denaturant concentration revealed that P13(MTCP1) is the slowest folding beta -structure protein reported to date. Comparison of the activation cooperativity values (m(f) and m(u)) indicates that the structu re of the transition state is quite close to the folded state in terms of e xposed surface area. The calculated contact order of P13(MTCP1) is relative ly low and does not appear to explain its slow rate of folding. We suggest that the complex topology of this protein, which would require the ordering of the beta -barrel through a long loop joining the two L-shaped component s of the barrel, could provide an explanation for this slow folding.