TY - JOUR
T1 - Thermal unfolding kinetics of ubiquitin in the microsecond-to-second time range probed by Tyr-59 fluorescence
AU - Santos, Maria Helena
N1 - Faria, Tiago Q. (ITQB)
PY - 2010/1/1
Y1 - 2010/1/1
N2 - Thermal folding/unfolding kinetics of wild-type ubiquitin (wt-UBQ) was studied in a wide time range, from microseconds to seconds, by combining rapid-mixing T-jump and laser T-jump with fluorescence detection (MTJ-F and LTJ-F, respectively) to monitor the fluorescence changes of Tyr-59 located on the 3(10)-helix. The kinetics occurs exclusively in the millisecond to second time range, and the decays are strictly single exponential. From global analysis of folding and unfolding decays, the k(f) and k(u) values were determined, without use of the equilibrium constant K. The activation enthalpy of folding is negative (Delta H-f(#)(T-m) = -10.8 kcal/mol), but the free energy of the transition state is substantially larger than that of the unfolded state (Delta G(f)(#)(T-m) = 7.6 kcal/mol >> RTm). Thus, wt-UBQ behaves as a two-state folder, when folding is monitored by the fluorescence of Tyr-59. The observation of kinetics on the microsecond time scale, when folding is monitored by the disruption of hydrogen bonds between beta-strands, using nonlinear infrared spectroscopy of the amide I vibrations (LTJ-DVE) [Chung, H. S.; Tokmakoff, A. Proteins: Struct., Funct., Bioinf 2008, 72, 474-487], seems to result from the fact that MTJ-F monitors the effective unfolding (backbone exposure to water) of the thermally excited protein alone, while LTJ-DVE also monitors preliminary events (hydrogen-bond breaking) and thermal re-equilibration of the thermally excited protein.
AB - Thermal folding/unfolding kinetics of wild-type ubiquitin (wt-UBQ) was studied in a wide time range, from microseconds to seconds, by combining rapid-mixing T-jump and laser T-jump with fluorescence detection (MTJ-F and LTJ-F, respectively) to monitor the fluorescence changes of Tyr-59 located on the 3(10)-helix. The kinetics occurs exclusively in the millisecond to second time range, and the decays are strictly single exponential. From global analysis of folding and unfolding decays, the k(f) and k(u) values were determined, without use of the equilibrium constant K. The activation enthalpy of folding is negative (Delta H-f(#)(T-m) = -10.8 kcal/mol), but the free energy of the transition state is substantially larger than that of the unfolded state (Delta G(f)(#)(T-m) = 7.6 kcal/mol >> RTm). Thus, wt-UBQ behaves as a two-state folder, when folding is monitored by the fluorescence of Tyr-59. The observation of kinetics on the microsecond time scale, when folding is monitored by the disruption of hydrogen bonds between beta-strands, using nonlinear infrared spectroscopy of the amide I vibrations (LTJ-DVE) [Chung, H. S.; Tokmakoff, A. Proteins: Struct., Funct., Bioinf 2008, 72, 474-487], seems to result from the fact that MTJ-F monitors the effective unfolding (backbone exposure to water) of the thermally excited protein alone, while LTJ-DVE also monitors preliminary events (hydrogen-bond breaking) and thermal re-equilibration of the thermally excited protein.
KW - STATE
KW - PROTEIN-FOLDING KINETICS
KW - IR SPECTROSCOPY
KW - STABILITY
KW - RESOLVED FLUORESCENCE
KW - TEMPERATURE-JUMP
KW - INTERMEDIATE
KW - FUNNELS
KW - DYNAMICS
KW - TRANSITION
U2 - 10.1021/jp104167h
DO - 10.1021/jp104167h
M3 - Article
SN - 1520-6106
VL - 114
SP - 9912
EP - 9919
JO - Journal of Physical Chemistry B
JF - Journal of Physical Chemistry B
IS - 30
ER -