Protein folding is a fundamental process in biology, key to understanding many human diseases. Experimentally, proteins often appear to fold via simple two- or three-state mechanisms involving mainly native-state interactions, yet recent network models built from atomistic simulations of small proteins suggest the existence of many possible metastable states and folding pathways. We reconcile these two pictures in a combined experimental and simulation study of acyl-coenzyme A-binding protein (ACBP), a two-state folder (folding time ~10 ms) exhibiting residual unfolded-state structure, and a putative early folding intermediate. Using single-molecule FRET in conjunction with side-chain mutagenises, we first demonstrate that the denatured state of ACBP at near-zero denaturant is unusually compact and enriched in long-range structure that can be perturbed by discrete hydrophobic core mutations. We then employ ultrafast laminar-flow mixing experiments to study the folding kinetics of ACBP on the microsecond timescale. These studies, along with with Trp-Cys quenching measurements of unfolded-state dynamics, suggest that unfolded-state structure forms on a surprisingly slow (~100 µs) timescale, and that sequence mutations strikingly perturb both time-resolved and equilibrium smFRET measurements in a similar way. A Markov State Model (MSM) of the ACBP folding reaction, constructed from over 30 milliseconds of molecular dynamics trajectory data, predicts a complex network of metastable stables, residual unfolded-state structure and kinetics consistent with experiment, but no well-defined intermediate preceding the main folding barrier. Taken together, these experimental and simulation results suggest that the previously characterized fast kinetic phase is not due to formation of a barrier-limited intermediate, but rather a more heterogeneous and slow acquisition of unfolded-state structure.
We have investigated the multidimensionality of the free energy landscape accessible to a nucleic acid hairpin by measuring the relaxation kinetics in response to two very different perturbations of the folding/unfolding equilibrium, either a laser temperature-jump or ion-jump (from rapid mixing with counterions). The two sets of measurements carried out on DNA hairpins (4 or 5 base pairs in the stem and 21-nucleotide polythymine loop), using FRET between end labels or fluorescence of 2-aminopurine in the stem as conformational probes, yield distinctly different relaxation kinetics in the temperature range 10-30 °C and salt range 100-500 mM NaCl, with rapid mixing exhibiting slower relaxation kinetics after an initial collapse of the chain within 8 μs of the counterion mixing time. The discrepancy in the relaxation times increases with increasing temperatures, with rapid mixing times nearly 10-fold slower than T-jump times at 30 °C. These results rule out a simple two-state scenario with the folded and unfolded ensemble separated by a significant free energy barrier, even at temperatures close to the thermal melting temperature T(m). Instead, our results point to the scenario in which the conformational ensemble accessed after counterion condensation and collapse of the chain is distinctly different from the unfolded ensemble accessed with T-jump perturbation. Our data suggest that, even at temperatures in the vicinity of T(m) or higher, the relaxation kinetics obtained from the ion-jump measurements are dominated by the escape from the collapsed state accessed after counterion condensation.
High-risk HPV is clearly associated with cervical cancer. HPV integration has been confirmed to promote carcinogenesis in the previous studies. In our study, a total of 285 DNA breakpoints and 287 RNA breakpoints were collected. We analyzed the characteristic of HPV integration in the DNA and RNA samples. The results revealed that the patterns of HPV integration in RNA and DNA samples differ significantly. FHIT, KLF5, and LINC00392 were the hotspot genes integrated by HPV in the DNA samples. RAD51B, CASC8, CASC21, ERBB2, TP63, TEX41, RAP2B, and MYC were the hotspot genes integrated by HPV in RNA samples. Breakpoints of DNA samples were significantly prone to the region of INTRON (P < 0.01, Chi-squared test), whereas in the RNA samples, the breakpoints were prone to EXON. Pathway analysis had revealed that the breakpoints of RNA samples were enriched in the pathways of transcriptional misregulation in cancer, cancer pathway, and pathway of adherens junction. Breakpoints of DNA samples were enriched in the pathway of cholinergic synapse. In summary, our data helped to gain insights into the HPV integration sites in DNA and RNA samples of cervical cancer. It had provided theoretical basis for understanding the mechanism of tumorigenesis from the perspective of HPV integration in the HPV-associated cervical cancers.
The defining property of two-state models of protein folding is that the measured relaxation rates are independent of the starting conditions and only depend on the final conditions. In this work we compare the kinetics of the very fast folding villin subdomain measured after a large change in denaturant concentration using an ultrarapid microfluidic mixer with the kinetics measured after a small temperature change in a laser T-jump experiment and find a significant difference in the observed folding kinetics. The final conditions of temperature and denaturant concentration and the use of tryptophan fluorescence as a probe are the same in both experiments, while the initial conditions are very different. The slower mixing kinetics show no evidence of the faster phase in T-jump experiments, which would support models of on- or off-pathway intermediates. Rather we interpret the combined mixer and T-jump experiments as evidence of an ensemble of unfolded states, some of which are traps. The ensemble after dilution from high denaturant is more expanded than the ensemble after an increase in temperature and, on average, takes longer to reach the native state.
To solve the problem that analyte molecules cannot easily enter "hot spots" on a conventional solid SERS substrate, we developed a mixing-assisted "hot spots" occupying (MAHSO) SERS strategy to improve utilization of "hot spots". Compared with the conventional substrate, the MAHSO substrate enhances the sensitivity of SERS measurement by thousands of times. The MAHSO substrate possesses excellent properties of high enhancement, high uniformity, and long-term stability because the MAHSO substrate is integrated inside an ultrafast microfluidic mixer. The mixer makes analytes and metal colloid homogeneously mixed, and analytes are naturally located in "hot spots", the gaps between adjacent NPs, during the process that NPs deposit on the channel wall. As a multi-inlet device, the MAHSO chip offers a convenient in situ method to study environmental effects on analytes or molecular interactions by flexibly regulating fluid in microchannels and monitoring responses of analytes by SERS spectra. Because all experiments are conducted in aqueous environments, which is similar to the physiological conditions, the MAHSO chip is especially suitable to be applied to study biomolecules. Using this strategy, different conformational changes of the wild type and mutant G150D of protein PMP22-TM4 depending on environmental pH have been observed in situ and analyzed. As a lab-on-a-chip (LoC) device, the MAHSO SERS chip will benefit the field of molecular dynamics, as well as molecule-molecule or molecule-surface interactions in the future.
β-CD modified plasmonic Pickering emulsions were synthesized for interfacial reaction monitoring as well as for kinetic study.
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