RESUMEN
Fast protein folding involves complex dynamics in many degrees of freedom, yet microsecond folding experiments provide only low-resolution structural information. We enhance the structural resolution of the five-helix bundle protein λ6-85 by engineering into it three fluorescent tryptophan-tyrosine contact probes. The probes report on distances between three different helix pairs: 1-2, 1-3, and 3-2. Temperature jump relaxation experiments on these three mutants reveal two different kinetic timescales: a slower timescale for 1-3 and a faster one for the two contacts involving helix 2. We hypothesize that these differences arise from a single folding mechanism that forms contacts on different timescales, and not from changes of mechanism due to adding the probes. To test this hypothesis, we analyzed the corresponding three distances in one published single-trajectory all-atom molecular-dynamics simulation of a similar mutant. Autocorrelation analysis of the trajectory reveals the same "slow" and "fast" distance change as does experiment, but on a faster timescale; smoothing the trajectory in time shows that this ordering is robust and persists into the microsecond folding timescale. Structural investigation of the all-atom computational data suggests that helix 2 misfolds to produce a short-lived off-pathway trap, in agreement with the experimental finding that the 1-2 and 3-2 distances involving helix 2 contacts form a kinetic grouping distinct from 1 to 3. Our work demonstrates that comparison between experiment and simulation can be extended to several order parameters, providing a stronger mechanistic test.
Asunto(s)
Colorantes Fluorescentes/química , Pliegue de Proteína , Cinética , Simulación de Dinámica Molecular , Mutación , Triptófano/química , Tirosina/químicaRESUMEN
PEGylated proteins play an increasingly important role in pharmaceutical drug delivery. We recently showed that short poly(ethylene glycol) (PEG) chains can affect protein structure, even when they are not making extensive contact with the protein surface. In contrast, PEG is generally thought to form a relatively unstructured coil, and its compactness depends on solvent conditions. Here we test whether a host protein could allow PEG to form recurrent structural motifs while the PEG chain is in contact with the protein surface. We link a PEG oligomer (n = 45) to one of two nearly opposite locations on the small α-helical protein λ6-85 to investigate this question. We first demonstrate experimentally that in these particular positions, PEG does not significantly affect the thermodynamic stability or folding kinetics of λ6-85. We then use several all-atom molecular dynamics (MD) simulations 1 µs in duration to show how PEG equilibrates between states extending into the solvent and states packed onto the protein surface. The packing reveals recurring structures, including persistent hydrogen bond and hydrophobic contact patterns that appear multiple times. Some interactions of PEG with surface lysines are best described as an "intermittent slithering" motion of the PEG around the side chain, as seen in short MD movies. Thus, PEG achieves a variety of metastable organized structures on the protein surface, somewhere between a random globule and true folding. We also investigated the PEG-protein interaction in the unfolded state of the protein. We find that PEG has a propensity to stabilize certain helices of λ6-85, no matter which of the two positions it was attached to. Thus, sufficiently long PEG chains are organized by the protein surface and in turn interact with certain elements of protein structure more than others, even when PEG is attached to very different sites.
Asunto(s)
Simulación de Dinámica Molecular , Polietilenglicoles/química , Pliegue de Proteína , Proteínas Represoras/química , Proteínas Reguladoras y Accesorias Virales/química , Enlace de Hidrógeno , Interacciones Hidrofóbicas e Hidrofílicas , Cinética , Estructura Secundaria de ProteínaRESUMEN
Nanopores have become ubiquitous components of systems for single-molecule manipulation and detection, in particular DNA sequencing where electric field driven translocation of DNA through a nanopore is used to read out the DNA molecule. Here, we present a double-pore system where two nanopores are drilled in parallel through the same solid-state membrane, which offers new opportunities for DNA manipulation. Our experiments and molecular dynamics simulations show that simultaneous electrophoretic capture of a DNA molecule by the two nanopores mechanically traps the molecule, increasing its residence time within the nanopores by orders of magnitude. Remarkably, by using two unequal-sized nanopores, the pore of DNA entry and exit can be discerned from the ionic current blockades, and the translocation direction can be precisely controlled by small differences in the effective force applied to DNA. The mechanical arrest of DNA translocation using a double-pore system can be straightforwardly integrated into any solid-state nanopore platform, including those using optical or transverse-current readouts.
Asunto(s)
ADN/análisis , Simulación de Dinámica Molecular , Nanoporos , Análisis de Secuencia de ADNRESUMEN
Local modulation of temperature has emerged as a new mechanism for regulation of molecular transport through nanopores. Predicting the effect of such modulations on nanopore transport requires simulation protocols capable of reproducing non-uniform temperature gradients observed in experiment. Conventional molecular dynamics (MD) method typically employs a single thermostat for maintaining a uniform distribution of temperature in the entire simulation domain, and, therefore, can not model local temperature variations. In this article, we describe a set of simulation protocols that enable modeling of nanopore systems featuring non-uniform distributions of temperature. First, we describe a method to impose a temperature gradient in all-atom MD simulations based on a boundary-driven non-equilibrium MD protocol. Then, we use this method to study the effect of temperature gradient on the distribution of ions in bulk solution (the thermophoretic effect). We show that DNA nucleotides exhibit differential response to the same temperature gradient. Next, we describe a method to directly compute the effective force of a thermal gradient on a prototypical biomolecule-a fragment of double-stranded DNA. Following that, we demonstrate an all-atom MD protocol for modeling thermophoretic effects in solid-state nanopores. We show that local heating of a nanopore volume can be used to regulate the nanopore ionic current. Finally, we show how continuum calculations can be coupled to a coarse-grained model of DNA to study the effect of local temperature modulation on electrophoretic motion of DNA through plasmonic nanopores. The computational methods described in this article are expected to find applications in rational design of temperature-responsive nanopore systems.
RESUMEN
The abnormal assembly of misfolded proteins into neurotoxic aggregates is the hallmark associated with neurodegenerative diseases. Herein, we establish a photocontrollable platform to trigger amyloidogenesis to recapitulate the pathogenesis of amyotrophic lateral sclerosis (ALS) by applying a chemically engineered probe as a "switch" in live cells. This probe is composed of an amyloidogenic peptide from TDP-43, a photolabile linker, a polycationic sequence both to mask amyloidogenicity and for cell penetration, and a fluorophore for visualization. The photocontrollable probe can self-assemble into a spherical vesicle but rapidly develops massive nanofibrils with amyloid properties upon photoactivation. The photoinduced in vitro fibrillization process is characterized by biophysical techniques. In cellular experiments, this cell-penetrable vesicle was retained in the cytoplasm, seeded the mislocalized endogenous TDP-43 into aggregates upon irradiation, and consequently initiated apoptosis. In addition, this photocontrollable vesicle interfered with nucleocytoplasmic protein transport and triggered cortical neuron degeneration. Our developed strategy provides in vitro and in vivo spatiotemporal control of neurotoxic fibrillar aggregate formation, which can be readily applied in the studies of protein misfolding, aggregation-induced protein mislocalization, and amyloid-induced pathogenesis in different diseases.
RESUMEN
With the aim of developing a DNA sequencing methodology, we theoretically examine the feasibility of using nanoplasmonics to control the translocation of a DNA molecule through a solid-state nanopore and to read off sequence information using surface-enhanced Raman spectroscopy. Using molecular dynamics simulations, we show that high-intensity optical hot spots produced by a metallic nanostructure can arrest DNA translocation through a solid-state nanopore, thus providing a physical knob for controlling the DNA speed. Switching the plasmonic field on and off can displace the DNA molecule in discrete steps, sequentially exposing neighboring fragments of a DNA molecule to the pore as well as to the plasmonic hot spot. Surface-enhanced Raman scattering from the exposed DNA fragments contains information about their nucleotide composition, possibly allowing the identification of the nucleotide sequence of a DNA molecule transported through the hot spot. The principles of plasmonic nanopore sequencing can be extended to detection of DNA modifications and RNA characterization.
Asunto(s)
ADN/genética , Nanoporos , Análisis de Secuencia de ADN , Secuencia de Bases , ADN de Cadena Simple/genética , Simulación de Dinámica Molecular , Espectrometría RamanRESUMEN
PEGylation, or addition of poly(ethylene glycol) chains to proteins, is widely used to improve delivery in pharmaceutical applications. Recent studies suggest that stabilization of a protein by PEG, and hence its proteolytic degradability, is sequence-dependent and requires only short PEG chains. Here we connect stabilization by short PEG chains directly to the structural dynamics of the protein and PEG chain. We measured the stability of human Pin1 WW domain with PEG-4 at asparagine 19 for a full mutant cycle at two positions thought to influence PEG-protein interaction: Ser16Ala and Tyr23Phe. We then performed explicit solvent molecular dynamics simulations on all PEGylated and PEG-free mutants. The mutant cycle yields a nonadditive stabilization effect where the pseudo-wild type and double mutant are more stabilized relative to unPEGylated proteins than are the two single mutants. The simulation reveals why: the double mutant suffers loss of ß-sheet structure, which PEGylation restores even though the PEG extends as a coil into the solvent. In contrast, in one of the single mutants, PEG preferentially interacts with the protein surface while disrupting the interactions of its asparagine host with a nearby methionine side chain. Thus, PEG attachment can stabilize a protein differentially depending on the local sequence, and either by interacting with the surface or by extending into the solvent. A simulation with PEG-45 attached to asparagine 19 shows that PEG even can do both in the same context.