20 research outputs found
Computational Study of Peptide Plane Stacking with Polar and Ionizable Amino Acid Side Chains
Parallel
and T-shaped stacking interactions of the peptide plane
with polar and ionizable amino acid side chains (including aspartic/glutamic
acid, asparagine/glutamine, and arginine) are investigated using the
quantum mechanical MP2 and CCSD computational methods. It is found
that the electrostatic interaction plays an essential role in determining
the optimal stacking configurations for all investigated stacking
models. For certain complexes, the dispersion interaction also contributes
considerably to stacking. In the gas phase, the stacking interaction
of the charged system is stronger than that of the neutral system,
and T-shaped stacking is generally more preferred than parallel stacking,
with the stacking energy in the range of −4 to −18 kcal/mol.
The solvation effect overall weakens stacking, especially for the
charged system and the T-shaped stacking configurations. In water,
the interaction energies of different stacking models are comparable
Liquid Crystalline Phase of G-Tetrad DNA for NMR Study of Detergent-Solubilized Proteins
Liquid Crystalline Phase of G-Tetrad DNA for NMR Study of Detergent-Solubilized Protein
A Mechanistic Study of Trichoderma reesei Cel7B Catalyzed Glycosidic Bond Cleavage
An
ONIOM study is performed to illustrate the mechanism of Trichoderma reesei Cel7B catalyzed <i>p</i>-nitrophenyl lactoside hydrolysis. In both the glycosylation and
deglycosylation steps, the reaction proceeds in a concerted way, meaning
the nucleophilic attack and the glycosidic bond cleavage occur simultaneously.
The glycosylation step is rate limiting with a barrier of 18.9 kcal/mol,
comparable to the experimental value derived from the <i>k</i><sub>cat</sub> measured in this work. The function of four residues
R108, Y146, Y170, and D172, which form a hydrogen-bond network involving
the substrate, is studied by conservative mutations. The mutants,
including R108K, Y146F, Y170F, and D172N, decrease the enzyme activity
by about 150–8000-fold. Molecular dynamics simulations show
that the mutations disrupt the hydrogen-bond network, cause the substrate
to deviate from active binding and hinder either the proton transfer
from E201 to O<sub>4</sub>(+1) or the nucleophilic attack from E196
to C<sub>1</sub>(−1)
The Slowdown of the Endoglucanase <i>Trichoderma reesei</i> Cel5A-Catalyzed Cellulose Hydrolysis Is Related to Its Initial Activity
One
important
feature of hydrolysis of cellulose by cellulases is that the reaction
slows down quickly after it starts. In this work, we investigate the
slowdown mechanism at the early stage of the reaction using endoglucanase <i>Tr</i>. Cel5A-catalyzed phosphate acid-swollen cellulose
(PASC) hydrolysis as a model system. Specifically, we focus on the
effect of enzyme adsorption on the reaction slowdown. Nineteen single
mutations are introduced (with the assistance of molecular dynamics
simulations) to perturb the enzyme PASC interaction, yielding the
adsorption partitioning coefficient <i>K</i><sub>r</sub> that ranged from 0.12 to 0.39 L/g, compared to that of the wild
type (0.26 L/g). Several residues,
including T18, K26, Y26, H229, and T300, are demonstrated to be important
for adsorption of the enzyme to PASC. The kinetic measurements show
that the slowdown of the hydrolysis is not correlated with the adsorption
quantified by the partitioning coefficient <i>K</i><sub>r</sub> but is anticorrelated with the initial activity. This result
suggests that the mutants with higher activity are more prone to being
trapped or deplete the most reactive substrate faster and the adsorption
plays no apparent role in the reaction slowdown. The initial activity
of Cel5A against PASC is correlated with the enzyme specific activity
against a soluble substrate <i>p</i>-nitrophenyl cellobioside
The Impact of Hydrogen Bonding on Amide <sup>1</sup>H Chemical Shift Anisotropy Studied by Cross-Correlated Relaxation and Liquid Crystal NMR Spectroscopy
Site-specific <sup>1</sup>H chemical shift anisotropy (CSA) tensors have been derived for the well-ordered backbone amide moieties in the B3 domain of protein G (GB3). Experimental input data include residual chemical shift anisotropy (RCSA), measured in six mutants that align differently relative to the static magnetic field when dissolved in a liquid crystalline Pf1 suspension, and cross-correlated relaxation rates between the <sup>1</sup>H<sup>N</sup> CSA tensor and either the <sup>1</sup>H−<sup>15</sup>N, the <sup>1</sup>H−<sup>13</sup>C′, or the <sup>1</sup>H−<sup>13</sup>C<sup>α</sup> dipolar interactions. Analyses with the assumption that the <sup>1</sup>H<sup>N</sup> CSA tensor is symmetric with respect to the peptide plane (three-parameter fit) or without this premise (five-parameter fit) yield very similar results, confirming the robustness of the experimental input data, and that, to a good approximation, one of the principal components orients orthogonal to the peptide plane. <sup>1</sup>H<sup>N</sup> CSA tensors are found to deviate strongly from axial symmetry, with the most shielded tensor component roughly parallel to the N−H vector, and the least shielded component orthogonal to the peptide plane. DFT calculations on pairs of <i>N</i>-methyl acetamide and acetamide in H-bonded geometries taken from the GB3 X-ray structure correlate with experimental data and indicate that H-bonding effects dominate variations in the <sup>1</sup>H<sup>N</sup> CSA. Using experimentally derived <sup>1</sup>H<sup>N</sup> CSA tensors, the optimal relaxation interference effect needed for narrowest <sup>1</sup>H<sup>N</sup> TROSY line widths is found at ∼1200 MHz
Quinary Interactions Weaken the Electric Field Generated by Protein Side-Chain Charges in the Cell-like Environment
The intramolecular
electric field (e-field) generated by protein
GB3 side-chain charges K/E10, K/E19, and D/K40 was measured in the
absence or presence of macromolecular crowding. The e-field responds
differently to different crowding agentsî—¸dextran, Ficoll, BSA,
and <i>E. coli</i> cell lysate. Dextran and Ficoll have
no effect on the e-field. The lysate generally weakens the e-field
but the amplitude of weakening varies greatly. For example, the e-field
by K19 is reduced by 67% in the presence of 90 g/L lysate, corresponding
to a charge change from 0.9 to 0.3 e for K19, whereas the e-fields
by D/K40 are weakened only by ∼7% under the same lysate concentration.
The extent of the e-field weakening by BSA is in between that by Ficoll
(dextran) and lysate. Further investigations suggest that the e-field
weakening mechanism by lysate is similar to that by NaCl. That is,
the e-field generated by a protein surface charge affects the distribution
of lysate which creates a reaction field and weakens the protein e-field.
Our study indicates that the protein electrostatic property can be
changed significantly due to quinary interaction with the cell environment
Direct Observation of CH/CH van der Waals Interactions in Proteins by NMR
van der Waals interactions are important
to protein stability and
function. These interactions are usually identified empirically based
on protein 3D structures. In this work, we performed a solution nuclear
magnetic resonance (NMR) spectroscopy study of van der Waals interactions
by detecting the through-space <sup>vdw</sup><i>J</i><sub>CC</sub>-coupling between protein aliphatic side chain groups. Specifically, <sup>vdw</sup><i>J</i><sub>CC</sub>-coupling values up to ∼0.5
Hz were obtained between the methyl and nearby aliphatic groups in
protein GB3, providing direct experimental evidence for the van der
Waals interactions. Quantum mechanical calculations suggest that the <i>J</i>-coupling is correlated with the exchange-repulsion term
of van der Waals interaction. NMR detection of <sup>vdw</sup><i>J</i><sub>CC</sub>-coupling offers a new tool to characterize
such interactions in proteins
Carboxyl–Peptide Plane Stacking Is Important for Stabilization of Buried E305 of Trichoderma reesei Cel5A
Hydrogen
bonds or salt bridges are usually formed to stabilize
the buried ionizable residues. However, such interactions do not exist
for two buried residues D271 and E305 of Trichoderma
reesei Cel5A, an endoglucanase. Mutating D271 to alanine
or leucine improves the enzyme thermostability quantified by the temperature <i>T</i><sub>50</sub> due to the elimination of the desolvation
penalty of the aspartic acid. However, the same mutations for E305
decrease the enzyme thermostability. Free energy calculations based
on the molecular dynamics simulation predict the thermostability of
D271A, D271L, and E305A (compared to WT) in line with the experimental
observation but overestimate the thermostability of E305L. Quantum
mechanical calculations suggest that the carboxyl–peptide plane
stacking interactions occurring to E305 but not D271 are important
for the carboxyl group stabilization. For the protonated carboxyl
group, the interaction energy can be as much as about −4 kcal/mol
for parallel stacking and about −7 kcal/mol for T-shaped stacking.
For the deprotonated carboxyl group, the largest interaction energies
for parallel stacking and T-shaped stacking are comparable, about
−7 kcal/mol. The solvation effect generally weakens the interaction,
especially for the charged system. A search of the carboxyl–peptide
plane stacking in the PDB databank indicates that parallel stacking
but not T-shaped stacking is quite common, and the most probable distance
between the two stacking fragments is close to the value predicted
by the QM calculations. This work highlights the potential role of
carboxyl amide π–π stacking in the stabilization
of aspartic acid and glutamic acid in proteins
Protein Apparent Dielectric Constant and Its Temperature Dependence from Remote Chemical Shift Effects
A NMR protocol is introduced that
permits accurate measurement
of minute, remote chemical shift perturbations (CSPs), caused by a
mutation-induced change in the electric field. Using protein GB3 as
a model system, <sup>1</sup>H<sup>N</sup> CSPs in K19A and K19E mutants
can be fitted to small changes in the electric field at distal sites
in the protein using the Buckingham equation, yielding an apparent
dielectric constant ε<sub>a</sub> of 8.6 ± 0.8 at 298 K.
These CSPs, and their derived ε<sub>a</sub> value, scale strongly
with temperature. For example, CSPs at 313 K are about ∼30%
smaller than those at 278 K, corresponding to an effective ε<sub>a</sub> value of about 7.3 at 278 K and 10.5 at 313 K. Molecular
dynamics simulations in explicit solvent indicate that solvent water
makes a significant contribution to ε<sub>a</sub>
Engineering a More Thermostable Blue Light Photo Receptor <i>Bacillus subtilis</i> YtvA LOV Domain by a Computer Aided Rational Design Method
<div><p>The ability to design thermostable proteins offers enormous potential for the development of novel protein bioreagents. In this work, a combined computational and experimental method was developed to increase the <i>T</i><sub>m</sub> of the flavin mononucleotide based fluorescent protein <i>Bacillus Subtilis</i> YtvA LOV domain by 31 Celsius, thus extending its applicability in thermophilic systems. Briefly, the method includes five steps, the single mutant computer screening to identify thermostable mutant candidates, the experimental evaluation to confirm the positive selections, the computational redesign around the thermostable mutation regions, the experimental reevaluation and finally the multiple mutations combination. The adopted method is simple and effective, can be applied to other important proteins where other methods have difficulties, and therefore provides a new tool to improve protein thermostability.</p></div