21 research outputs found
Site-Specific Internal Motions in GB1 Protein Microcrystals Revealed by 3D <sup>2</sup>H–<sup>13</sup>C–<sup>13</sup>C Solid-State NMR Spectroscopy
<sup>2</sup>H quadrupolar line shapes deliver rich information
about protein dynamics. A newly designed 3D <sup>2</sup>H–<sup>13</sup>C–<sup>13</sup>C solid-state NMR magic angle spinning
(MAS) experiment is presented and demonstrated on the microcrystalline
β1 immunoglobulin binding domain of protein G (GB1). The implementation
of <sup>2</sup>H–<sup>13</sup>C adiabatic rotor-echo-short-pulse-irradiation
cross-polarization (RESPIRATION CP) ensures the accuracy of the extracted
line shapes and provides enhanced sensitivity relative to conventional
CP methods. The 3D <sup>2</sup>H–<sup>13</sup>C–<sup>13</sup>C spectrum reveals <sup>2</sup>H line shapes for 140 resolved
aliphatic deuterium sites. Motional-averaged <sup>2</sup>H quadrupolar
parameters obtained from the line-shape fitting identify side-chain
motions. Restricted side-chain dynamics are observed for a number
of polar residues including K13, D22, E27, K31, D36, N37, D46, D47,
K50, and E56, which we attribute to the effects of salt bridges and
hydrogen bonds. In contrast, we observe significantly enhanced side-chain
flexibility for Q2, K4, K10, E15, E19, N35, N40, and E42, due to solvent
exposure and low packing density. T11, T16, and T17 side chains exhibit
motions with larger amplitudes than other Thr residues due to solvent
interactions. The side chains of L5, V54, and V29 are highly rigid
because they are packed in the core of the protein. High correlations
were demonstrated between GB1 side-chain dynamics and its biological
function. Large-amplitude side-chain motions are observed for regions
contacting and interacting with immunoglobulin G (IgG). In contrast,
rigid side chains are primarily found for residues in the structural
core of the protein that are absent from protein binding and interactions
<sup>1</sup>H‑Detected REDOR with Fast Magic-Angle Spinning of a Deuterated Protein
Rotational
echo double resonance (REDOR) is a highly successful
method for heteronuclear distance determination in biological solid-state
NMR, and <sup>1</sup>H detection methods have emerged in recent years
as a powerful approach to improving sensitivity and resolution for
small sample quantities by utilizing fast magic-angle spinning (>30
kHz) and deuteration strategies. In theory, involving <sup>1</sup>H as one of the spins for measuring REDOR effects can greatly increase
the distance measurement range, but few experiments of this type have
been reported. Here we introduce a pulse sequence that combines frequency-selective
REDOR (FSR) with <sup>1</sup>H detection. We demonstrate this method
with applications to samples of uniformly <sup>13</sup>C,<sup>15</sup>N,<sup>2</sup>H-labeled alanine and uniformly <sup>13</sup>C,<sup>2</sup>H,<sup>15</sup>N-labeled GB1 protein, back-exchanged with
30% H<sub>2</sub>O and 70% D<sub>2</sub>O, employing a variety of
frequency-selective <sup>13</sup>C pulses to highlight unique spectral
features. The resulting, robust REDOR effects provide (1) tools for
resonance assignment, (2) restraints of secondary structure, (3) probes
of tertiary structure, and (4) approaches to determine the preferred
orientation of aromatic rings in the protein core
Tissue Factor Residues That Modulate Magnesium-Dependent Rate Enhancements of the Tissue Factor/Factor VIIa Complex
The
blood coagulation cascade is initiated when the cell-surface
complex of factor VIIa (FVIIa, a trypsin-like serine protease) and
tissue factor (TF, an integral membrane protein) proteolytically activates
factor X (FX). Both FVIIa and FX bind to membranes via their Îł-carboxyglutamate-rich
domains (GLA domains). GLA domains contain seven to nine bound Ca<sup>2+</sup> ions that are critical for their folding and function, and
most biochemical studies of blood clotting have employed supraphysiologic
Ca<sup>2+</sup> concentrations to ensure saturation of these domains
with bound Ca<sup>2+</sup>. Recently, it has become clear that, at
plasma concentrations of metal ions, Mg<sup>2+</sup> actually occupies
two or three of the divalent metal ion-binding sites in GLA domains,
and that these bound Mg<sup>2+</sup> ions are required for full function
of these clotting proteins. In this study, we investigated how Mg<sup>2+</sup> influences FVIIa enzymatic activity. We found that the presence
of TF was required for Mg<sup>2+</sup> to enhance the rate of FX activation
by FVIIa, and we used alanine-scanning mutagenesis to identify TF
residues important for mediating this response to Mg<sup>2+</sup>.
Several TF mutations, including those at residues G164, K166, and
Y185, blunted the ability of Mg<sup>2+</sup> to enhance the activity
of the TF/FVIIa complex. Our results suggest that these TF residues
interact with the GLA domain of FX in a Mg<sup>2+</sup>-dependent
manner (although effects of Mg<sup>2+</sup> on the FVIIa GLA domain
cannot be ruled out). Notably, these TF residues are located within
or immediately adjacent to the putative substrate-binding exosite
of TF
NMR Determination of Protein p<i>K</i><sub>a</sub> Values in the Solid State
Charged residues play an important role in defining key mechanistic features in many biomolecules. Determining the p<i>K</i><sub>a</sub> values of large, membrane, or fibrillar proteins can be challenging with traditional methods. In this study we show how solid-state NMR is used to monitor chemical shift changes during a pH titration for the small soluble β1 immunoglobulin binding domain of protein G. The chemical shifts of all the amino acids with charged side-chains throughout the uniformly <sup>13</sup>C,<sup>15</sup>N-labeled protein were monitored over several samples varying in pH; p<i>K</i><sub>a</sub> values were determined from these shifts for E27, D36, and E42, and the bounds for the p<i>K</i><sub>a</sub> of other acidic side-chain resonances were determined. Additionally, this study shows how the calculated p<i>K</i><sub>a</sub> values give insights into the crystal packing of the protein
Structural Intermediates during α-Synuclein Fibrillogenesis on Phospholipid Vesicles
α-Synuclein (AS) fibrils are the main protein component
of
Lewy bodies, the pathological hallmark of Parkinson’s disease
and other related disorders. AS forms helices that bind phospholipid
membranes with high affinity, but no atomic level data for AS aggregation
in the presence of lipids is yet available. Here, we present direct
evidence of a conversion from α-helical conformation to β-sheet
fibrils in the presence of anionic phospholipid vesicles and direct
conversion to β-sheet fibrils in their absence. We have trapped
intermediate states throughout the fibril formation pathways to examine
the structural changes using solid-state NMR spectroscopy and electron
microscopy. The comparison between mature AS fibrils formed in aqueous
buffer and those derived in the presence of anionic phospholipids
demonstrates no major changes in the overall fibril fold. However,
a site-specific comparison of these fibrillar states demonstrates
major perturbations in the <i>N</i>-terminal domain with
a partial disruption of the long β-strand located in the 40s
and small perturbations in residues located in the “non-β
amyloid component” (NAC) domain. Combining all these results,
we propose a model for AS fibrillogenesis in the presence of phospholipid
vesicles
High-Resolution NMR Studies of Human Tissue Factor
<div><p>In normal hemostasis, the blood clotting cascade is initiated when factor VIIa (fVIIa, other clotting factors are named similarly) binds to the integral membrane protein, human tissue factor (TF). The TF/fVIIa complex in turn activates fX and fIX, eventually concluding with clot formation. Several X-ray crystal structures of the soluble extracellular domain of TF (sTF) exist; however, these structures are missing electron density in functionally relevant regions of the protein. In this context, NMR can provide complementary structural information as well as dynamic insights into enzyme activity. The resolution and sensitivity for NMR studies are greatly enhanced by the ability to prepare multiple milligrams of protein with various isotopic labeling patterns. Here, we demonstrate high-yield production of several isotopically labeled forms of recombinant sTF, allowing for high-resolution NMR studies both in the solid and solution state. We also report solution NMR spectra at sub-mM concentrations of sTF, ensuring the presence of dispersed monomer, as well as the first solid-state NMR spectra of sTF. Our improved sample preparation and precipitation conditions have enabled the acquisition of multidimensional NMR data sets for TF chemical shift assignment and provide a benchmark for TF structure elucidation.</p></div
Components of media used for isotopically labeled growths of sTF.
<p>Components of media used for isotopically labeled growths of sTF.</p
SDS-PAGE analysis of sTF purification.
<p>SDS-PAGE 12% acrylamide gel of sTF samples stained with Coomassie Brilliant Blue R-250 showing: Lane 1: Precision Plus Protein<sup>TM</sup> Dual Color marker (Bio-Rad, Hercules, CA, USA); Lane 2: water and sucrose combined supernatant; Lane 3: Q-Sepharose® Fast Flow supernatant; Lane 4: Post 0.45 μm filter; Lane 5: pre-load on Ni<sup>2+</sup> affinity column; Lane 6: 500 mM imidazole elution; Lane 7: concentrated sTF.</p
Solid-state <sup>15</sup>N-<sup>13</sup>CA correlation spectra of uniform and glycerol labeled sTF.
<p>(A) <sup>15</sup>N-<sup>13</sup>CA correlation spectrum of ~30 mg of uniform <sup>13</sup>C,<sup>15</sup>N ammonium sulfate-precipitated sTF with 5 mM Cu-EDTA. The spectrum was acquired for 3 hours and 20 minutes with an acquisition time of 25 ms. (B) <sup>15</sup>N-<sup>13</sup>CA correlation spectrum of ~25 mg of 2-<sup>13</sup>C glycerol, <sup>2</sup>H, <sup>15</sup>N ammonium sulfate-precipitated sTF with 5 mM Cu-EDTA. The spectrum was acquired for 3 hours with an acquisition time of 30 ms. Both spectra were collected at 750 MHz (<sup>1</sup>H frequency) at a variable temperature set point of -5°C with a MAS rate of 12.5 kHz. Both spectra were processed with 10 Hz of Lorentzian-to-Gaussian line broadening in each dimension, sine bell apodization, and zero filled 8192 points in the direct (F1) dimension and 2048 in the indirect (F2) dimension with contours drawn at 6 times the noise floor. (C) <sup>13</sup>C 1D slices extracted from the <sup>15</sup>N-<sup>13</sup>CA 2D spectrum of uniform <sup>13</sup>C-<sup>15</sup>N ammonium sulfate-precipitated sTF shown in A. The corresponding <sup>15</sup>N chemical shifts in the indirect dimension are indicated. (D) <sup>13</sup>C 1D slices extracted from the <sup>15</sup>N-<sup>13</sup>CA 2D spectrum of 2-<sup>13</sup>C glycerol, <sup>2</sup>H, <sup>15</sup>N ammonium sulfate-precipitated sTF shown in B. The corresponding <sup>15</sup>N chemical shifts in the indirect dimension are indicated.</p
<sup>1</sup>H-<sup>15</sup>N 2D HSQC correlation spectrum.
<p>Solution NMR fingerprint spectrum of 100 μM uniform <sup>13</sup>C,<sup>15</sup>N sTF in 50 mM sodium phosphate (pH 6.5), 50 mM NaCl, 5% DSS, 10% D<sub>2</sub>O, 0.1% NaN<sub>3</sub> acquired at a variable temperature set point of 35°C on a Varian/Agilent VNMRS 17.6 T (750 MHz <sup>1</sup>H frequency) spectrometer.</p