4 research outputs found
Evidence from 900 MHz <sup>1</sup>H MAS NMR of Displacive Behavior of the Model OrderāDisorder Antiferroelectric NH<sub>4</sub>H<sub>2</sub>AsO<sub>4</sub>
NH<sub>4</sub>H<sub>2</sub>AsO<sub>4</sub> (ADA) is a model compound for
understanding the mechanism of phase transitions in the KH<sub>2</sub>PO<sub>4</sub> (KDP) family of ferroelectrics. ADA exhibits a paraelectric
(PE) to antiferroelectric (AFE) phase transition at <i>T</i><sub>N</sub> ā¼ 216 K whose mechanism remains unclear. With
the view of probing the role of the various protons in the transition
mechanism, we have employed the high-resolution technique of magic
angle spinning at the high Zeeman field of 21.1 T (<sup>1</sup>H resonance
at 900 MHz). We measured the temperature dependence of the isotropic
chemical shift and spinālattice relaxation time, <i>T</i><sub>1</sub>, of the OāHĀ·Ā·Ā·O and NH<sub>4</sub><sup>+</sup> protons through the <i>T</i><sub>N</sub>.
As <i>T</i> ā <i>T</i><sub>N</sub>, NMR
peaks from the PE and AFE phases are seen to coexist over a temperature
range of about 3 K, showing formation of nearly static (lifetime >
milliseconds) pretransitional clusters in this lattice as it approaches
its <i>T</i><sub>N</sub>, consistent with the near first-order
nature of the phase transition. The isotropic chemical shift of the
OāHĀ·Ā·Ā·O protons exhibited a steplike anomaly
at <i>T</i><sub>N</sub>, providing direct evidence of displacive
character in this lattice commonly thought of as an orderādisorder
type. No such anomaly was noticeable for the NH<sub>4</sub><sup>+</sup> protons. Both sets of protons exhibited orderādisorder characteristics
in their <i>T</i><sub>1</sub> data, as analyzed in terms
of the standard Bloembergen, Purcell, and Pound (BPP) model. These
data suggest that the traditionally employed classification of equilibrium
phase transitions into <i>orderādisorder</i> and <i>displacive</i> ones, should rather be ā<i>orderādisorder
cum displacive</i>ā type
<sup>17</sup>O MAS NMR Correlation Spectroscopy at High Magnetic Fields
The structure of
two protected amino acids, FMOC-l-leucine
and FMOC-l-valine, and a dipeptide, <i>N</i>-acetyl-l-valyl-l-leucine (N-Ac-VL), were studied via one-
and two-dimensional solid-state nuclear magnetic resonance (NMR) spectroscopy.
Utilizing <sup>17</sup>O magic-angle spinning (MAS) NMR at multiple
magnetic fields (17.6ā35.2 T/750ā1500 MHz for <sup>1</sup>H) the <sup>17</sup>O quadrupolar and chemical shift parameters were
determined for the two oxygen sites of each FMOC-protected amino acids
and the three distinct oxygen environments of the dipeptide. The one-
and two-dimensional, <sup>17</sup>O, <sup>15</sup>Nā<sup>17</sup>O, <sup>13</sup>Cā<sup>17</sup>O, and <sup>1</sup>Hā<sup>17</sup>O double-resonance correlation experiments performed on the
uniformly <sup>13</sup>C,<sup>15</sup>N and 70% <sup>17</sup>O-labeled
dipeptide prove the attainability of <sup>17</sup>O as a probe for
structure studies of biological systems. <sup>15</sup>Nā<sup>17</sup>O and <sup>13</sup>Cā<sup>17</sup>O distances were
measured via one-dimensional REAPDOR and ZF-TEDOR experimental buildup
curves and determined to be within 15% of previously reported distances,
thus demonstrating the use of <sup>17</sup>O NMR to quantitate interatomic
distances in a fully labeled dipeptide. Through-space hydrogen bonding
of N-Ac-VL was investigated by a two-dimensional <sup>1</sup>H-detected <sup>17</sup>O R<sup>3</sup>-R-INEPT experiment, furthering the importance
of <sup>17</sup>O for studies of structure in biomolecular solids
Structural Model of the Tubular Assembly of the Rous Sarcoma Virus Capsid Protein
The orthoretroviral
capsid protein (CA) assembles into polymorphic
capsids, whose architecture, assembly, and stability are still being
investigated. The N-terminal and C-terminal domains of CA (NTD and
CTD, respectively) engage in both homotypic and heterotypic interactions
to create the capsid. Hexameric turrets formed by the NTD decorate
the majority of the capsid surface. We report nearly complete solid-state
NMR (ssNMR) resonance assignments of Rous sarcoma virus (RSV) CA,
assembled into hexamer tubes that mimic the authentic capsid. The
ssNMR assignments show that, upon assembly, large conformational changes
occur in loops connecting helices, as well as the short 3<sub>10</sub> helix initiating the CTD. The interdomain linker becomes statically
disordered. Combining constraints from ssNMR and cryo-electron microscopy
(cryo-EM), we establish an atomic resolution model of the RSV CA tubular
assembly using molecular dynamics flexible fitting (MDFF) simulations.
On the basis of comparison of this MDFF model with an earlier-derived
crystallographic model for the planar assembly, the induction of curvature
into the RSV CA hexamer lattice arises predominantly from reconfiguration
of the NTDāCTD and CTD trimer interfaces. The CTD dimer and
CTD trimer interfaces are also intrinsically variable. Hence, deformation
of the CA hexamer lattice results from the variable displacement of
the CTDs that surround each hexameric turret. Pervasive H-bonding
is found at all interdomain interfaces, which may contribute to their
malleability. Finally, we find helices at the interfaces of HIV and
RSV CA assemblies have very different contact angles, which may reflect
differences in the capsid assembly pathway for these viruses
HIVā1 Capsid Function Is Regulated by Dynamics: Quantitative Atomic-Resolution Insights by Integrating Magic-Angle-Spinning NMR, QM/MM, and MD
HIV-1
CA capsid protein possesses intrinsic conformational flexibility,
which is essential for its assembly into conical capsids and interactions
with host factors. CA is dynamic in the assembled capsid, and residues
in functionally important regions of the protein undergo motions spanning
many decades of time scales. Chemical shift anisotropy (CSA) tensors,
recorded in magic-angle-spinning NMR experiments, provide direct residue-specific
probes of motions on nano- to microsecond time scales. We combined
NMR, MD, and density-functional-theory calculations, to gain quantitative
understanding of internal backbone dynamics in CA assemblies, and
we found that the dynamically averaged <sup>15</sup>N CSA tensors
calculated by this joined protocol are in remarkable agreement with
experiment. Thus, quantitative atomic-level understanding of the relationships
between CSA tensors, local backbone structure, and motions in CA assemblies
is achieved, demonstrating the power of integrating NMR experimental
data and theory for characterizing atomic-resolution dynamics in biological
systems