6 research outputs found
Sodium Dodecyl Sulfate Monomers Induce XAO Peptide Polyproline II to α‑Helix Transition
XAO peptide (Ac–X<sub>2</sub>A<sub>7</sub>O<sub>2</sub>–NH<sub>2</sub>; X: diaminobutyric
acid side chain, −CH<sub>2</sub>CH<sub>2</sub>NH<sub>3</sub><sup>+</sup>; O: ornithine side chain,
−CH<sub>2</sub>CH<sub>2</sub>CH<sub>2</sub>NH<sub>3</sub><sup>+</sup>) in aqueous solution shows a predominantly polyproline II
(PPII) conformation without any detectable α-helix-like conformations.
Here we demonstrate by using circular dichroism (CD), ultraviolet
resonance Raman (UVRR) and nuclear magnetic resonance (NMR) spectroscopy
that sodium dodecyl sulfate (SDS) monomers bind to XAO and induce
formation of α-helix-like conformations. The stoichiometry and
the association constants of SDS and XAO were determined from the
XAO–SDS diffusion coefficients measured by pulsed field gradient
NMR. We developed a model for the formation of XAO–SDS aggregate
α-helix-like conformations. Using UVRR spectroscopy, we calculated
the Ramachandran ψ angle distributions of aggregated XAO peptides.
We resolved α-, π- and 3<sub>10</sub>- helical conformations
and a turn conformation. XAO nucleates SDS aggregation at SDS concentrations
below the SDS critical micelle concentration. The XAO<sub>4</sub>–SDS<sub>16</sub> aggregates have four SDS molecules bound to each XAO to
neutralize the four side chain cationic charges. We propose that the
SDS alkyl chains partition into a hydrophobic core to minimize the
hydrophobic area exposed to water. Neutralization of the flanking
XAO charges enables α-helix formation. Four XAO–SDS<sub>4</sub> aggregates form a complex with an SDS alkyl chain-dominated
hydrophobic core and a more hydrophilic shell where one face of the
α-helix peptide contacts the water environment
Polyglutamine Fibrils: New Insights into Antiparallel β‑Sheet Conformational Preference and Side Chain Structure
Understanding the structure of polyglutamine
(polyQ) amyloid-like
fibril aggregates is crucial to gaining insights into the etiology
of at least ten neurodegenerative disorders, including Huntington’s
disease. Here, we determine the structure of D<sub>2</sub>Q<sub>10</sub>K<sub>2</sub> (Q10) fibrils using ultraviolet resonance Raman (UVRR)
spectroscopy and molecular dynamics (MD). Using UVRR, we determine
the fibril peptide backbone Ψ and glutamine (Gln) side chain
χ<sub>3</sub> dihedral angles. We find that most of the fibril
peptide bonds adopt antiparallel β-sheet conformations; however,
a small population of peptide bonds exist in parallel β-sheet
structures. Using MD, we simulate three different potential fibril
structural models that consist of either β-strands or β-hairpins.
Comparing the experimentally measured Ψ and χ<sub>3</sub> angle distributions to those obtained from the MD simulated models,
we conclude that the basic structural motif of Q10 fibrils is an extended
β-strand structure. Importantly, we determine from our MD simulations
that Q10 fibril antiparallel β-sheets are thermodynamically
more stable than parallel β-sheets. This accounts for why polyQ
fibrils preferentially adopt antiparallel β-sheet conformations
instead of in-register parallel β-sheets like most amyloidogenic
peptides. In addition, we directly determine, for the first time,
the structures of Gln side chains. Our structural data give new insights
into the role that the Gln side chains play in the stabilization of
polyQ fibrils. Finally, our work demonstrates the synergistic power
and utility of combining UVRR measurements and MD modeling to determine
the structure of amyloid-like fibrils
UV Resonance Raman Investigations of Peptide and Protein Structure and Dynamics
UV Resonance Raman Investigations of Peptide and Protein Structure and Dynamic
2D Photonic Crystal Protein Hydrogel Coulometer for Sensing Serum Albumin Ligand Binding
Bovine and human serum albumin (BSA
and HSA) are globular proteins
that function as bloodstream carriers of hydrophobes such as fatty
acids and drugs. We fabricated novel photonic crystal protein hydrogels
by attaching 2D colloidal arrays onto pure BSA and HSA hydrogels.
The wavelengths of the diffracted light sensitively report on the
protein hydrogel surface area. The binding of charged species to the
protein hydrogel gives rise to Donnan potentials that change the hydrogel
volume causing shifts in the diffraction. These photonic crystal protein
hydrogels act as sensitive Coulometers that monitor the hydrogel charge
state. We find multiple high-affinity BSA and HSA binding sites for
salicylate, ibuprofen and picosulfate by using these sensors to monitor
binding of charged drugs. We demonstrate proof-of-concept for utilizing
protein hydrogel sensors to monitor protein–ionic species binding
Glutamine and Asparagine Side Chain Hyperconjugation-Induced Structurally Sensitive Vibrations
We
identified vibrational spectral marker bands that sensitively
report on the side chain structures of glutamine (Gln) and asparagine
(Asn). Density functional theory (DFT) calculations indicate that
the Amide III<sup>P</sup> (AmIII<sup>P</sup>) vibrations of Gln and
Asn depend cosinusoidally on their side chain OCCC dihedral angles
(the χ<sub>3</sub> and χ<sub>2</sub> angles of Gln and
Asn, respectively). We use UV resonance Raman (UVRR) and visible Raman
spectroscopy to experimentally correlate the AmIII<sup>P</sup> Raman
band frequency to the primary amide OCCC dihedral angle. The AmIII<sup>P</sup> structural sensitivity derives from the Gln (Asn) C<sub>β</sub>–C<sub>γ</sub> (C<sub>α</sub>–C<sub>β</sub>) stretching component of the vibration. The C<sub>β</sub>–C<sub>γ</sub> (C<sub>α</sub>–C<sub>β</sub>) bond
length inversely correlates with the AmIII<sup>P</sup> band frequency.
As the C<sub>β</sub>–C<sub>γ</sub> (C<sub>α</sub>–C<sub>β</sub>) bond length decreases, its stretching
force constant increases, which results in an upshift in the AmIII<sup>P</sup> frequency. The C<sub>β</sub>–C<sub>γ</sub> (C<sub>α</sub>–C<sub>β</sub>) bond length dependence
on the χ<sub>3</sub> (χ<sub>2</sub>) dihedral angle results
from hyperconjugation between the C<sub>δ</sub>O<sub>ϵ</sub> (C<sub>γ</sub>O<sub>δ</sub>) π*
and C<sub>β</sub>–C<sub>γ</sub> (C<sub>α</sub>–C<sub>β</sub>) σ orbitals. Using a Protein Data
Bank library, we show that the χ<sub>3</sub> and χ<sub>2</sub> dihedral angles of Gln and Asn depend on the peptide backbone
Ramachandran angles. We demonstrate that the inhomogeneously broadened
AmIII<sup>P</sup> band line shapes can be used to calculate the χ<sub>3</sub> and χ<sub>2</sub> angle distributions of peptides.
The spectral correlations determined in this study enable important
new insights into protein structure in solution, and in Gln- and Asn-rich
amyloid-like fibrils and prions
UV Resonance Raman Investigation of the Aqueous Solvation Dependence of Primary Amide Vibrations
We
investigated the normal mode composition and the aqueous solvation
dependence of the primary amide vibrations of propanamide. Infrared,
normal Raman, and UV resonance Raman (UVRR) spectroscopy were applied
in conjunction with density functional theory (DFT) to assign the
vibrations of crystalline propanamide. We examined the aqueous solvation
dependence of the primary amide UVRR bands by measuring spectra in
different acetonitrile/water mixtures. As previously observed in the
UVRR spectra of <i>N</i>-methylacetamide, all of the resonance
enhanced primary amide bands, except for the Amide I (AmI), show increased
UVRR cross sections as the solvent becomes water-rich. These spectral
trends are rationalized by a model wherein the hydrogen bonding and
the high dielectric constant of water stabilizes the <i>ground
state</i> dipolar <sup>–</sup>OCNH<sub>2</sub><sup>+</sup> resonance structure over the neutral OCNH<sub>2</sub> resonance structure. Thus, vibrations with large CN
stretching show increased UVRR cross sections because the Cî—¸N
displacement between the electronic ground and excited state increases
along the Cî—¸N bond. In contrast, vibrations dominated by Cî—»O
stretching, such as the AmI, show a decreased displacement between
the electronic ground and excited state, which result in a decreased
UVRR cross section upon aqueous solvation. The UVRR primary amide
vibrations can be used as sensitive spectroscopic markers to study
the local dielectric constant and hydrogen bonding environments of
the primary amide side chains of glutamine (Gln) and asparagine (Asn)