| Literature DB >> 24121323 |
Takeshi Yokoyama1, Mineyuki Mizuguchi, Yuko Nabeshima, Katsuhiro Kusaka, Taro Yamada, Takaaki Hosoya, Takashi Ohhara, Kazuo Kurihara, Ichiro Tanaka, Nobuo Niimura.
Abstract
Transthyretin (TTR) is a tetrameric protein. TTR misfolding and aggregation are associated with human amyloid diseases. Dissociation of the TTR tetramer is believed to be the rate-limiting step in the amyloid fibril formation cascade. Low pH is known to promote dissociation into monomer and the formation of amyloid fibrils. In order to reveal the molecular mechanisms underlying pH sensitivity and structural stabilities of TTR, neutron diffraction studies were conducted using the IBARAKI Biological Crystal Diffractometer with the time-of-flight method. Crystals for the neutron diffraction experiments were grown up to 2.5 mm(3) for four months. The neutron crystal structure solved at 2.0 Å revealed the protonation states of His88 and the detailed hydrogen-bond network depending on the protonation states of His88. This hydrogen-bond network is involved in monomer-monomer and dimer-dimer interactions, suggesting that the double protonation of His88 by acidification breaks the hydrogen-bond network and causes the destabilization of the TTR tetramer. Structural comparison with the X-ray crystal structure at acidic pH identified the three amino acid residues responsible for the pH sensitivity of TTR. Our neutron model provides insights into the molecular stability related to amyloidosis.Entities:
Keywords: amyloidosis; hydrogen-bond network; neutron protein crystallography; pH sensitivity; transthyretin
Mesh:
Substances:
Year: 2013 PMID: 24121323 PMCID: PMC3795539 DOI: 10.1107/S090904951302075X
Source DB: PubMed Journal: J Synchrotron Radiat ISSN: 0909-0495 Impact factor: 2.616
Figure 1Structure of the TTR tetramer. The dimer–dimer contacts are indicated as dashed circles. Subunit A is shown in grey, B in green, C in blue and D in magenta.
Figure 2The TTR crystal for the neutron diffraction experiment.
Figure 3Time-of-flight neutron diffraction image recorded by iBIX. The three-dimensional diffraction data were projected in time-of-flight.
Statistics on the data collection and refinement
Numbers in parentheses refer to the highest-resolution shell.
| Crystal data | |
| Resolution range (Å) | 12.1–2.0 (2.07–2.00) |
| Space group |
|
| Unit cell (Å) |
|
| Unique reflections | 15307 (2080) |
|
| 19.1 (30.6) |
| Completeness (%) | 86.4 (72.5) |
|
| 4.3 (1.5) |
| Redundancy | 2.6 (1.7) |
| Refinement data | |
|
| 23.4 |
|
| 27.2 |
| RMSD bonds (Å) | 0.010 |
| RMSD angles (°) | 1.207 |
R sym = ΣΣ|I (hkl) − I()|/ΣΣ I (hkl).
R factor = Σ|F o| − |F c|/|F o|, where F o and F c are the observed and calculated structure factor amplitudes, respectively.
R free was calculated with 5% of the data excluded from the refinement.
Figure 4The hydrogen-bond network consisted of His88 and water molecules. The |F o| − |F c| difference neutron scattering length density map was calculated omitting His88 and water molecules (contoured at 2.5σ). The hydrogen bonds are indicated as dashed yellow lines. The residue names of subunit A are shown in grey and those of D are in magenta. Unexchangeable H atoms are not displayed.
List of hydrogen bonds and possible CH⋯O hydrogen bonds formed between subunits A and D
| Acceptor | Donor | Distance (Å) |
|---|---|---|
| Hydrogen bonds | O⋯O, N (O⋯ | |
| A19( | Y114( | 3.0 (2.2) |
| S112( | S112( | 2.5 (1.9) |
| A19( | Y114( | 3.0 (2.2) |
| CH⋯O hydrogen bonds | O⋯C (O⋯H) | |
| A19( | Y114( | 3.4 (2.6) |
| V20( | P113( | 3.6 (2.8) |
| V20( | Y114( | 3.4 (2.8) |
| A19( | S112( | 3.6 (2.9) |
| A19( | S112( | 3.6 (2.9) |
| V20( | P113( | 3.6 (2.7) |
| A19( | Y114( | 3.4 (2.6) |
| V20( | Y114( | 3.4 (2.8) |