doi:10.1006/jmbi.2000.4306
Copyright © 2001 Academic Press. All rights reserved.
Regular article
The molecular basis for the inverse temperature transition of elastin1
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Bin Lia, Darwin O. V. Alonsoa and Valerie Daggetta,
, 
a Department of Medicinal Chemistry, University of Washington, Seattle WA 98195-7610, USA
Received 29 June 2000;
revised 1 November 2000;
accepted 6 November 2000. ;
Available online 26 February 2002.
Abstract
Elastin undergoes an “inverse temperature transition” such that it becomes more ordered as the temperature increases. To investigate the molecular basis for this behavior, molecular dynamics simulations were conducted above and below the transition temperature. Simulations of a 90-residue elastin peptide, (VPGVG)18, with explicit water molecules were performed at seven different temperatures between 7 and 42 °C, for a total of 80 ns. Beginning from an idealized β-spiral structure, hydrophobic collapse was observed over a narrow temperature range in the simulations. Moreover, simulations above and below elastin’s transition temperature indicate that elastin has more turns and distorted β-structure at higher temperatures. Water was critical to the inverse temperature transition and elastin-associated water molecules can be divided into three categories: those closely associated with βII turns; those that form hydrogen bonds with the main-chain groups; and those hydrating the hydrophobic side-chains. Water-swollen, monomeric elastin above the transition temperature is best described as a compact amorphous structure with distorted β-strands, fluctuating turns, buried hydrophobic residues, and main-chain polar atoms that participate in hydrogen bonds with water. Below the transition temperature, elastin is expanded with
40 % local β-spiral structure. Overall the simulations are in agreement with experiment and therefore appear to provide an atomic-level description of the conformational properties of elastin monomers and the basis for their elastomeric properties.
Author Keywords: inverse temperature transition; hydrophobic collapse; elastin-associated water; molecular dynamics simulations; β-spiral
Abbreviations: CD, circular dichroism; MD, molecular dynamics
Figure 1. Temperature-dependent conformational behavior of elastin. The 6-ns structure from each simulation is shown with the main-chain in red and side-chain atoms in green.
Figure 2. C
α root-mean-square deviation from the starting β-spiral structure as a function of simulation time at seven different temperatures.
Figure 3. Temperature-induced structural changes of elastin
via quenching or heating of structures shown in
Figure 1. The final structure from each simulation is shown with glycine in red and proline and valine in green. The solvent accessible surface area is provided in parentheses.
Figure 4. Ramachandran plots over 6–9ns for the high (40 and 42 °C, green) and low (7 and 10 °C, blue) temperature simulations.
Figure 5. Representative dynamics of βII turn formation/deformation at 42 °C. (a) snapshots of the representative turn of Val81-Val84; (b,c) the anti-correlation of Gly83 Ψ and Val84 Φ, corresponding to a crankshaft-like motion in turn regions (arrows indicate the time points of the snapshots).
Figure 6. Hydrophobic collapse and expulsion of water molecules are responsible for the inverse temperature transition of elastin. The elastin main-chain is shown in red. Elastin-associated water molecules are in blue and water molecules expelled upon collapse are in magenta. The average change in non-polar solvent-accessible surface area and the number of expelled water molecules over 3–6 ns are plotted as a function of temperature. The values for the starting β-spiral structure are shown at 0 °C. The expelled water molecules represent the change in the number of water molecules in shells 1 and 2.
Figure 7. Cycles of expansion and contraction of elastin at 42 °C from 6–9 ns. (a) Total solvent-accessible surface area (Å
2); (b) the number of hydrophobic contacts; (c) representative snapshots of elastin with the main-chain polar atoms in red and all others in green.
Table 1. Average properties of various temperature simulations over different time periods

The data were averaged over the designated time periods.
Table 2. Tabulation of different types of hydrogen bonds formed above and below the transition temperature

Structures were evaluated every 5 ps from 6–9 ns. Numbers in parentheses are the average numbers of hydrogen bonds per structure.
Table 3. Comparison of different elastin models with experimental results

+, Agrees with the experiment; −, disagrees with the experiment; ?, unknown, hard to judge.
Corresponding author
1 Edited by A. R. Fersht