Temperature-Induced
Reversible First-Order Single
Crystal to Single Crystal Phase Transition in Boc‑γ<sup>4</sup>(<i>R</i>)Val-Val-OH: Interplay of Enthalpy and
Entropy
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Abstract
Crystals
of Boc-γ<sup>4</sup>(<i>R</i>)Val-Val-OH
undergo a reversible first-order single crystal to single crystal
phase transition at <i>T</i><sub>c</sub> ≈ 205 K
from the orthorhombic space group <i>P</i>22<sub>1</sub>2<sub>1</sub> (<i>Z</i>′ = 1) to the monoclinic
space group <i>P</i>2<sub>1</sub> (<i>Z</i>′
= 2) with a hysteresis of ∼2.1 K. The low-temperature monoclinic
form is best described as a nonmerohedral twin with ∼50% contributions
from its two components. The thermal behavior of the dipeptide crystals
was characterized by differential scanning calorimetry experiments.
Visual changes in birefringence of the sample during heating and cooling
cycles on a hot-stage microscope with polarized light supported the
phase transition. Variable-temperature unit cell check measurements
from 300 to 100 K showed discontinuity in the volume and cell parameters
near the transition temperature, supporting the first-order behavior.
A detailed comparison of the room-temperature orthorhombic form with
the low-temperature (100 K) monoclinic form revealed that the strong
hydrogen-bonding motif is retained in both crystal systems, whereas
the non-covalent interactions involving side chains of the dipeptide
differ significantly, leading to a small change in molecular conformation
in the monoclinic form as well as a small reorientation of the molecules
along the <i>ac</i> plane. A rigid-body thermal motion analysis
(translation, libration, screw; correlation of translation and libration)
was performed to study the crystal entropy. The reversible nature
of the phase transition is probably the result of an interplay between
enthalpy and entropy: the low-temperature monoclinic form is enthalpically
favored, whereas the room-temperature orthorhombic form is entropically
favored