TY - JOUR
T1 - Description of hydration water in protein (green fluorescent protein) solution
AU - Perticaroli, Stefania
AU - Ehlers, Georg
AU - Stanley, Christopher B.
AU - Mamontov, Eugene
AU - O'Neill, Hugh
AU - Zhang, Qiu
AU - Cheng, Xiaolin
AU - Myles, Dean A.A.
AU - Katsaras, John
AU - Nickels, Jonathan D.
N1 - Publisher Copyright:
© 2016 American Chemical Society.
PY - 2017/1/25
Y1 - 2017/1/25
N2 - The structurally and dynamically perturbed hydration shells that surround proteins and biomolecules have a substantial influence upon their function and stability. This makes the extent and degree of water perturbation of practical interest for general biological study and industrial formulation. We present an experimental description of the dynamical perturbation of hydration water around green fluorescent protein in solution. Less than two shells (∼5.5 Á) were perturbed, with dynamics a factor of 2-10 times slower than bulk water, depending on their distance from the protein surface and the probe length of the measurement. This dependence on probe length demonstrates that hydration water undergoes subdiflusive motions (τ ∝ q-2.5 for the first hydration shell, τ ∝ q-2.3 for perturbed water in the second shell), an important difference with neat water, which demonstrates diffusive behavior (τ ∝ q-2). These results help clarify the seemingly conflicting range of values reported for hydration water retardation as a logical consequence of the different length scales probed by the analytical techniques used.
AB - The structurally and dynamically perturbed hydration shells that surround proteins and biomolecules have a substantial influence upon their function and stability. This makes the extent and degree of water perturbation of practical interest for general biological study and industrial formulation. We present an experimental description of the dynamical perturbation of hydration water around green fluorescent protein in solution. Less than two shells (∼5.5 Á) were perturbed, with dynamics a factor of 2-10 times slower than bulk water, depending on their distance from the protein surface and the probe length of the measurement. This dependence on probe length demonstrates that hydration water undergoes subdiflusive motions (τ ∝ q-2.5 for the first hydration shell, τ ∝ q-2.3 for perturbed water in the second shell), an important difference with neat water, which demonstrates diffusive behavior (τ ∝ q-2). These results help clarify the seemingly conflicting range of values reported for hydration water retardation as a logical consequence of the different length scales probed by the analytical techniques used.
UR - http://www.scopus.com/inward/record.url?scp=85019075253&partnerID=8YFLogxK
U2 - 10.1021/jacs.6b08845
DO - 10.1021/jacs.6b08845
M3 - Article
C2 - 27783480
AN - SCOPUS:85019075253
SN - 0002-7863
VL - 139
SP - 1098
EP - 1105
JO - Journal of the American Chemical Society
JF - Journal of the American Chemical Society
IS - 3
ER -