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Biophys J, July 2001, p. 25-42, Vol. 81, No. 1
and
*Laboratoire d'Immunologie, Hôpital de Sainte-Marguerite,
13274 Marseille Cedex 09, France and
George W. Woodruff
School of Mechanical Engineering, Georgia Institute of Technology,
Atlanta, Georgia 30332 USA
The rate and distance-dependence of
association between surface-attached molecules may be determined by
monitoring the motion of receptor-bearing spheres along ligand-coated
surfaces in a flow chamber (Pierres et al., Proc. Natl. Acad.
Sci. U.S.A. 95:9256-9261, 1998). Particle arrests reveal bond
formation, and the particle-to-surface distance may be estimated from
the ratio between the velocity and the wall shear rate. However,
several problems are raised. First, data interpretation requires
extensive computer simulations. Second, the relevance of standard
results from fluid mechanics to micrometer-size particles separated
from surfaces by nanometer distances is not fully demonstrated. Third,
the wall shear rate must be known with high accuracy. Here we present a
simple derivation of an algorithm permitting one to simulate the motion
of spheres near a plane in shear flow. We check that theoretical
predictions are consistent with the experimental dependence of motion
on medium viscosity or particle size, and the requirement for
equilibrium particle height distribution to follow Boltzman's law. The
determination of the statistical relationship between particle velocity
and acceleration allows one to derive the wall shear rate with
1-s
1 accuracy and the Hamaker constant of interaction
between the particle and the wall with a sensitivity better than
10
21 J. It is demonstrated that the correlation between
particle height and mean velocity during a time interval
t is maximal when
t is about 0.1-0.2 s for
a particle of 1.4-µm radius. When the particle-to-surface distance
ranges between 10 and 40 nm, the particle height distribution may be
obtained with a standard deviation ranging between 8 and 25 nm,
provided the average velocity during a 160-ms period of time is
determined with 10% accuracy. It is concluded that the flow chamber
allows one to detect the formation of individual bonds with a minimal
lifetime of 40 ms in presence of a disruptive force of ~5 pN and to
assess the distance dependence within the tens of nanometer range.
Biophys J, July 2001, p. 25-42, Vol. 81, No. 1
© 2001 by the Biophysical Society 0006-3495/01/07/25/18 $2.00
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