FLOW CYTOMETRIC MEASUREMENT OF KINETIC AND EQUILIBRIUM BINDING PARAMETERS OF ARGININE-GLYCINE-ASPARTIC ACID LIGANDS IN BINDING TO GLYCOPROTEIN IIB IIIA ON PLATELETS/
B. Bednar et al., FLOW CYTOMETRIC MEASUREMENT OF KINETIC AND EQUILIBRIUM BINDING PARAMETERS OF ARGININE-GLYCINE-ASPARTIC ACID LIGANDS IN BINDING TO GLYCOPROTEIN IIB IIIA ON PLATELETS/, Cytometry, 28(1), 1997, pp. 58-65
Antagonists of platelet glycoprotein IIb/IIIa (GPIIb/IIIa) represent a
new therapeutic approach in inhibiting platelet aggregation, thus pro
viding a powerful form of antithrombotic therapy. The measurement of b
inding of arginine-glycine-aspartic acid (RGD) peptidomimetics to GPII
b/IIIa on platelets is a key for the further understanding of ligand-r
eceptor interactions and, thus, the design of new antagonists, The flo
w cytometric measurement of dynamic and equilibrium binding parameters
of two new potent RGD peptidomimetics, L-762,745 and L-769,434, conta
ining a fluorescein moiety is described in this paper, Kinetic binding
measurements with these fluorescent ligands indicate a two-step bindi
ng mechanism that involves a conformational rearrangement of the recep
tor-ligand complex, The overall second-order binding constants are for
both fluorescent ligands several orders of magnitude slower than for
diffusion-controlled processes. The values of k(-1) and K-D obtained b
y fitting the kinetic binding data in a two-step model are in good agr
eement with directly detected values of k(off)(L-762,745) = (1.9 +/- 0
.6) 10(-3) s(-1), k(off)(L-769,434) = (5.1 +/- 0.7) 10(-3) s(-1), K-D(
L-762,745) = 12 +/- 0.5 nM, and K-D(L-769,434) = 8 +/- 0.3 nM, Equilib
rium binding measurements of fluorescent ligands with an orally active
nonfluorescent antagonist, L-738,167, provided apparent dissociation
binding constant K-D of this ligand in the range from 0.1 to 0.2 nM, T
he kinetic dissociation measurement of L-738,167 using the binding of
the fluorescent ligand L-762,745 as a reporting method yielded a k(off
) for L-738,167 of (4.1 +/- 0.1) x 10(-4) s(-1) (t(1/2) = 28 min). (C)
1997 Wiley-Liss, Inc.