RESUMEN
Fibrin gels are biological networks that play a fundamental role in blood coagulation and other patho/physiological processes, such as thrombosis and cancer. Electron and confocal microscopies show a collection of fibers that are relatively monodisperse in diameter, not uniformly distributed, and connected at nodal points with a branching order of â¼3-4. Although in the confocal images the hydrated fibers appear to be quite straight (mass fractal dimension D(m) = 1), for the overall system 1
Asunto(s)
Simulación por Computador , Fibrina/química , Geles/química , Luz , Microscopía Confocal , Polimerizacion , Dispersión de RadiaciónRESUMEN
The average pore size ξ0 of filamentous networks assembled from biological macromolecules is one of the most important physical parameters affecting their biological functions. Modern optical methods, such as confocal microscopy, can noninvasively image such networks, but extracting a quantitative estimate of ξ0 is a nontrivial task. We present here a fast and simple method based on a two-dimensional bubble approach, which works by analyzing one by one the (thresholded) images of a series of three-dimensional thin data stacks. No skeletonization or reconstruction of the full geometry of the entire network is required. The method was validated by using many isotropic in silico generated networks of different structures, morphologies, and concentrations. For each type of network, the method provides accurate estimates (a few percent) of the average and the standard deviation of the three-dimensional distribution of the pore sizes, defined as the diameters of the largest spheres that can be fit into the pore zones of the entire gel volume. When applied to the analysis of real confocal microscopy images taken on fibrin gels, the method provides an estimate of ξ0 consistent with results from elastic light scattering data.
Asunto(s)
Simulación por Computador , Fibrina/química , Microscopía Confocal/métodos , Biopolímeros/química , Geles/química , Luz , Dispersión de RadiaciónRESUMEN
The features of scattered and transmitted light by dilute suspensions of transparent submicron particles are investigated both in the spectral and in the perceived colorimetric domains, as a function of effective particle diameter D, particle-host refractive-index mismatch m, and scattering angle θ. Our results show that the wavelength λ-dependence of the scattering and extinction cross sections remains quite similar well beyond the Rayleigh regime up to particle sizes of a few hundreds nm, but only for specific scattering angles that depend on D and m, and tend to 90° on approaching the Rayleigh regime. Close to this limit (D/λ<<1), a simple criterion that relates the perceived scattering color at θ=90° and the ratio of the sample extinction coefficients at two properly selected wavelengths is demonstrated. A comparison between computed and measured data is presented.
RESUMEN
The kinetics of release of fibrinopeptide A (FPA) and B (FPB) by thrombin were investigated on unfractionated fibrinogen samples as a function of CaCl(2) concentration. A 50 mM Tris, 104 mM NaCl, pH 7.4 (TBS) buffer, to which 1 mM EDTA-Na(2) (TBE) or 2.5 (TBC2.5), 14 (TBC14), and 30 mM CaCl(2) (TBC30) was alternatively added, was employed. The % FPA versus time curves were fitted with single stretched-exponential growth functions, where the stretch parameter beta likely reflects substrate polydispersity (beta = 1, monodisperse). For TBE, TBS, TBC14, and TBC30, we found beta approximately 1, with corresponding normalized rate constants (K(a)) of 3.8, 4.2, 2.7, and 1.9 x 10(-5) [(NIHu/L)s](-1). Surprisingly, in TBC2.5 we found beta = 0.69, with an "average" K(a) of 3.5 x 10(-5) [(NIHu/L)s](-1). This effect disappeared [beta = 0.97, K(a) = 2.7 x 10(-5) [(NIHu/L)s](-1)] with an increase in the ionic strength I to that of TBC30 with 186 mM NaCl (TBCaNa buffer). FPB releases were instead consistent with a nonstretched consecutive exponential growth function, except in TBC30 where some FPB appeared to be cleaved independently. Log-log plots of K(a) versus Ca(2+) concentration, Cl(-) concentration, or I showed a strong linear correlation with only the latter two except in TBCaNa, again suggesting specific effects of the physiological Ca(2+) concentration and I on FPA release. The corresponding K(b) plots showed instead that both total depletion and high Ca(2+) hampered FPB release. To further investigate the TBC2.5 beta = 0.69 effect, FG polydispersity was assessed by Western blot analyses. The thrombin-binding gamma'-chain isoform was approximately 4%, resulting in a bound:free thrombin ratio of approximately 25:75. With regard to the C-terminal ends of the Aalpha-chains, approximately 45% were either intact or lightly degraded, while the remaining approximately 55% were more degraded. Fitting the % FPA release data in TBC2.5 with a sum of two exponentials resulted in a faster component and a slower component (K(a1)/K(a2) approximately 6), with a ratio of approximately 48:52. While a role for the gamma'-chain isoform cannot be excluded, this good correlation with the C-terminal degradation of the Aalpha-chains suggests their calcium-dependent involvement in FPA release.