scholarly journals Size and Shape of Human Fibrinogen in Solution

1977 ◽  
Author(s):  
V. Hofmann ◽  
P.W. Straub ◽  
T. Binkert ◽  
E. Serrallach ◽  
W. Känzig ◽  
...  

In order to obtain information on size and shape of the fibrinogen molecule in solution the translational diffusion coefficient (DT), the rotational diffusion coefficients (DR⊥ and DR//) and the sedimentation coefficients (S) have been measured on human fibrinogen with a clottaoility above 95%. The methods used were dynamic light scattering, nanosecond fluorescence depolarization and analytical ultracentrifugation. Dynamic light scattering yields DT = 2.0 ± 3% x 10-7 cm2sec–1 at a concentration of 7 mg/ml in 0.15 M Tris-NaCl, pH 7.4. DT is strongly dependent on concentration, being 3.4 ± 10% × 10-7 cm2 sec-1 at 0.1 mg/ml. The rotation along the minor axis as measured with the same method is DR = // 1.5 × 106 sec-1 at 0.1 mg/ml. The rotation along the major axis as measured on fibrinogen labeled with dansylchloride is DR// = 1.5 x106 sec–1. S is also strongly dependent on concentration, being 7.9 S at 0.1 mg/ml, 8.1 S at 1 mg/ml and 6.6 S at 10 mg/ml.These results fit with an elongated molecule having an axial ratio of 7. They are compatible with a MW of 340’000 only for concentrations above 2 mg/ml, while at lower concentrations (0.1 mg/ml) they agree with a MW of approximately half the accepted value.

1979 ◽  
Vol 41 (04) ◽  
pp. 648-654 ◽  
Author(s):  
Eugene N Serrallach ◽  
Victor E Hofmann ◽  
Martin Zulauf ◽  
Thomas Binkert ◽  
Robert Hofmann ◽  
...  

SummaryThere is no general agreement on the size and shape of the fibrinogen molecule. We have studied the diffusion of the fibrinogen in solution by means of dynamic light scattering, nanosecond fluorescence depolarization and analytical ultracentrifugation. The results obtained under physiological concentration, pH an ionic strength are DT = 2.0 × 10-7 cm2sec-1, DR⊥ = 40’000 sec-1. Nanosecond fluorescence depolarization yielded DR// = 1.6 × 106 sec-1. Tentatively this value is interpreted as DR//, namely rotational diffusion about the major axis of the molecule. The sedimentation coefficient is 8.1 S. The hydrodynamic parameters derived from our measurements were compared with those calculated on the basis of the models proposed by Hall and Slayter, Hudry-Clergeon and Marguerie et al., Bachmann and Lederer, and Köppel.The agreement is poor even if the degree of hydration is varied within wide limits. However, satisfactory agreement can be achieved by assuming a flexible molecule of about 900 Å length corresponding to two end-to-end bound trinodular structures of the Hall and Slayter type, with a nodule diameter of about 45 Å. Experimental evidence indicates that the discrepancies between the different models might be due to different techniques of sample preparation leading to different conformations of the molecule.


Fractal colloid aggregates are studied with both static and dynamic light scattering. The dynamic light scattering data are scaled onto a single master curve, whose shape is sensitive to the structure of the aggregates and their mass distribution. By using the structure factor determined from computer-simulated aggregates, and including the effects of rotational diffusion, we predict the shape of the master curve for different cluster distributions. Excellent agreement is found between our predictions and the data for the two limiting régimes, diffusion-limited and reaction-limited colloid aggregation. Furthermore, using data from several completely different colloids, we find that the shapes of the master curves are identical for each régime. In addition, the cluster fractal dimensions and the aggregation kinetics are identical in each régime. This provides convincing experimental evidence of the universality of these two régimes of colloid aggregation.


Langmuir ◽  
2010 ◽  
Vol 26 (15) ◽  
pp. 12740-12747 ◽  
Author(s):  
James B. Falabella ◽  
Tae Joon Cho ◽  
Dean C. Ripple ◽  
Vincent A. Hackley ◽  
Michael J. Tarlov

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