ULTRA SMALL-ANGLE X-RAY SCATTERING STUDY OF FLOCCULATION IN SILICA-FILLED RUBBER

2014 ◽  
Vol 87 (2) ◽  
pp. 348-359 ◽  
Author(s):  
Satoshi Mihara ◽  
Rabin N. Datta ◽  
Wilma K. Dierkes ◽  
Jacques W. M. Noordermeer ◽  
Naoya Amino ◽  
...  

ABSTRACT The flocculation of silica during vulcanization is monitored using the ultra small-angle X-ray scattering technique for two different types of silica: a highly dispersible silica (HD) and a conventional silica (CV), mixed into a blend of S-SBR and BR rubbers. The cutoff length of the silica aggregate Rss and the mass fractal dimension Dm, which indicate the degree of flocculation of aggregates, are estimated according to the modified unified equation. The aggregate radius Ra is estimated to be related to the lower cutoff length Rss, indicating the radius of gyration of the mass-fractal structure. For both silicas, Ra increases during vulcanization. For the CV silica, an increase of Dm is observed, whereas no significant increase of Dm can be seen for the HD silica. The Ra of CV is relatively high compared with that of HD. On the other hand, the CV silica shows a relatively lower Dm compared with that of HD. These results indicate that CV has a larger size of aggregates and lower degree of agglomeration of its aggregates. The presence of di(tri-ethoxy-silyl-propyl)tetrasulfide (TESPT) as coupling agent between the silica and rubber decreases the aggregate radius of silica. However, in the absence of TESPT, a low mass-fractal dimension, which means a low degree of agglomeration of aggregates, is observed. This results from a lower mobility of silica aggregates, depending on the size of the aggregates. The silica loading also has an influence on the flocculation process. The aggregate radius increases as the silica loading is increased. At the same time, a higher mass-fractal dimension, and therefore also a higher degree of agglomeration, can be seen at higher silica loading.

Biochemistry ◽  
1985 ◽  
Vol 24 (24) ◽  
pp. 6740-6743 ◽  
Author(s):  
B. A. Seaton ◽  
J. F. Head ◽  
D. M. Engelman ◽  
F. M. Richards

1988 ◽  
Vol 43 (5-6) ◽  
pp. 373-376 ◽  
Author(s):  
P. M. Abuja ◽  
I. Pilz

The quaternary structure of ribulose-1,5-bisphosphate carboxylase/oxygenase from tobacco (Nicotiana tabacum) was investigated in solution by means of small angle X-ray scattering. The most important molecular parameters as the radius of gyration (Rg) and the maximum diameter (Dmax) were determined. Both the active and the inactive form of the enzyme were measured at 5 °C and at 20 °C. A more distinct difference in size could be detected between the inactive forms at these two temperatures (Rg = 4.80 nm (5 °C) and 4.68 nm (20 °C)) than between the active forms (Rg = 4.73 nm and 4.69 nm). The maximum diameters were determined to be 13.1 nm for the inactive form at 5 °C and 12.8 nm for the other forms. A model is proposed consisting of eight large and eight small subunits arranged in the way that seems to be typical for this enzyme in higher plants.


2005 ◽  
Vol 38 (1) ◽  
pp. 132-138 ◽  
Author(s):  
Artur Braun ◽  
Jan Ilavsky ◽  
Brian C. Dunn ◽  
Pete R. Jemian ◽  
Frank E. Huggins ◽  
...  

Monolithic silica aerogels with radial symmetry were synthesized by supercritical drying, doped to 2% and 10% with cobalt, and reduced with hydrogen. All samples were investigated with ultra-small-angle X-ray scattering. The non-doped aerogels have three populations of scatterers with radii of gyration of about 10, 40 and 60–70 Å. The doped aerogels show an additional structure with a radius of gyration ranging from 1050 to 3000 Å. This structure causes intensity oscillations, thus revealing a relatively narrow size distribution. Scattering curves of the 10%-doped aerogels fitted well to a Lifshitz–Slyozov–Wagner particle size distribution, thus revealing that Ostwald ripening might have occurred during aerogel preparation. The same range also shows differences depending on whether the samples were reduced, or in their as-prepared condition. Scattering curves obtained from the cylinder-axis region were different from the scattering curves obtained from the sample boundary, indicating a process-dependent skin effect.


2016 ◽  
Vol 49 (5) ◽  
pp. 1412-1419 ◽  
Author(s):  
Christopher D. Putnam

The Guinier region in small-angle X-ray scattering (SAXS) defines the radius of gyration,Rg, and the forward scattering intensity,I(0). In Guinier peak analysis (GPA), the plot ofqI(q)versus q2transforms the Guinier region into a characteristic peak for visual and automated inspection of data. Deviations of the peak position from the theoretical position in dimensionless GPA plots can suggest parameter errors, problematic low-resolution data, some kinds of intermolecular interactions or elongated scatters. To facilitate automated analysis by GPA, the elongation ratio (ER), which is the ratio of the areas in the pair-distribution functionP(r) after and before theP(r) maximum, was characterized; symmetric samples have ER values around 1, and samples with ER values greater than 5 tend to be outliers in GPA analysis. Use of GPA+ER can be a helpful addition to SAXS data analysis pipelines.


2021 ◽  
Vol 21 (1) ◽  
pp. 538-546
Author(s):  
Baisheng Nie ◽  
Kedi Wang ◽  
Yu Fan ◽  
Junsheng Zhao ◽  
Letong Zhang ◽  
...  

The complexity and multiscale structure of coal pores significantly influence the gas diffusion and seepage characteristics of coal. To apply small angle X-ray scattering (SAXS) to study the coal pore structure parameters within the scale of 1–100 nm in the methane adsorption process, the X-ray window was optimized and a gas adsorption chamber was designed to interface with the small angle X-ray scattering platform. The fractal dimension and porosity of Hami coal samples under different methane pressures were studied using the small angle X-ray scattering platform and adsorption chamber. The surface and nanopore fractal information of the nanopores in coal were distinguished. The variation trends of the pores and surface fractal dimension with time under the same methane pressure were compared. The results indicate that the surface dimension changes from 2.56 to 2.75, and the extremum point may indicate that the primary nanopore structure is crushed by the adsorbed gas after approximately 15 minutes. This work clarifies that the fractal dimension can characterize the changes in nanopores in the process of gas adsorption by using SAXS. According to the fractal characteristics, the adsorption of gas in coal nanopores is summarized as four steps: expansion from adsorbance, deformation, crushing and recombination. The minimum porosity is 0.95% and the extreme value point is 1.47%. This work also shows that decrease in surface energy affect the porosity changes in nano-size pores. This work is of some significance to coalbed methane permeability improvement and gas extraction.


1971 ◽  
Vol 4 (4) ◽  
pp. 317-318 ◽  
Author(s):  
I. Simon

A differential method is presented for the evaluation of small-angle X-ray scattering data. The direct determination of slight changes in the radius of gyration of colloid particles is rendered possible by the method proposed.


1982 ◽  
Vol 37 (9) ◽  
pp. 824-832 ◽  
Author(s):  
Peter Zipper ◽  
Gertraud Ribitsch ◽  
Josef Schurz ◽  
Hans Bünemann

The binding of Hg2+ and 3,6-bis-(acetatomercurimethyl)-dioxane (BAMD) to sonicated calf thymus DNA was studied by small-angle X-ray scattering and viscosity measurements. The scat­tering experiments with DNA complexed by different amounts of mercurials (for Hg2+ rb = 0-0.79, for BAMD rb = 0-0.86 mol of mercurial bound per mol of base pairs) established that the rod-like character of the DNA molecules is maintained up to high binding ratios. They revealed further a steady decrease of the cross-section radius of gyration Rc for the DNA · Hg2+ complex and a similar decrease of Rc for the DNA · BAMD complex up to rb = 0.35. This behav­iour is certainly caused by the incorporation of both mercurials near the axis of the DNA helix. Binding of BAMD at rb > 0.35 led to an increase of Rc which behaviour obviously reflects the lo­cation of mercury atoms at large distances from the axis, possibly on the surface of the helix. The increase of the mass per unit length Mc upon binding of the mercurials was found to be much higher than expected. This finding established that the length of the DNA helix decreases by 0.10±0.01 nm per bound mercurial at low binding ratios (i.e. up to rb = 1/3 for BAMD, up to possibly rb = 0.5 for Hg2+). A similar conclusion was also drawn from the observed decrease of intrinsic viscosity [rj] with increasing rb. The analysis of Mc at high binding ratios suggests that every BAMD molecule bound beyond rb=1/3 decreases the length of the DNA by 0.21 ±0.05 nm whereas Hg2+ when bound beyond rb = 0.5 causes no change of the length.


Langmuir ◽  
2000 ◽  
Vol 16 (13) ◽  
pp. 5588-5592 ◽  
Author(s):  
Thomas P. Rieker ◽  
Manuela Hindermann-Bischoff ◽  
Françoise Ehrburger-Dolle

Blood ◽  
2016 ◽  
Vol 128 (22) ◽  
pp. 254-254
Author(s):  
Jian Zhu ◽  
Joshua Muia ◽  
Louis Deforche ◽  
Karen Vanhoorelbeke ◽  
Niraj H. Tolia ◽  
...  

Abstract Introduction: ADAMTS13 is a multidomain protein with metalloprotease (M), disintegrin-like (D), thrombospondin-1 (T), Cys-rich (C) and spacer (S) domains, followed by 7 T domains and 2 CUB domains. ADAMTS13 cleaves the cryptic Tyr1605-Met1606 bond in the A2 domain of von Willebrand factor (VWF), which inhibits the growth of platelet-rich thrombi. When subjected to tensile stress in solution, bound to platelets, or on endothelial cell surfaces, VWF interacts with multiple exosites on ADAMTS13, changing the conformation of both proteins. These close contacts enhance the specific interaction between ADAMTS13 and VWF in vivo. Interactions between VWF and proximal MDTCS domains of ADAMTS13 have been investigated extensively. ADAMTS13 distal domains T8-CUB2 are required to bind the D4 domain of VWF, and the CUB domains promote the cleavage of platelet-decorated VWF strings. Using mutagenesis, small-angle X-ray scattering (SAXS) and enzyme kinetics, we have shown that ADAMTS13 adopts a folded conformation with distal T8-CUB2 domains close to the proximal MDTCS domains and a hinge point between the T4 and T5 domains. We have used internal deletions of T domains to identify a possible "minimal" structure for a functional and stably folded ADAMTS13. Methods: Recombinant human hADAMTS13, pigeon pADAMTS13, and various T domain deletion mutations were produced in T-Rex 293 cell lines and purified to homogeneity. Similar inactive variants of each protein were prepared with the mutation E225Q, which abolishes catalytic activity but does not affect protein folding. SAXS data were collected at the SIBYLS beamline (Lawrence Berkeley National Laboratory) for ADAMTS13 and deletion variants. The radius of gyration (Rg) and maximum particle size (Dmax) were calculated from scattering profiles using DATGNOM. Ab initio envelopes were generated from scattering profiles using DAMMIN. A molecular model of ADAMTS13 was built from crystal structures of ADAMTS4 MD domains (2rjp) and ADAMTS13 DTCS domains (3ghm), and using HHpred to model distal T domains, CUB domains, and linkers after T4 and T8. ADAMTS13 activity assays were performed at pH 6.0 and pH 7.4 with the fluorogenic substrate FRETS-rVWF71. Monoclonal antibodies (Mabs) against different distal domains of ADAMTS13 and recombinant VWF D4 domain were added to assess allosteric activation. Results: Rg and Dmax of ADAMTS13 variants are shown in Table 1. For Del4L, with deletion of linker region between T4 and T5, values of Rg and Dmax are ~5% smaller than for full length ADAMTS13. Deletion of both T4 and the linker region (Del4pL), reduced Rg and Dmax ~10%. Deletions of distal domains (Del7, Del8, Del8L, and Del8pL) that are spatially close to the proximal domains increased Rg and Dmax ~14%, which is consistent with partial unfolding of the condensed full length ADAMTS13 structure. Del2to8, which lacks all distal T domains between S and CUBs, aggregated in solution. Del2to7, which retains only T8, has Rg and Dmax 15% and 17% smaller than ADAMTS13, respectively. The kcat values for all variants at pH 7.4 are consistent with autoinhibition of the proximal MDTCS domains by any remaining distal domains. The additional of Mabs recognizing T7, T8 and CUBs slightly (~1.5 fold) activated individual deletion mutants. Del2to7, Del2to8, and Del3to6 had similar activities when compared with ADAMTS13. Though Del2to7 and Del3to6 could be activated by Mabs ~3 fold, only Del3to6 could be activated slightly ~1.3-fold by D4 domain, compared to 1.8-fold activation of hADAMTS13. pADAMTS13 is structurally similar to human Del3to6, and was activated by D4 domain ~4 fold but not by Mabs. Fitting to the ab initio envelopes show a folded conformation for hADAMTS13, Del7, Del8 and Del8L (Figure 1), consistent with a hinge in the flexible linker after T4. pADAMTS13 and Del2to7 had more compact envelopes, consistent with removal of most of the folded segment present in full length hADAMTS13. Conclusions: Deletion of individual distal T domains does not relieve the autoinhibition of ADAMTS13. Del3to6 is the only human deletion mutant examined that can be activated by both Mabs and VWF D4 domain, similar to hADAMTS13. pADAMTS13 is structurally similar to Del3to6, retains normal activation by VWF D4, and shows a SAXS envelope consistent with a truncated version of hADAMTS13. Our findings suggest that Del3to6 and pADAMTS13 represent the "minimal" structure of allosterically-regulated, functional ADAMTS13. Disclosures Sadler: Ablynx: Consultancy; 23andMe: Consultancy; BioMarin: Consultancy.


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