The largest database of trusted experimental protocols

Saxsess

Manufactured by Anton Paar
Sourced in Austria

The SAXSess is a small-angle X-ray scattering (SAXS) instrument designed for material characterization. It measures the scattering of X-rays by a sample, providing information about the size, shape, and structure of nanometer-scale particles or structures within the material. The SAXSess is capable of analyzing a wide range of materials, including polymers, proteins, nanoparticles, and more.

Automatically generated - may contain errors

15 protocols using saxsess

1

SAXS Analysis of Precursor Solution

Check if the same lab product or an alternative is used in the 5 most similar protocols
Room temperature studies of the precursor solution were performed on a SAXSess instrument from Anton Paar (Graz, Austria). The instrument was equipped with a Cu Kα X-ray source (λ = 1.54 Å) operated in line collimation mode. Samples were filled into a quartz capillary flow cell and data were collected at 25 °C using imaging plates from Fujifilm (Greenwood, SC, USA), which were read by a cyclone scanner from PerkinElmer (Covina, CA, USA). One-dimensional corrected and reduced scattering profiles I(q) as a function of the absolute value of the scattering vector q, with q = 4π/λ sin(θ/2), where θ is the scattering angle, were obtained using Anton Paar’s SAXSquant 2D and 1D software, including the subtraction of the dark current and the empty cell scattering. To normalize the data to an absolute scale, water was used as a secondary calibration standard [57 (link)]. The scattering data were analyzed using SasView version 5.0.4, with slit-smearing accounted for in the fit model. Alternatively, the slit-smeared data were desmeared using SAXSquant 2.0.
+ Open protocol
+ Expand
2

SAXS Characterization of Dispersions

Check if the same lab product or an alternative is used in the 5 most similar protocols
SAXS measurements were performed in a flow-through capillary with a Kratky-type instrument (SAXSess from Anton Paar, Austria) at 294 1 K. The SAXSess has a low sample-to-detector distance of 0.309 m, which is appropriate for investigation of dispersions with low scattering intensities. The samples were measured as delivered after vortexing for 3 min. The measured intensity was converted to an absolute scale according to Orthaber et al. (2000 ▸ ). The scattering vector magnitude q depends on the wavelength λ of the radiation (λ = 0.154 nm) as q = (4πn/λ)sinθ. Deconvolution (slit length desmearing) of the SAXS curves was performed with the SAXS-Quant software (Anton Paar). Samples analysed with SAXS were used as prepared. Curve fitting was conducted with the software SASfit (Bressler et al., 2015 ▸ ).
+ Open protocol
+ Expand
3

SAXS Analysis of Holoenzyme Complex

Check if the same lab product or an alternative is used in the 5 most similar protocols
Holoenzymes were purified as described above and the final buffer composition was 10 mM Mops pH 7, 50 mM NaCl, 2 mM MgCl2, 1 mM TCEP-HCl and 0.2 mM ATP. Immediately prior to the SAXS experiments purified holoenzyme complexes were concentrated to a final concentration of ~8-12 mg/ml using using 30,000 MWCO Millipore concentrators then filtered using 0.2 micron Z-spin microfuge filters. The SAXS data were collected for 90 min for the wild-type and mutant samples. SAXS data were acquired at 12 °C using the SAXSess (Anton Paar) line collimation (10 mm) instrument at the University of Utah. Data were collected using an image plate detector and normalized buffer subtraction and data reduction to I(q) versus q (q = (4πsinθ)/λ; 2θ is the scattering angle; λ = 1.54 Å CuKα) was carried out using the program SAXSquant 2.0. P(r) functions for the experimental and theoretical scattering were calculated using GNOM (as implemented in ATSAS 2.5.0; [42 ]). The experimental scattering data were corrected for smearing effects in GNOM using beam length profile parameters measured at the time of protein data collection. The theoretical scattering profile for the Δ366-379 RIα2:C2 complex crystal structure was calculated using CRYSOL.
+ Open protocol
+ Expand
4

Multi-Technique Characterization of Materials

Check if the same lab product or an alternative is used in the 5 most similar protocols
Solid-state 13C NMR spectra were recorded on a Agilent 400/54 Premium Shielded NMR spectrometer equipped with a CP/MAS probe. High resolution transmission electron microscopy (HRTEM) images were obtained by means of a JEOL JEM 2100 operating at 200 kV. FT-IR measurements were carried out using Thermo scientific NICOLET iS10. Brunauer-Emmet-Teller (BET) surface area analysis was conducted using a Belsorp-Max (BEL Japan. Inc.) analyzer. Pore size distribution was obtained using the Barret-Joyner-Halenda (BJH) model on the adsorption branch. Small angle X-ray scattering was analyzed with an Anton Paar SAXSess (Cu Kα radiation, λ = 1.54 Å). Fluorescence spectra measurements were performed with the use of a Perkin Elmer LS 45 luminescence spectrometer equipped with a 10 mm quartz emission cuvette from Helma.
+ Open protocol
+ Expand
5

Small-Angle X-ray Scattering Analysis

Check if the same lab product or an alternative is used in the 5 most similar protocols
SAXS measurements
were performed by SAXSess (Anton-Paar, Austria, Cu Kα, λ
= 0.154 nm), in which samples were sealed in quartz capillary tubes.
+ Open protocol
+ Expand
6

SAXS Analysis of TMAT-AuNPs

Check if the same lab product or an alternative is used in the 5 most similar protocols
The core diameters of the TMAT-AuNPs were determined in solution using SAXS measured on an Anton Paar SAXSess instrument. Samples for SAXS were prepared at about 250–500 mg/l and exposed to X-rays from a Long Fine Focal spot (LFF) sealed X-rays tube (Cu 1.54 Å) powered by a generator at 2kW, using in-line collimation mode, monochromatized and focused by multilayer optics, measured with a Roper CCD in a Kratky camera. An average of 50 scans of 50 s was used for these samples. Both the background and dark current were subtracted before desmearing using the beam profile generated by the transmitted beam in an Anton Paar SAXSQuant. The size distribution was determined by the desmeared data fitted in the IRENA package for IGOR Pro (Ilavsky and Jemian, 2009 ).
+ Open protocol
+ Expand
7

XRD Analysis of Blend and Hybrid Composites

Check if the same lab product or an alternative is used in the 5 most similar protocols
The XRD profiles of the blend and hybrid composites were measured using an Anton Paar SAXSess (Anton Paar, Graz, Austria) instrument operating at 40 kV and 50 mA in line collimation. The radiation was Cu Kα radiation with a wavelength of 0.154 nm and the exposure time of the sample was 10 min. Scattering radiation was detected in a 2θ = 5–90° rate of 1 s per step.
+ Open protocol
+ Expand
8

SAXS Analysis of β-CD and Dodecane Precipitates

Check if the same lab product or an alternative is used in the 5 most similar protocols
The SAXS measurement of the β-CD power and lyophilized dodecane/β-CD precipitates was conducted on a high-flux small-angle X-ray scattering instrument (SAXSess, Anton Paar) equipped with a Kratky blockcollimation system. A Philips PW3830 sealed-tube X-ray generator (Cu Kα) was employed to simultaneously measure the small-angle and wide-angle X-ray scattering (WAXS and SAXS) of the samples. The scanning patterns extend to the high-angle range (the q range covered by the imaging plate is from 0.0 to 27.2 nm−1, q = 4πsinθ/λ, where λ is the wavelength of 0.1542 nm and 2θ is the scattering angle). The scattering angles were calibrated with aluminum.
+ Open protocol
+ Expand
9

Liquid Crystalline Nanostructure Analysis

Check if the same lab product or an alternative is used in the 5 most similar protocols
The liquid crystalline phase of the LLC gel was observed by cross-polarized microscopy (CPM, MP41, Mshot, China) with a heat stage (KER3100-08S Mshot, China) thermostatically at 37 ± 0.5 °C or heated from 25 to 40 °C at a rate of 2 °C/min.
Further phase identification and structure analysis of crystalline cell nanostructure were performed with small angle X-ray scattering (SAXS, SAXSess, Anton Paar, UK) at 37 ± 0.5 °C. The gel sample was wrapped in aluminum foil and fixed in a sample holder. The wavelength of the X-ray radiated by a Cu Kα emitter under 50 kV and 40 mA was 0.1542 nm. The scattering factor q of Bragg peaks was set from 0.04 to 4.00 nm−1. The specific parameters of crystalline cell were calculated by the following equations (Caboi et al., 2001 (link)):
q=(4πsinθ)/λ
d=2π/q
a=(h2+k2+l2)1/2d
where 2θ is the scattering angle and λ is the wavelength of 0.1542 nm, d is the crystalline inter-planar space of liquid crystalline phase, a is crystalline lattice parameter which indicates the size of water channels in the liquid crystalline cell nanostructure, h, k, and l are Ptolemy indexes and have no dimension.
+ Open protocol
+ Expand
10

Small-Angle X-Ray Scattering of RNA

Check if the same lab product or an alternative is used in the 5 most similar protocols
SAXS data was measured using a SAXSess (Anton Paar) laboratory SAXS instrument. 100-μl samples of E1-GArN (1.86 mg/ml) or E1-GArM (1.73 mg/ml) were measured in and blanked against RNAase-free water (Promega) with exposure times of 20 min each. The scattering curves were monitored during the long exposure time as a test for radiation damage, which was not found to be an issue in this case. The SAXS data were normalized for concentration and an indirect Fourier transform performed using the program Gnom48 . The mean square radius of the cross-section (R2cs) of the RNA is descriptive of the degree of secondary structure or self-association. R2cs was measured in a Q range between 0.7 and 1.7 nm−1 (ref. 49 ).
+ Open protocol
+ Expand

About PubCompare

Our mission is to provide scientists with the largest repository of trustworthy protocols and intelligent analytical tools, thereby offering them extensive information to design robust protocols aimed at minimizing the risk of failures.

We believe that the most crucial aspect is to grant scientists access to a wide range of reliable sources and new useful tools that surpass human capabilities.

However, we trust in allowing scientists to determine how to construct their own protocols based on this information, as they are the experts in their field.

Ready to get started?

Sign up for free.
Registration takes 20 seconds.
Available from any computer
No download required

Sign up now

Revolutionizing how scientists
search and build protocols!