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Micromax 003

Manufactured by Rigaku
Sourced in Japan

The Micromax-003 is a compact X-ray diffractometer designed for the analysis of small samples. It features a sealed tube X-ray source, a goniometer, and a detector. The instrument is capable of collecting high-quality X-ray diffraction data from a variety of sample types, including powders, thin films, and single crystals.

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10 protocols using micromax 003

1

Peptide Fiber Formation and X-ray Analysis

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In an Eppendorf tube, 2 mg of peptide powder were dissolved in 0.8 mL of water. The solution was vortexed at room temperature. The resulting cloudy solution was allowed to settle for 7 days to form fibers, after which the tube was spun down and the aqueous solvent was decanted. Residual water was further removed slowly in a dehydration chamber. After 48 h, the dehydrated fibers were cryo-protected in 30% glycerol and flash-frozen in liquid nitrogen. The fiber X-ray diffraction pattern was collected using an in-house sealed tube microfocus X-ray generator (Micro-Max-003, Rigaku Corporation) with Saturn944 CCD and Cu Kα (1.54 Å) radiation at 100 K. This result is shown in Figure 3B. In another experiment, TDP-43(341–357) fibers were prepared as previously described, except that they were left in the dehydration chamber for 24 h. The resulting fibers were analyzed with an X-ray powder diffractometer (PANalytical X’Pert 3) on a spinning sample holder. The data were collected over a 2θ range from 1 to 50°. This is result is shown in Figure S10 in the SI.
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2

Small- and Near-Wide-Angle X-Ray Scattering

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Small- and near wide-angle X-ray scattering (SAXS/NWAXS) measurements were performed using a point-focusing SAXS instrument (originally Molecular Metrology, recently considerably upgraded by SAXSLAB, now Xenocs) at room temperature. Rigaku Micromax-003, a low-power micro source equipped with X-ray optics working at U = 50 kV and I = 0.6 mA generated a CuKα beam with a wavelength of λ = 0.154 nm. Scattering was detected by the 2D detector Pilatus3 300K (Dectris) at 0.449 m and 0.0573 m from the sample. Merging data from these two distances allowed reaching reliable q interval from 0.13 to 35 nm-1, where q is the magnitude of the scattering vector q = 4π sin(θ)/λ and θ is half of the scattering angle. Samples were sealed in 1.5 mm-diameter quartz capillaries (the scattering of an empty capillary was not subtracted from the scattering curves of samples). Sample to detector distance was calibrated using silver behenate or Si standard. Data were azimuthally averaged and adjusted to an absolute scale using a glassy carbon standard.
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3

Structural Analysis of SETD2-H3K36M Complexes

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X-ray diffraction data set on a SETD2-SAM-H3K36M complex crystal was collected using a Saturn944HG CCD mounted on a Rigaku Micromax-003 X-ray generator. X-ray diffraction data set on a SETD2-SAH-H3K36M complex crystal was collected at the Advanced Photon Source beamline NE-CAT 24-ID-E using an ADSC Q315r detector. The diffraction images were processed and scaled with the HKL-2000 package29 .
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4

SAXS Characterization of Thermally Induced Self-Assembly

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The SAXS data were collected using a pinhole camera (MolMet, Rigaku, Japan, modified by SAXSLAB/Xenocs) on a microfocused X-ray beam generator (Rigaku MicroMax 003) operating at 50 kV and 0.6 mA (30 W). Vacuum version of a Pilatus 300 K detector was used with the camera. Primary beam position and sample-to-detector distances were calibrated using an AgBehenate sample. Borosilicate capillaries were used as measurement containers for the samples. To cover the range of scattering vectors (q) from 0.005 to 1.100 Å−1, two experimental settings were used.
q=4πλsinθ
where 2 θ is the scattering angle, and λ is the incident wavelength.
We chose 22 °C and 40 °C as the measurement temperatures to obtain data throughout the thermally induced self-assembly process. Obtained scattering data were reduced using software based on the PyFAI Python library [42 (link)], and SASFit [43 (link)] and SASView [44 (link)] were used to fit the data.
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5

Small-Angle X-Ray Scattering of Samples

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Samples were characterized by small-angle X-ray scattering (SAXS) and near wide-angle X-ray scattering (NWAXS) at room temperature. Measurements were performed by means of the point focusing SAXS instrument (originally Molecular Metrology, recently considerably upgraded by SAXSLAB, now Xenocs). The CuKα beam with the wavelength of λ = 0.154 nm was generated by Rigaku Micromax-003, which is a low-power microsource equipped with X-ray optics working at U = 50 kV and I = 0.6 mA. Scattering was detected by the 2D detector Pilatus3 300K (Dectris) at two different distances of 0.541 and 0.052 m from the sample. After merging data from these positions, the reliable q interval from 0.13 to 35 nm−1, where q is the magnitude of the scattering vector q = 4π sin(θ)/λ and θ is half of the scattering angle, was reached. Measurements were performed in sealed capillaries of either boron glass or quartz with a diameter of 1.5 or 2 mm. Sample to detector distance was calibrated by means of a silver behenate or silicon standard. Data were azimuthally averaged and adjusted to an absolute scale using glassy carbon standard. The scattering curve of an empty capillary was subtracted from the scattering curves of samples.
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6

Structural Characterization of 14-3-3σ Bound to Ataxin pS776

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The pS776 peptide was dissolved at 10 mM in buffer containing 20 mM Hepes pH 7.4, 2 mM MgCl2 and 2 mM DTT. 14-3-3σΔC, at 377 μM (10 mg/mL), was mixed in the same buffer with the Ataxin pS776 peptide at a 1:2 molar stoichiometry and incubated overnight at 4 °C. Crystals were then obtained by hanging drop vapor diffusion in EasyXtal plates (Qiagen) by screening an in-house grid of crystallisation solutions containing 0.095 M Hepes (pH 7.1, 7.3, 7.5, 7.7), 0.19 M CaCl2, 5% glycerol, 24–29% PEG 400. Crystals were directly flash-frozen in liquid nitrogen. Diffraction data were collected using an in-house MicroMax-003 sealed tube X-ray generator and Pilatus 200 K detector (Rigaku). Data were indexed an integrated using XDS,63 (link) and then scaled using AIMLESS.64 (link), 65 (link) The structure was then solved by molecular replacement using Phaser.66 (link), 67 (link) Phenix.refine67 (link), 68 (link) and Coot69 (link) were used in alternating cycles of automatic and manual structure refinement. Figures were prepared using PyMOL.70
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7

Spectroscopic Analysis of Organic Compounds

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TLC was performed on silica gel GF254 plates (Qingdao Haiyang Chemical Co., Ltd., Qingdao, China). Compounds were visualized by irradiation with UV light or by treatment with 0.05 g/mL ninhydrin in ethanol or potassium iodide reagent. 1H-NMR and 13C-NMR were recorded on a Bruker Avance-400 MHz instrument (Bruker BioSpin AG, Fällanden, Switzerland). HRMS were obtained with a LC-ESI-Q-TOF-MS apparatus (Waters, Milford, MA, USA). HPLC analysis of GLYX-13 was performed on an Agilent LC 1100 system (Agilent Technologies Inc., Santa Clara, CA, USA) equipped with a diode array detector. Chiral analysis of intermediate were carried out using a Shimadzu LC 20AD system (SIMADZU, Kyoto, Japan) with a SPD-20A UV detector or an Agilent LC 1100 system equipped with a diode array detector. Single crystal diffraction analysis of 7 was performed on a MicroMax-003 (Rigaku Corporation, Tokyo, Japan) X-ray single crystal diffractometer and powder diffraction analysis of 7 was performed by a Bruker D8 FOCUS powder diffractometer (Bruker BioSpin AG, Fällanden, Switzerland). The L-amino acids (protected or free) were obtained from GL Biochem Ltd. (Shanghai, China). Other reagents were provided by Aladdin (Shanghai, China). The organic solvents were commercially available products (Lingfeng Chemical Reagent Co., Ltd., Shanghai, China) and were used without further purification.
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8

Wide-Angle X-Ray Scattering Protocol

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Wide-angle X-ray scattering (WAXS) experiments were performed using a pinhole camera (MolMet, Rigaku, Japan, modified by SAXSLAB/Xenocs) attached to a microfocused X-ray beam generator (Rigaku MicroMax 003) operating at 50 kV and 0.6 mA (30 W). The camera was equipped with a vacuum version of Pilatus 300K 2-dimensional detector. Calibration of primary beam position and sample-to-detector distances was performed using Si powder sample. Experimental setups covered the scattering vector, q = (4π/λ)sinΘ, where λ is the wavelength and 2Θ is the scattering angle, in the range 0.22–1.42 Å−1. Homemade software based on PyFAI Python library (doi:10.1088/1742-6596/425/20/202012) was used for data reduction. Samples were measured in reflection mode with incident beam angle set to 1.3 degree.
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9

Structural Determination of 14-3-3.12 Protein

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Unlabeled 14-3-3.12 was soaked into preformed crystals of 14-3-3σΔc, which grew in 25% PEG400, 5% Glycerol, 0.2 M CaCl2, 0.1 M HEPES pH 7.5 plus 2 mM BME within two weeks. The soaked crystal was fished after 15 days of incubation and flash-frozen in liquid nitrogen. Diffraction data was collected at 100K on an in-house Rigaku Micromax-003 (Rigaku Europe, Kemsing Sevenoaks, UK) sealed tube X-ray source and Dectris Pilatus 200K detector (DECTRIS Ltd Baden-Daettwil, Switzerland). Integration, scaling and merging of data was done using DIALS (CCP4i2) after which molecular replacement is done with MOLREP (CCP4i2) using PDB 4JC3 as search model. A three-dimensional structure of 14-3-3.12 was generated using eLBOW (Phenix) after which it was built within this structure based on visual inspection of Fo-Fc and 2FoFc electron density maps in Coot. Several rounds of model building and refinement (based on isotropic b-factors and standard set of stereo-chemical restraints: covalent bonds, angles, dihedrals, planarities, chiralities, non-bonded) were performed using Coot and Phenix.refine. See Supplementary Table 12 for data collection and refinement statistics. Structural coordinates have been deposited in the PDB (6TCH).
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10

SAXS Analysis of Liquid Crystals

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SAXS measurements were carried out on a NanoMAX-IQ instrument (Rigaku) with a Pilatus 100 K detector (Dectris), a Cu target sealed tube source (MicroMax-003, Rigaku) in vacuum and at controlled temperature (Julabo). An effective scattering-vector range of 0.008 Å À1 < q < 0.6 Å À1 was investigated and scattering images were integrated into the one-dimensional scattering function I(q). The scattering intensity is shown as a function of the momentum transfer q = 4pk -1 sin(h/2), where k is the photon wavelength of 1.524 Å and h is the scattering angle. Samples were filled into a 1.5 mm internal diameter quartz capillary and sealed with epoxy glue. The q-range was calibrated using silver behenate as the standard. The liquid crystalline space groups and lattice parameters (a) were determined by the relative positions of the Bragg peaks in the scattering curves, which correspond to the reflections on planes defined by their (hkl) Miller indices [28] .
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