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X pert diffractometer

Manufactured by Philips
Sourced in Netherlands, Germany, United Kingdom

The X'Pert diffractometer is an analytical instrument used for X-ray diffraction (XRD) analysis. It is designed to provide detailed information about the structural and compositional characteristics of solid materials. The X'Pert diffractometer measures the intensity of X-rays reflected or scattered from the surface of a sample at different angles, producing a diffraction pattern that can be used to identify the crystalline phases present in the material.

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107 protocols using x pert diffractometer

1

X-ray Diffraction Analysis of Samples

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X-ray diffraction (XRD) measurements were aquired using a diffractometer model (Type PHILIPS X’ Pert Diffractometer) having a Cukα (λ = 0.154056 nm) at room temperature. The diffraction patterns were recorded automatically with scanning speed (4°/min) and chart speed (20 mm/min). The X-ray diffraction patterns were investigated in the range of 2θ between 4° and 60°.
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2

Preparing Biomass Samples for XRD Analysis

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Samples for XRD analysis are based on the biomass separated from an aliquot. A detailed description of this process was previously31 (link) given. Finally, the biomass was placed as thin and as homogeneous as possible on a homemade sample holder. The sample holder consists of a 1 mm thick and 25 mm diameter Si(977) single crystal mounted in a 32 mm diameter and 4 mm thick plate of polycarbonate, which fits directly to the support of the Phillips X-pert diffractometer employed for the X-ray diffraction measurements.
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3

X-Ray Diffraction Analysis of Fiber Ash

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The XRD analysis of fiber ash and unprocessed fiber was carried out using the Phillips X'Pert diffractometer. The fiber ash particulate were pressed into metal disks using a steel mould cylinder of 15 mm diameter and pressure of 20 MPa. The diffraction was measured between 5o and 50o at 40 kV and 50 mA [21 ].
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4

Characterization of MFM-300(VIII) Membrane

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The purity of MFM-300(VIII) was confirmed by powder X-ray diffraction before loading into the MMM. The membrane morphology was studied by scanning electron microscopy (SEM) using a Hitachi S-4800 Field-Emission Scanning Electron Microscope with Energy Dispersive X-ray (EDX) detector and cold cathode electron source. The membrane cross section was prepared via freeze fracturing using liquid N2. The sample was then coated with gold via sputtering using an Emitech coater. PXRD analysis was also carried out on a Philips X'Pert diffractometer to ensure retention of the crystallinity of the MOF once incorporated into the membrane.
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5

X-Ray Powder Diffraction of Crystalline Formulations

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XRPD was used for characterizing crystalline materials and providing information on structures. The dust and surface sweep method were used. Approximately 20 mg of sample was dispersed on a sample holder and loaded into a Philips X’PERT® diffractometer equipment. Each sample was exposed to Cu-kα radiation, the angles of incidence being from 5° to 50°. The test conditions are 40 mV voltage and 55 mA intensity. The diffractograms obtained from the raw materials (MLX, lactose, Metolose® and Eudragit®) and the CNM formulation and its placebo make it possible to know if the samples are crystalline or amorphous. GID method has also been used, which consists in that the angle of incidence (θ) remains fixed while the detector moves normally around the axis of the goniometer [38 (link)]. GID is a surface-sensitive technique that, allows the characterization of epitaxial films with thicknesses down to a few atomic layers. All measurements were made with a Philips X’PERT® diffractometer, where the radiation was the same as for the measurements by the powder method. In this study, we have used an incidence angle (θ) of 1°. Before the measurements, the equipment was carefully aligned and calibrated. A spatial sample holder was used that could be adjusted to the height of the sample. Under these conditions, the CNM formulation was measured.
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6

Comprehensive Material Characterization by SEM, TEM, XRD, and XPS

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The morphology of the samples was characterized by field emission SEM using a JEOL JSM7001F FE-SEM equipped with an EDS. Transmission electron microscopy and SAED were performed using a JEOL JEM-2010 Plus TEM. XRD patterns were acquired using a Philips X' Pert diffractometer equipped with a Cu Kα radiation source (λ = 0.15406 nm). XPS was performed in a VG Escalab 220i-XL equipped with a hemispherical analyzer recorded for a twin anode X-ray source. The fine structure of the photoelectron lines was analyzed using Casa XPS software (2.3.19 version).
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7

Characterization of SnO2 Nanoparticles

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SnO2 nanoparticles were analyzed by X-ray diffraction (XRD) performed on a Philips X’Pert diffractometer (2θ from 20° to 80°, λ = 1.5406 Å) with Cu Kα radiation. Micromorphology and element distribution of pure SnO2 and Pt-decorated SnO2 were characterized by field emission scanning electron microscopy (FE-SEM, Hitachi S-4800, Tokyo, Japan) and an energy dispersive spectrometer (EDS, Hitachi S-4800, Tokyo, Japan). TEM images were obtained by a JEOL 2100F microscope (Tokyo, Japan). The X-ray photoelectron spectroscopy (XPS) test was conducted by a Kratos XSAM800 spectrometer (Manchester, England).
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8

Advanced Characterization of Novel Materials

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FT-IR spectra were recorded on a Bruker ALPHA spectrometer from 500 to 4000 cm−1 using KBr pellets. UV-Vis spectra were recorded on a PerkinElmer LAMBDA 25 spectrophotometer. XRD patterns were recorded on a Philips X'pert diffractometer with mono chromatized Cu Kα radiation at 40 kV and 20 mA (Ni filter, 2θ 10 to 70° with a step size of 0.05° and a count time of 1 s). TEM images were obtained on a transmission electron microscope (TEM, Philips MC 10) with an acceleration voltage of 80 kV. Thermogravimetric analysis (TGA) was performed on a STA 1500 instrument at a heating rate of 10 °C min−1 in air atmosphere. GC analyses were performed on a GC Chrom from Teif Gostar Faraz Co., Iran (split/splitless injector, capillary SAB-5 column, FID detector, N2 as carrier gas with flow rate of 0.8 mL min−1, column temp: 260 °C).
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9

Physicochemical Characterization of Nanomaterials

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X-ray powder diffraction (XRD) patterns were acquired on a PHILIPS X’PERT diffractometer using Cu Kα radiation. The data were recorded from 5° to 50° (2θ) with a resolution of 0.01°. Scanning electron microscopy (SEM) micrographs were obtained on a XL30 ESEM (Philips, Lelyweg, the Netherlands) electronic microscope operating at 200 kV. Nitrogen adsorption–desorption isotherms at −196 °C were measured using an AutoSorb equipment (Quantachrome Instruments, Boynton Beach, Florida, USA). Samples were degassed at 150 °C and high vacuum during 180 h. The micropore surface area was calculated by using the Brunauer–Emmett–Teller (BET) model [37 (link)]. The pore volume and diameter were estimated by non-local DFT calculations, assuming a kernel model of N2 at −196 °C on carbon (cylindrical pores, NL-DFT equilibrium model) [38 (link)] and external surface was estimated by t-plot method and Harkins Jura equation [39 (link)]. Simultaneous thermogravimetry and derivative thermogravimetric analyses (TGA/DTG) were carried out under a nitrogen atmosphere with an N2 flow of 100 mL·min−1 at a heating rate of 5 °C/min up to 700 °C, using a SDT 2860 apparatus (TA Instruments, New Castle, DE, USA).
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10

Characterization of N-Doped Graphene Powders

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The phase composition of the as-prepared powders was analyzed by powder X-ray diffraction (XRD) analyses (Philips X’ Pert diffractometer) with CuKα radiation. Environmental scanning electron microscopy (ESEM, Helios Nanolab 600i) and high-resolution transmission electron microscopy (HRTEM JEM-2100) were used to observe the morphology of the graphene sheets. The TEM specimens were prepared by dropping ethanol/water (38 v/v%) solution containing 1 wt % N-doped graphene onto a copper grid and drying at 100 °C. Raman spectra were obtained using a Raman Station (B&WTEK, BWS435-532SY) with a 532 nm wavelength laser corresponding to 2.34 eV, 30% of the laser power (total power: 240 mW) was used on the samples. X-ray photoelectron spectroscopy (XPS, Thermo Fisher) was utilized to determine the bonding characteristics of the samples. All XPS peaks are calibrated according to the C 1 s peak (284.6 eV). The composition was confirmed using X-ray fluorescence (XRF, AXIOS-PW4400) in order to determine the presence of any metallic elements. 2 milligrams of N-doped graphene powder was spread out on the surface of boric acid powder (99.0%, Sinopharm Chemical Reagent Co., Ltd.), the effective test zone is a disk surface with a diameter of 20 mm. The magnetic properties were measured using a Quantum Design MPMS magnetometer based on a superconducting quantum interference device (SQUID).
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