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Pw 1729

Manufactured by Philips
Sourced in Netherlands, United Kingdom, United States

The PW 1729 is a laboratory equipment manufactured by Philips. It is designed for general-purpose laboratory applications. The core function of this product is to provide a reliable and precise measurement tool for laboratory analyses.

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12 protocols using pw 1729

1

Characterization of (Co, Mn) co-doped ZnO

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The crystallographic structure characteristics of the undoped and (Co, Mn) co-doped ZnO samples were performed employing an X-ray diffractometer equipment type Philips PW 1729, equipped with a monochromatic radiation source (Cukα, λ = 1.54056 Å, Philips PW 1729 system, Cambridge, MA, USA). The X-ray photoelectron spectroscopy (XPS) analyses were carried out using a Thermo-VG Scientific MultiLab, ESCA Probe with Al Kα 1486.7 eV (Fisher Scientific, Waltham, MA, USA) as an exciting source in order to identify the chemical elements and their oxidation states.
In addition, the surface morphology of the thin films has been explored by electronic scanning microscopy (class EDAX XL 30 (S.E), EDAX, Mahwah, NJ, USA). The optical properties of all the ZnO samples, in terms of the transmission (T%) and optical band gap energy (Eg), were analyzed in the 250–2500 nm range with a spectrophotometer device (type Perkin Elmer Lambda 950). The magnetic properties studies were accomplished using a vibrating sample magnetometer (VSM, Microsense EV9, DMG MORI Manufacturing USA, Inc., Davis, CA, USA). The magnetization (M) measurements were conducted at room temperature in the field range from −20 kOe to 20 kOe.
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2

Thermal and X-ray Analysis of ICIE16M Glass

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The DSC for ICIE16M glass particles was conducted to determine the glass transition temperature (Tg) and crystallization temperature (Tc) [60 (link),61 (link),62 (link),63 (link),64 (link)]. A 50 µg sample of the glass powder was heated at rates of 10 °C min−1 and 20 °C min−1 using Stanton-Redcroft DSC 1500 (PL Thermal Sciences, Epsom, UK) series. A starting temperature of 50 °C was used and final temperature of 1100 °C using a Nitrogen atmosphere.
X-ray diffraction spectrometry was performed on the samples (in powder form in silicone sample holder) using the PANalytical X'Pert Pro diffractometer (Malvern, UK) powered by Philips PW 1729 X-ray generator. Phase identification was carried out by means of the software program PANalytical High Score Plus (Version 2.2b, Malvern Panalytical Ltd, Malvern, UK). Diffraction data is acquired by exposing powder samples to Cu-Kα X-ray radiation, which has a characteristic wavelength (λ) of 1.5418 Å. X-rays were generated from a Cu anode supplied with 40 kV and a current of 40 mA.
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3

Comprehensive Characterization of Materials

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A Philips model (PW-1729, Cambridge, UK) diffractometer (with 2θ from 20° to 80°) was used to investigate the samples by X-ray diffraction. FTIR spectroscopy was used to create an FTIR spectrum in the wavenumber range from 200 cm−1 to 4000 cm−1 (Perkin Elmer 1430, Hamburg, Germany). Transmission electron microscopy (TEM) was involved in studying the microstructure of the samples (JEOL1010, Tokyo, Japan). SEM was used to investigate the morphology of the samples (JEOL JSM-6460, Tokyo, Japan). Image-J and Gatan digital micrograph software were used for calculating average pore size or pores area, the average crystallite size (D), and image processing. Thermogravimetric analyzer (TGA) characterizations were performed in the air with a 10 °C/min rate using a Perkin Elmer Top-Loading Series (STA-6000, Germany). A vibrating sample magnetometer (VSM) with operating system V1.6 control software was used to monitor magnetic hysteresis loops (Oxford OX8JTL, London, UK). Using the R–L–C Bridge (type BM591, Tokyo, Japan), the initial magnetic permeability (μi), DC resistivity (ρ), and at various frequencies, the dielectric constant (ε) was calculated as a temperature function.
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4

Crystallinity Analysis of TDF and LCP

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The crystallinity of TDF and TDF loaded LCP was determined using X-ray diffractometer (PW 1729; Philips, Almelo, Netherlands). The samples were irradiated with Cu Kα radiation (1.542 Å) between 5 and 50° 2θ with a scan speed of 0.2 s/step and a step size of 0.0388°.
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5

Quantifying Film Crystallinity via WAXD Analysis

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The film crystallinity was studied via WAXD analysis, on a Philips PW 1729 (Phillips, Eindhoven, the Netherlands), in reflection mode, using nickel-filtered Cu-Kα radiation (1.5418 Å). Hence, the degree of crystallinity of each film was calculated using the formula proposed by Hermans and Weidinger, as follows (Equation (1)) [24 (link)]: %Crystallinity=QstQamQst×100,
where Qst and Qam are the areas calculated under the X-ray curves from the semi-crystalline and amorphous samples, respectively.
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6

Qualitative Analysis of Calcium and Magnesium Dietary Supplements

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Our studies were focused on a qualitative analysis of selected dietary supplements containing calcium and magnesium compounds. Samples of dietary supplements were very finely ground in an agate mortar, until a homogeneous fine powder was obtained. The tests were carried out using a PW1050 polycrystalline diffractometer with a PW1729 generator from Philips. Bragg-Brentano focusing of diffractive radiation was applied. The total duration of the analysis of each supplement amounted to 48 h, the angular range of the goniometer: 5°÷135°, CuKα1 radiation (λ = 1.54056 Å), filter—Ni. During the experiment, a full scan in the angle range of 5°–120° was carried out, with an angular step of 0.05°, and the scanning time was 0.1 s. The next measurement was configured so that the angle range matched to the given preparation subjected to the analysis. When the tested sample did not exhibit any peaks above 80°, the second measurement was recorded in the 2θ angle range of 5°÷80° or 10°÷80°. Parameters of the second measurement were as follows: 0.02° angular step and 0.02 s scanning time, affecting the quality of the diffraction pattern distinctly. The measurement was carried out twice or thrice to eliminate all errors.
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7

Structural and Electrochemical Analysis of ZnO Nanorods

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An X-ray diffractometer (Philips PW 1729) with CuKα1 radiation (λ = 1.5406 Å) was used to analyze the crystal structure of ZnO nanorods grown on Ni-foam substrate. Field-emission scanning electron microscopy (FESEM; Zeiss LEO 1550 Gemini) was employed to observe the surface morphology of samples. Elemental analysis was carried out with an energy-dispersive X-ray spectrometer (EDS) attached to the FESEM system. Electrochemical performances of ZnO-NR-based Ni-foam electrodes/substrates were investigated via a three-electrode electrochemical workstation (CHI potentiostat, USA). ZnO-NRs@Ni-foam, platinum plate and Ag/AgCl were used as working electrode, counter electrode, and reference electrode, respectively.
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8

Characterization of Chitosan Nanoparticles

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The physical and cytotoxic characteristics of the obtained CSNP were assessed. The physical characteristics, including the shape and size of the particles, and the powder pattern were considered as reported in our previous studies [11 (link),21 (link)]. A scanning electron microscope (SEM; Phillips-500, Hamburg, Germany) was used for detecting particle morphology. A transmission electron microscopy (TEM; EM900, Zeiss, Oberkochen, Germany) was used for detecting the particles’ shape and average diameter. A Zetasizer (Nano ZS®) of dynamic light scattering was used for estimating the average size and the size distribution of particles. An X-ray diffractometer (PW 1729, Philips, Eindhoven, The Netherlands) was used for the detection of the X-ray diffraction (XRD) pattern of the obtained CSNP powder.
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9

XRPD Analysis of CFA Samples

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The XRPD analysis of all samples including pure CFA was performed using X-ray diffractometer (PW 1729, Philips, the Netherland) with copper (Cu) anode, generator tension 40 kV, generator current 30 mA, and scanning speed 2°/min over the interval of 10–90°/2θ.
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10

Characterization of Solid-Dispersed MOLPs

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SEM-energy dispersive X-ray spectroscopy (SEM-EDS) with an EDS Oxford Instruments® XMax 20 mm2 detector (Carl Zeiss Microscopy, Oberkochen, Germany) was used to analyze the morphology and the elemental composition of the pure MOLP and solid-dispersed MOLPs. Operating conditions of 20 V accelerating voltage and 8.5 mm were applied. The mineral phases were studied using a Philips diffractometer (PW1840), HT generator (PW1729), and chart recorder (PW8203A) (GmbH, Germany).
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