D8 advance davinci
The D8 Advance Davinci is a X-ray diffractometer designed for advanced materials analysis. It provides high-resolution X-ray diffraction measurements for a wide range of applications.
Lab products found in correlation
10 protocols using d8 advance davinci
Comprehensive Characterization of Catalytic Materials
Synthesis and Characterization of MgFe-LDH
Comprehensive Nanoparticle Characterization
Quantify Cement Crystalline Components
Crystalline State Determination of PKPI
Characterization of Synthesized Catalysts via Advanced Microscopy and Spectroscopy
Characterization of BC, PBC-2, and nZVI@PBC-20
Determining Point of Zero Charge of AB
solid addition method was used to determine the point of zero charge
(pHPZC) of AB.52 (link) Several 0.1
mol/L KNO3 solutions were adjusted at pH values between
2 and 8 by adding 0.1 HNO3 or NaOH. Each solution with
0.1 g of AB was placed in a sealed flask under constant stirring (150
rpm). After 48 h, the final pH was measured. The plot of ΔpH
(pHf – pH0) against the initial pH (pH0) was made to obtain pHPZC.
AB characterization
was carried out before and after the adsorption experiments by SEM,
XRD, and solid-state 13C CP/MAS NMR. The morphology of
the biosorbent was evaluated by using a scanning electron microscope,
JEOL JSM-6400 (US). EDS microanalysis was conducted to identify the
elements in AB. The samples were weighed (0.2 g) and characterized
with an X-ray diffractometer, Bruker D8 Advance Da Vinci (USA), using
Cu Kα radiation at a step size of 0.03°. Nuclear magnetic
resonance analysis was performed using CP/MAS for 13C nuclei
in a 500 MHz spectrometer (Bruker, USA).
Magnesium Deposition on Copper Substrate
Comprehensive Characterization of Synthesized Powders
and the morphology of the synthesized powders were investigated by
energy-dispersive X-ray spectroscopy (EDX) and scanning electron microscopy
(SEM), using a Zeiss EVO 40 microscope. Gas porosity and specific
surface area of the powders were explored using a Micromeritics TriStar
II Plus automated gas sorptometer. X-ray powder diffraction (XRPD)
data were collected at room temperature on a Bruker D8 Advance Da
Vinci diffractometer. X-ray photoelectron spectroscopy (XPS) analyses
were performed using a Kratos AXIS Ultra DLD. XPS quantification was
performed using the instrument sensitivity factors and high-resolution
scans.
All specifications about instruments, equipment, data
collection, and evaluation are reported in the
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