The largest database of trusted experimental protocols

18 protocols using vacprep 061

1

BET Surface Area Measurement Protocol

Check if the same lab product or an alternative is used in the 5 most similar protocols
The specific surface area of each product was measured by N2 adsorption according to the Brunauer–Emmett–Teller (BET) method. Nitrogen adsorption-desorption isotherms were registered on a TriStar 3000 equipment (Micromeritics, Norcross, GA, USA). Prior to the measurements, the samples were degassed overnight under vacuum at 120 °C on a VacPrep 061 (Micromeritics, Norcross, GA, USA). For each product, the measurement was repeated two times on three independent samples.
+ Open protocol
+ Expand
2

Measuring Unbound Water Content in Samples

Check if the same lab product or an alternative is used in the 5 most similar protocols
The unbound water content of the samples was experimentally determined by estimating the weight loss of the powder sample stored under vacuum (VacPrep 061, Micromeritics, USA) at room temperature (22 ± 2°C) for 48 h.
+ Open protocol
+ Expand
3

Measuring Specific Surface Area of Powders

Check if the same lab product or an alternative is used in the 5 most similar protocols
Nitrogen gas adsorption (TriStar II 3020, Micromeretics, USA) was used to determine the specific surface area of the powders. Before analysis, the samples were treated under vacuum (VacPrep 061, Micromeritics, USA) overnight at room temperature (22 ± 2°C). A 5-point analysis was performed using a nitrogen relative pressure (p/p0) between 0.06–0.20 and the Brunauer – Emmett – Teller (BET) adsorption theory was used to calculate the specific surface area (SSABET).
The bulk roughness (BR) of the different D-mannitol particles was calculated as the ratio between the SSABET and the theoretical specific surface area (SSAsv) calculated based on the particle size volume-distribution assuming spherical particles (Eq.1) (14 (link), 15 ).
SSASV=6Dsv×ρ
The Dsv is the Sauter mean diameter determined by laser diffraction as described above in the relevant section and ρ is the true density of the particles. The true density was calculated as the ratio between the mass of particles and their respective volume. The particle volume was determined by helium pycnometry (AccuPyc II 1340, Micromeritics, USA), using 20 purges at 19.5 psi with an equilibration rate of 0.0050 psi/min.
+ Open protocol
+ Expand
4

Porous Material Characterization Using Nitrogen Adsorption

Check if the same lab product or an alternative is used in the 5 most similar protocols
Pore size, pore volume and BET (Brunauer–Emmett–Teller) specific surface area were determined using nitrogen gas adsorption in a liquid nitrogen bath at 77 K. Measurements were made with a TriStar II Plus, 3030 (Micromeritics, Norcross, GA, USA). Prior to analysis, samples were degassed overnight at 105°C under vacuum using a VacPrep061 (Micromeritics). Pore size distributions were obtained using non‐local density functional theory applied to the adsorption branch of nitrogen sorption isotherms using a Carbon Pore Slit model (ʎ = 0.2). The surface area was determined by applying the BET equation on at least five points in the relative pressure interval 0.05–0.3 [8]. The total pore volume was determined at a relative pressure of 0.97 at the adsorption branch of the isotherm.
+ Open protocol
+ Expand
5

Nitrogen Adsorption-Desorption for BET Analysis

Check if the same lab product or an alternative is used in the 5 most similar protocols
The
Brunauer–Emmett–Teller (BET) surface area and porosity
of the materials were determined at 77 K by the nitrogen (N2) adsorption–desorption method (TriStar II Plus, Micromeritics),
and the samples were degassed at 150 °C for 5 h prior to the
measurements (VacPrep 061 degassing unit).
+ Open protocol
+ Expand
6

Nitrogen Adsorption of Material Sheets

Check if the same lab product or an alternative is used in the 5 most similar protocols
Nitrogen adsorption experiments were performed on a Micromeritics TriStar II Plus at 77 K (Micromeritics Instrument Corporation, Norcross, GA). Samples were dried on a Micromeritics VacPrep 061 sample degas system at 95 °C under flowing N2 gas prior to analysis. Surface area was determined by use of the Brunauer-Emmett-Teller (BET) method and total pore volume was determined by the single point method at relative pressure (P/P0) of 0.97. An individual sheet was determined to have a BET surface area of 51 m2·g−1 and a single point total pore volume of 0.188 cm3·g−1.
+ Open protocol
+ Expand
7

Characterization of ZnO Nanoparticles

Check if the same lab product or an alternative is used in the 5 most similar protocols
Skeleton density (pycnometric density) measurements were carried out using the helium pycnometer (AccuPyc II 1340, FoamPyc V1.06, Micromeritics), the measurements were carried out in accordance with ISO 12154:2014 at the temperature of 25±2°C. The specific surface area of NPs was determined using the surface analyser (Gemini 2360, V 2.01, Micromeritics) by the nitrogen adsorption-desorption method based on the linear form of the BET (Brunauer-Emmett-Teller) isotherm equation, in accordance with ISO 9277:2010. Prior to performing measurements of density and specific surface area, the ZnO samples were subjected to 2h desorption (VacPrep 061, Micromeritics), under vacuum (0.05 mbar) at the temperature of 150°C. Based on the determined specific surface area and skeleton density, the average size of particles defining their diameter was determined using the equation, with the assumption that all particles are spherical and identical.34 (link),37 (link)
+ Open protocol
+ Expand
8

Characterization of MOF Crystalline Phases

Check if the same lab product or an alternative is used in the 5 most similar protocols
The crystalline phases of the MOF-801, MIP-202, and Muc-Zr MOF were characterized by X-ray powder diffraction using a RIGAKU MINIFLEX 600 diffractometer and a BRUKER France SAS AXS D8 ADVANCE diffractometer. Thermo-gravimetric analyses (TGA, TA Instruments SDT Q600 Thermal Gravimetric Analyzer, New Castle, DE, USA) were recorded using a ramp of 10 °C/min. The textural properties of the materials were characterized by nitrogen adsorption at 77 K using a micromeritics VacPrep 061 (sample degas system) and a micromeritics TriStar (Surface Area and Porosity Analyzer (TriStar 3000 gas adsorption analyzer (Micromeritics, Norcross, GA, USA). The equivalent specific surface areas were determined using the BET transform of the sorption isotherm in the relative pressure range between 0.005 and 0.05, taking 0.162 nm2 as the cross-sectional area for adsorbed nitrogen molecules. Scanning electron microscopy (SEM) was performed using a using a Hitachi S4800 microscope (Hitachi, Tokyo, Japan). The ultrasonic bath was an Elma transonic Ti-H-5 brand (Singen, Germany). Fourier transform infrared spectroscopy in transmission mode has been performed using a IFS55 Bruker spectrometer (Bruker, Paris, France) (MCT cryodetector) with a 2 cm−1 resolution in a spectral domain 6000–400 cm−1. The different powdered materials were diluted using dry KBr before being pressed and further analysed.
+ Open protocol
+ Expand
9

Gas Adsorption Analysis of Powders

Check if the same lab product or an alternative is used in the 5 most similar protocols
Before gas adsorption measurements (n = 2) were carried out in a Tristar II 3020 (Micromeritics, Norcross, GA, USA), the samples were dried under vacuum (0.15 mbar) overnight at 30 °C (VacPrep 061, Micromeritics, Norcross, GA, USA). The samples were analyzed at 77.350 K using a nitrogen relative pressure (p/p0) in the 0.01–0.99 range. The specific surface area of the powders was calculated using the Brunauer, Emmmett and Teller (BET) adsorption theory (7-point analysis in the 0.05–0.2 p/p0 range). To determine the macro- and mesopores size distribution, a modification to the Kelvin equation (Equation (1)) was used (Barrett–Joyner–Halenda method) [2 (link)].
log(PP0)=2σVRTrk
where σ and V are the surface tension and molar volume of liquid nitrogen, respectively, R is the universal gas constant, T the absolute temperature and rk the Kelvin radius. The radius of the pores at the different relative pressures follows directly from the sum of the thickness of adsorbed nitrogen layer with the rk.
+ Open protocol
+ Expand
10

Comprehensive Magnesium Stearate Characterization

Check if the same lab product or an alternative is used in the 5 most similar protocols
The PSD of the MgSt brands was measured using laser diffraction in dry dispersion mode at a dispersion pressure of 0.5 bars. The cumulative undersized particle parameters d10 (μm), d50 (μm) and d90 (μm) were calculated. Morphological evaluation of the studied MgSt brands was conducted using scanning electron microscopy (SEM). The SSA of the studied MgSt brands was determined by nitrogen adsorption using the Brunauer-Emmett-Teller (BET) method. Samples of approximately 1 g were dispensed into 3/8” OD sample tubes and prior to analysis, the tubes were outgassed using a VacPrep 061 (Micromeritics, USA) outgassing unit under vacuum at ambient temperature for a minimum of 15 h. Experiments were conducted using a Tristar 3030 instrument (Micromeritics, USA). For each sample tube, specific surface area was calculated from a linear fit of the adsorption isotherm in a relative pressure range of 0.05–0.30 Pa. Three samples tubes were tested for each brand of MgSt and the reported results are the mean values of triplicate determinations [40 ].
+ 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!