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Alpha ra 8

Manufactured by Lauda
Sourced in Germany

The Alpha RA 8 is a laboratory equipment designed for precise and reliable analysis. It functions as a high-performance analytical instrument, providing accurate and consistent measurements. The core purpose of the Alpha RA 8 is to facilitate scientific research and testing across various industries.

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7 protocols using alpha ra 8

1

Electrochemical Characterization of NiMo/Ti Catalysts

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A conventional three-electrode electrochemical cell was used for electrochemical measurements. The fabricated NiMo/Ti and Au(NiMo)/Ti catalysts were employed as working electrodes, a Pt sheet was used as a counter electrode, and a calomel electrode was used as a reference. All potentials in this work were converted to the reversible hydrogen electrode (RHE) scale using the following Equation (5):
Current densities were calculated using the electrodes’ geometric area of 2 cm2. Linear sweep voltammograms were recorded in a 1 M NaOH solution and always deaerated by argon (Ar) for 20 min prior to measurements. HER polarization curves were recorded from the open circuit potential (OCP) to −0.42 V (vs. RHE) at a polarization rate of 10 mV·s−1. Polarization curves were recorded at several temperatures from 25 to 75 °C, and temperatures were set with a water jacket connected to a LAUDA Alpha RA 8 thermostat. Stability was studied by recording chronoamperometry (CA) curves for HER at a potential of −0.22 V (vs. RHE) for half an hour. All electrochemical measurements were performed with a Metrohm Autolab potentiostat (PGSTAT302, Utrecht, The Netherlands) using the Electrochemical Software (Nova 2.1.4).
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2

Ultrasonic Processing of Pomegranate Juice

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An ultrasonic liquid processor (Misonix, Inc., New York, USA) supplied with a 19 mm diameter probe, amplitude levels of 24.4–61 µm, at constant frequency of 20 kHz was used to sonicate the 100 mL pomegranate juices. Ultrasonic treatment was carried out in a 150 mL double wall cylindrical vessel pyrex glass with 60 mm inner diameter, 80mm outer diameter, 65 mm outer height and 55 mm inner height connected to a recirculating refrigerated water bath (Cooling thermostat: Lauda Alpha RA 8, Lauda-Königshofen, Germany) to attain a constant temperature in the juice sample during sonication. Ethylene glycol (2°C according to amplitude levels) with flow rate of 0.5 L/min was used as the refrigerant to remove the heat generated during sonication to maintain sample temperature constant at 25 ± 1 °C. The ultrasound probe was submerged to a depth of 25 mm in the pomegranate juice to constantly sonicate at various wave amplitudes of 50, 75 and 100% and times of 0, 3, 6, 9, 12 and 15 min. For microbial studies, the inoculated pomegranate juices (100 mL) were sonicated in a 150 mL cylindrical vessel under the conditions described at the sub lethal temperature (25°C). The samples were recovered at the exit of the ultrasonic cell, poured into sterile glass tubes; the tubes were immediately immersed into and kept in an ice bath until survivor enumerations.
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3

Carbon Steel Corrosion in CO2 Environment

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Carbon steel L360NB was chosen since this is the commercialized and realistic material for CO2 transport pipeline. The chemical composition of this steel is shown in Table 1. From the as-received pipeline sections, testing coupons were machined to the size of 20 mm × 15 mm × 5 mm. Typical sample preparation included mechanical polishing using 60, 120, and finally, 320 grit silicon carbide abrasive papers, cleaning with ethanol and degreasing with acetone and drying using nitrogen gas prior to every test. The mass and the dimensions of the specimens were measured for weight loss calculation. Experimental condition is summarized in Table 2.
All tests in this study were conducted in a system consisting of three double-walled glass cells connected to a cooling system (Alpha RA8, Lauda, Lauda-Königshofen, Germany) to maintain the temperature at 278 K (5 °C). Each cell has 4 ports to purge the CO2 gas (purity > 99.995%, Linde AG, Germany) (50–60 mL/min) and to insert working, counter, and Ag/AgCl reference electrodes. In the case of exposure test, the coupon was hanged on the Teflon wire, while in the electrochemical test, the coupons were weld to a stick made of high-alloyed material. Before each test, 500 mL condensate was used and purged strongly with Ar (purity > 99.998%, Linde) for 30 min, then 1 h with CO2 to reach the saturation state and stable pH (≈1.9).
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4

Time-resolved Transient Absorption Spectroscopy

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Transient absorption measurements were performed as described in (19 (link)). In detail, time-resolved optical absorption spectroscopy was performed at 277 K with a commercially available laser flash photolysis spectrometer (LP920K, Edinburgh Instruments Ltd., Kirkton Campus, UK), and data were recorded with a digital oscilloscope (TDS-3012C, Tektronix, Beaverton, OR). The protein sample was placed in a synthetic quartz (Suprasil) semimicro cell (108F-QS, Hellma, Muellheim, Germany). The temperature was regulated to 277 ± 1 K by a temperature controller (Alpha RA 8, LAUDA, Lauda-Koenigshofen, Germany). Optical excitation was carried out using an OPO system (OPO PLUS, Continuum, San Jose, CA) pumped with a Nd:YAG laser (Surelite I, Continuum) at a wavelength of 460 nm, a pulse width of 6 ns, and a pulse energy of 4.0 ± 0.2 mJ. The repetition rate of the spectrometer was set to 6.67 mHz. To account for background signals, transients were measured alternately with and without optical excitation and used for calculation of difference absorbance spectra with Beer-Lambert’s law. We recorded two datasets per sample, one on a microsecond time scale to probe the deprotonation of the terminal tryptophan and the other on a millisecond time scale to probe the recombination of the radical pair.
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5

Specific Conductance Measurement Protocol

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Specific conductance data were measured at T = 293.15, 298.15 and 303.15 K with the Pye-Unicam PW 9509 model conductivity meter having the frequency of 2000 Hz using a dip-type cell with a cell constant of 1.15 cm−1 with an uncertainty of 0.01%. The instrument cell was calibrated by using the proposed method [32 (link)] using the aqueous potassium chloride solution. The temperature of the measurement cell was controlled with a Lauda Alpha RA 8 thermostat with ± 0.05 K.
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6

Freezing and Melting Dynamics of Ice

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The measurements were performed in a special chamber (LHU-113, ESPEC, Japan) with controlled temperature and humidity (Fig. S1,ESI †). Temperature in the chamber could be controlled in the range between +50 1C and À20 1C (with AE0.5 1C accuracy), and humidity could be controlled in the range between 30% and 90% RH (with AE2% accuracy). Samples were mounted on a flat copper plate by using thermally conductive double sided copper tape. The temperature of the copper plate was maintained by using a Peltier element with a thermoelectric temperature controller (TC/TPC 150, Data Physics, Germany), and a cooling thermostat (Alpha RA 8, Lauda, Germany). For all the experiments humidity of the chamber was accurately maintained at a constant relative humidity (RH) of 80%, while the temperature was gradually decreased from +15 1C to À15 1C with a cooling rate of 2 1C min À1 . After cooling to À15 1C, the temperature was kept constant for 20 min. Finally, the samples were heated to +15 1C. We recorded the whole process of the freezing and melting of ice with the help of a digital camera (DMC-TZ31, Panasonic). All the samples (fabricated on 2 cm  1 cm silicon wafers) were mounted vertically at a 901 tilt angle on the cooling plate.
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7

Fluorescent Compound Analysis via HPLC

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EEFMs were measured on a PerkinElmer LS 55 luminescence spectrometer equipped with a xenon discharge lamp (equivalent to 20 kW for 8 ms duration) and connected to a PC microcomputer, using 1.00 cm quartz cells. Instrumental parameters were: excitation and emission slits 5 nm, photomultiplier voltage 850 V, scan rate 1500 nm min À 1 . The temperature of the cell holder was regulated using a Lauda (Frankfurt, Germany) Alpha RA8 thermostatic bath.
HPLC was carried out on an Agilent 1200 liquid chromatograph (Agilent Technologies, Waldbronn, Germany) equipped with a quaternary pump operating at 0.7 mL min À 1 and a fluorescence detector irradiating at 225 nm and measuring at 306 nm.
A Rheodyne injector with a 20.0 μL loop was employed to spread the sample onto a Poroshell 120 EC C18 column (2.7 μm average particle size, 100 mm  4.6 mm i.d.).
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