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Ag agcl electrode

Manufactured by Thermo Fisher Scientific
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The Ag/AgCl electrode is a reference electrode used in electrochemical measurements. It consists of a silver (Ag) wire coated with silver chloride (AgCl), immersed in a solution containing chloride ions. This electrode provides a stable and reproducible reference potential, which is a crucial component in various electrochemical techniques, such as potentiometry, voltammetry, and electrochemical sensors.

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2 protocols using ag agcl electrode

1

Thermal Equilibrium Measurements and Hyperpolarized Dissolutions

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14.1T thermal equilibrium measurements and hyperpolarized dissolutions were performed with a D2O- or H2O-based buffer. Each buffer consisted of 100mM Tris base and 1mM ethylenediaminetetraacetic acid (Fisher Scientific, USA). H2O-based buffers were adjusted to pH 7.4 with conc. HCl and 10N NaOH (Fisher Scientific, USA) and D2O-based buffers were adjusted to pD 7.4 with conc. DCl and 10N NaOD (Sigma-Aldrich, USA). pH and pD of H2O- and D2O-based buffers were measured with a Ag/AgCl electrode (Fisher Scientific, USA). Since the ionization constants of H2O and D2O (13.99 and 14.96)23 and reduction potentials of H+ and D+ (0V and −0.044V)24 are similar, we assumed that an Ag/AgCl pH electrode could be used to roughly approximate pD.
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2

Microfluidic Liquid Crystal Zeta Potential Sensor

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The three-electrode scheme was employed as shown in Figure 1. The ITO substrate (Qunguan Electronic Technology Co., Ltd., Dongguan, China) was used as the working electrode. The counter electrode was a commercially available platinum foil (Fisher Scientific, Waltham, MA, USA). The reference electrode was an Ag/AgCl electrode (Fisher Scientific, Waltham, MA, USA).
The measurement setup of the microchip is illustrated in Figure 1. In the measurement, a (Fiber-Lite MI-150R, Dolan-Jenner Industries, Boxborough, MA, USA) light source was used to generate the incident light. The polarizer and the analyzer films (Renianus, Guangzhou, China) were used to only allow light with specific polarization to pass. Liquid crystal (Liquid crystal mixture E7 from BOC Sciences, Shirley, New York, NY, USA) filled the wells to sense the change in zeta potentials. The setup was placed under an inverted Olympus I-70 microscope (Olympus Life Science, Tokyo, Japan). In all measurements, we utilized a 20× magnification objective lens with a numerical aperture of 0.4. The transmitted light was detected by a CCD camera (MF603C-CCD from AmScope, Irvine, CA, USA). The captured images were subsequently processed using a MATLAB program to generate a peak-to-peak light-intensity map, which was then converted into a surface potential distribution.
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