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3531 z hi tester

Manufactured by HIOKI
Sourced in Japan

The 3531 Z Hi-tester is a precision instrument designed for high-voltage measurement and testing. It features a wide measurement range and high accuracy to ensure reliable results. The device is capable of measuring voltages up to 5 kV and is suitable for a variety of laboratory and electrical applications.

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7 protocols using 3531 z hi tester

1

Electrical Impedance Spectroscopy for Energy Storage

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Electrical impedance spectroscopy (EIS) is an appropriate technique for learning a material’s electrical property, and has been used in electrochemical energy storage devices [46 (link)]. It gives vital evidence about the electrical properties at the interfacial space among electronically conducting electrodes and electrolytes. Before impedance measurements, the electrolyte films were cut into small discs of 2 cm in diameter and then positioned between two stainless steel electrodes via spring pressure. The impedance measurements were performed via HIOKI 3531 Z Hi-tester (Hioki, Nagano, Japan) with a computer in the frequency range between 50 Hz and 5000 kHz at room temperature. Software extracted both real (Z′) and imaginary (Z″) parts of the impedance spectra of the EIS plots. From the plot’s intersection with the real axis, the bulk resistance (Rb) was obtained. From the Rb, the conductivity of the films was measured using Equation (2) [46 (link)]: σdc=(1Rb)×(tA)
where t is the thickness of the film and A is the area of the electrode.
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2

Structural and Electrical Characterization of Thin Films

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X-Ray Diffraction (XRD) patterns were acquired using an Empyrean X-ray diffractometer, (PANalytical, Netherland) with operating current and voltage of 40 mA and 40 kV, respectively. The samples were irradiated with a beam of monochromatic CuKα X-radiation of wavelength λ = 1.5406 Å and the glancing angle of the X-ray diffraction was in the range of 5° ⩽ 2θ ⩽ 80° withastepsizeof0.1°.
The acquisition of impedance spectra of the films was conducted using a HIOKI 3531 Z Hi-tester in the frequency range of 50 Hz to 1000 kHz and at various temperatures ranging from 303 K to 373 K. The prepared SPE films were cut into small discs of 2 cm in diameter and placed between two stainless steel electrodes under spring pressure. The cell was connected to a computer equipped with customized software to record both real (Z′) and imaginary (Z′′) parts of the complex impedance (Z*) spectra. Consequently, from these data, complex permittivity (ε*) and complex electric modulus (M*) can be then estimated.
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3

Structural Analysis of SPE Samples

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To examine the structural changes of the prepared samples, the XRD has been employed. The Siemens D-5000 X-ray diffractometer (Bruker AXS GmbH, Berlin, Germany) was used with an operating voltage of 40 kV and a current of 40 mA. The blended SPE samples were studied through the monochromic XRD of wavelength (λ = 1.5406 Å) with a 2θ glancing angle ranging from 10° to 80° with a step size of 0.1°. The measurements of electrical impedance spectroscopy of the fabricated samples were done using an impedance analyzer of LCR meter (HIOKI 3531 Z Hi-tester, Nagano, Japan). The operating frequencies were in the range of (50 Hz ≤ f ≤ 1 MHz) at the room temperature. Two stainless-steel electrodes were used as a working electrode to investigate the electrolytes after the films were cut into appropriate size.
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4

Electrical Characterization of Solid Polymer Electrolytes

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Complex impedance spectroscopy as a powerful technique is not only for determining the electrical properties of materials but also for investigating the interfacial region between the electronically conducting electrodes and the electrolytes. As described in the experimental section, the separating phase was obtained from the solid polymer electrolyte (SPE) films by cutting them into small discs (2 cm diameter) and sandwiching them between two stainless steel electrodes using spring pressure. The impedance of the films was measured using a HIOKI 3531 Z Hi-tester (HIOKI, Nagano, Japan), which was controlled by a computer in the frequency range from 50 Hz to 5000 kHz. Software was used to measure the real (Zr) and imaginary (Zi) parts of impedance. To present the impedance spectra of Zr and Zi, a Nyquist plot was used, and an analysis of the spectra was performed from the determination of the intercept of the plot with the real impedance axis to gain the bulk resistance. All conductivity values were also calculated using the equation shown below [24 (link),25 (link)].
σdc=(1Rb)×(tA)
where t and A are the thickness and surface area of the film, respectively.
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5

Characterization of Chitosan-Silver Nanocomposites

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The XRD was recorded at room temperature using X-ray diffractometer (Bruker AXS, Billerica, MA, USA) with operating voltage and current of 40 kV and 40 mA, respectively. A beam of monochromatic, X-radiation of wavelength λ = 1.5406 A° was used to scan the samples with the glancing angles in the range of 5° ≤ 2θ ≤ 80° and step size of 0.1°. A Jasco V-570 UV–vis-NIR spectrophotometer (Jasco SLM-468, Tokyo, Japan) in the absorbance mode was used to record the UV–vis spectra of the chitosan-silver nitrate membrane film and their nanocomposites. The electrical properties of the samples were carried out using HIOKI 3531 Z Hi-tester (Nagano, Japan). For electrical impedance spectroscopy (EIS) measurements, the films were cut into small discs with 2 cm in diameter and sandwiched between two stainless steel electrodes. The impedance of the films was measured within the frequency range of 0.05–1000 kHz.
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6

Structural and Electrical Analysis of Electrolyte Membranes

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The XRD was performed on the samples using an X-ray diffractometer (Bruker AXS, Billerica, MA, USA) with an operating voltage and current of 40 kV and 40 mA, respectively. The samples were scanned with a beam of monochromatic, X-radiation of wavelength λ = 1.5406 A° and the glancing angles were in the range of 5° ≤ 2θ ≤ 80° with a step size of 0.1°. The electrical behavior of the electrolyte membranes were examined using a HIOKI 3531 Z Hi-tester within the frequency range of 50–1000 kHz.
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7

Characterization of Nanocomposite Polymer Films

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The ultraviolet-visible (UV-Vis) absorption spectra of the prepared films were recorded on a UV-vis spectrometer (V-570, Jasco, Japan) with the scanning range from 180 to 1000 nm. To investigate the surface microstructure of the nanocomposite films, optical micrograph (OM) images were taken. The images at adjusted magnification were taken by an optical microscope (MEIJI) through an attached camera-controlled (DINO-LITE) software. Furthermore, the surface morphology of the samples was examined by scanning electron micrograph (SEM) using the FEI Quanta 200 FESEM scanning electron microscope. X-Ray Diffraction XRD patterns were recorded using Empyrean X-ray diffractometer, (PANalytical, Netherland) with operating current and voltage of 40 mA and 40 kV, respectively. The samples were scanned with a beam of monochromatic CuKα X-radiation of wavelength (λ = 1.5406 Ǻ), and the glancing angles X-ray diffraction was in the range of 5° ≤ 2θ ≤ 80° with a step size of 0.1°.
The impedance of the films was measured using HIOKI 3531 Z Hi-tester within a frequency range of 50 Hz to 1000 kHz. The SPE blend films were cut into small discs (2 cm diameter) and sandwiched between two stainless steel electrodes under spring pressure. The measurements were also carried out at different temperatures ranging from 303 K to 363 K.
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