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Nicolet 460

Manufactured by Thermo Fisher Scientific
Sourced in United States, Germany

The Nicolet-460 is a Fourier Transform Infrared (FTIR) spectrometer designed for laboratory use. It is capable of analyzing the infrared absorption or transmission spectra of solid, liquid, and gas samples. The Nicolet-460 provides accurate and reproducible infrared data for a variety of applications.

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6 protocols using nicolet 460

1

Characterization of Biochar Surface Properties

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The surface morphology of BCs was observed by SEM (Zeiss
Supra 40, Germany). Automatic specific surface area and pore size
analyzer (GEMINT VII 2390) was used to determine the Brunauer–Emmett–Teller
(BET) surface area and pore structure of BCs. The crystal phase structure
was presented by an XRD diffractometer (Bruker D8 Advance, Germany).
The surface functional groups were analyzed and quantified by FTIR
(Nicolet-460, Thermo Fisher) and Boehm titration (Supporting Information).27 (link) The
elemental contents of C, N, O, and H in BCs were determined by elemental
analysis (Flash 2000, Thermo Fisher).51 Point of zero charge (PZC) is used to determine the surface charge
of BCs.28 (link) XPS analysis (Nicolet 460, Thermo
Fisher) was conducted to determine the binding energy between electrons
and characterize the elements on the surface of BCs.
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2

Characterization of Flexible Pressure Sensor

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The morphology and structure of the PMR nanocomposite thin films were characterized using scanning electron microscopy (SEM, MAGELLAN-400, USA). The crystal phase structures of the PMR nanocomposite thin films were characterized by X-ray diffraction (XRD, Haoyuan DX-2700BH, China). The response performance of the flexible sensor was measured with a digital source meter (Keithley 6510 Source Meter SMU Instrument, Beaverton, OR, USA). The thickness of the PMR nanocomposite thin film was measured by means of the step meter (DektakXT, Boyue Instruments Co. Ltd., Shanghai, China). The Fourier transform infrared spectrum (FTIR, Thermo Scientific Nicolet 460, Woodland, CA, USA) was performed to analyze the FTIR spectra of the thin films.
The change rate of the sensor increased with the increase in the applied external pressure, which can clearly distinguish different pressures. The change rate of resistance can be expressed as follows: Y=ΔRR=RRpR
where Y is the change rate of resistance; Rp is the resistance of the flexible sensor under the action of pressure; and R is the resistance of the sensor under no pressure.
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3

Fourier Transform Infrared Spectroscopy of Materials

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The chemical structures of the different materials were characterized by Fourier transform infrared spectroscopy (Nicolet-460 Thermo Fisher) at a wavenumber scan range of 600–4000 cm−1.
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4

Characterization of Complex Coacervate Nanostructures

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FTIR experiments were performed using an FTIR spectrophotometer (Nicolet-460, Thermo Fisher Scientific, Waltham, MA, USA). The complexes obtained after freeze-drying were milled and pressed with potassium bromide and polymer in a ratio of 200:1. Transmittance values between 4000 cm−1 and 400 cm−1 were measured to determine the functional relationship between the different compounds.
XRD analyses of the samples were performed using a smart X-ray diffractometer (SmartLab 3KW, Rigaku Corporation, Tokyo, Japan), according to Dong et al. [20 (link)], with slight modifications. The prepared powder was flattened on a glass plate for X-ray diffraction analysis, and the scanning range was 2θ from 5o to 50°, with a step size of 5 °/min/scan rate.
Scanning electron microscopy (SEM) of the samples was conducted using a SU1510 SEM (Hitachi, Tokyo, Japan). The freeze-dried powder was adhered to a double-sided adhesive tape, coated with gold, and observed using a scanning electron microscope at a magnification of 500×.
An FEI Tecnai 12 (FEI Company, Hillsboro, NH, USA) was used for transmission electron microscopy (TEM). A drop of the complex coacervate solution was placed on a 400-mesh copper grid. The grids were then dried overnight at 40 °C, and the morphology of the samples was observed using an electron microscope with a single-tilt sample rack at an accelerating voltage of 100 kV.
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5

Characterization of ArPPK2-Cu3(PO4)2·3H2O Nanoflowers

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The sample
morphology and microstructure of the ArPPK2-Cu3(PO4)2·3H2O nanoflower were
analyzed by SEM (S4800, Hitachi High Technologies Corporation). The
material crystal phase was characterized by powder XRD (Bruker D8,
Cu Kα radiation) among the range of 5–90° at the
rate of 0.02/s. FT-IR (Nicolet-460, Thermo Fisher Scientific) was
performed in the range of 400–4000 cm–1 on
a KBr pellet.33 (link) The surface properties
and composition were conducted by XPS (ESCALAB 250xi, Thermo Fisher
Scientific).
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6

Characterization of Polyionic Liquid Hydrogels

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1H NMR were recorded with a 500 MHz Bruker Avance instrument and FTIR were recorded with Nicolet-460 (Thermo Fisher, Waltham, MA, USA). The diameters and zeta potentials of PILs were determined by DLS at 25 °C and electrophoretic light scattering (ELS) using a zeta Sizer Nano ZS (Malvern Instruments, Westborough, MA, USA).
The gelation time and the rheological properties of the hydrogels were evaluated at a constant frequency f = 1 Hz (25 °C) by a Malvern Kinexus pro rheometer. Following hydrogel formation, the frequency sweep experiment was performed at γ = 0.5%, and f = 0.1–100 Hz, and the amplitude sweep experiment was performed f = 1 Hz and γ = 0.1–100%.
The surface morphology of the freeze-dried hydrogels was observed using FE-SEM (Zeiss Sigma 500, Oberkochen, Germany). All samples were coated with gold before characterization.
Compressive stress–strain measurements of the freeze-dried hydrogels (d = 2 mm, h = 5 mm) were obtained using compression test machine (Bose ELF3200, Framingham, MA, USA). The load cell was 10 N, and the compression velocity was 1 mm/min. The stress and strain values were taken at the rupture point when the freeze-dried hydrogels brake.
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