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Frontier fourier transform infrared ftir spectrometer

Manufactured by PerkinElmer
Sourced in United States

The Frontier Fourier transform infrared (FTIR) spectrometer is a laboratory instrument that measures the absorption or transmission of infrared light by a sample. It collects data in the form of an interferogram and converts it into a single-beam infrared spectrum using Fourier transform analysis. The Frontier FTIR spectrometer is designed to provide accurate and reproducible infrared spectral data for a variety of applications.

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5 protocols using frontier fourier transform infrared ftir spectrometer

1

Infrared Characterization of Composite Materials

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The infrared properties of the composite materials were characterized according to standard protocols.25,26,42 (link) The total infrared reflectance and transmittance spectra were obtained by using a Frontier Fourier transform infrared (FTIR) spectrometer (PerkinElmer) outfitted with a mid-infrared integrating sphere (Pike Technologies) and were analyzed with the Spectrum (PerkinElmer) and Origin 8.5 (OriginLab) software packages. The measurements were referenced to a National Institute of Standards and Technology (NIST)-verified Pike Technologies Diffuse Gold Standard. The composite materials were mounted on home-built size-adjustable stages, which allowed for the application of strains between 0% and 100%. The total reflectance spectra were collected at an illumination angle of 12°, and the total transmittance spectra were collected at a normal illumination angle. The spectra were collected in an indoor environment at room temperature, i.e., typically ∼20 °C. The average reflectance and transmittance value changes were calculated for the composites over the wavelength range of 4.5–16.5 μm by subtracting the average values at strains of 0% from the average values at strains of >0%. The experiments were performed on at least eight different composite materials of each type, with similar results obtained in each instance.
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2

Characterization of Chemical Compounds

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An Electrothermal 9100 apparatus (Electrothermal Engineering Ltd., Southend-on-Sea, UK) was used for melting point acquisition. IR spectra were measured on a Frontier Fourier transform infrared (FT-IR) spectrometer (PerkinElmer, Waltham, MA, USA) with an ATR accessory. NMR spectra were recorded on an Avance DPX 400 spectrometer (Bruker, Billerica, MA, USA) running at 400.13 MHz for 1H and 100.61 MHz for 13C. EI-MS were obtained on a MAT 95 spectrometer (70 eV, Finnigan, San Jose, CA, USA). Thin layer chromatography (TLC) was realized on precoated silica gel glass plates (5 × 10 cm, Merck silica gel 60 F254, Darmstadt, Germany). Column chromatography was carried out on silica gel (60–200 mesh) purchased from J. T. Baker (Phillipsburg, NJ, USA). Size-exclusion chromatography was performed on Sephadex LH-20 (Lipophilic Sephadex, Amersham Biosciences Ltd., purchased from Sigma-Aldrich Chemie, Steinheim, Germany).
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3

ATR-FTIR Spectroscopic Analysis of Samples

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ATR-IR spectra were acquired using a Frontier Fourier transform infrared (FTIR) spectrometer (Perkin Elmer, Villebon-sur-Yvette, France) equipped with a Quest single reflection diamond attenuated total reflectance (ATR) accessory (Specac, Orpington, UK). The spectral range was set between 4000 and 400 cm−1 with spectral resolution of 4 cm−1. A drop ≈100 µL was deposited directly onto the diamond surface and spectroscopic measurements were performed immediately. Prior to sample measurement, a background spectrum was recorded in the air (4 averaged scans) and the sample spectrum (4 averaged scans) was automatically ratioed with it via software (Spectrum, Perkin Elmer), effectively normalising it to a maximum reflectance of 1 (100%). The data were further processed by software to express the spectrum in terms of sample absorbance. For each sample, 3 deposits have been measured and 3 spectra per drop have been collected. Ultimately, 9 spectra were recorded from each sample, capturing inter- and intra-variability during measurements. Spectra from pure compounds have also been collected using similar parameters. The entire operation to analyse 1 drop, including cleaning the ATR crystal, collection of the background, and collecting the IR spectrum from the sample, takes less than 30 s.
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4

Reflectance Micro-FTIR Analysis of Direct Placement and CAD/CAM RBC Samples

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The particles from all direct placement and CAD/CAM RBC sampleswere washed with ultra-high quality (UHQ) water, and left to dry at room temperature for 8 h, prior to deposition on a stainless-steel flat sample holder for infrared micro-analysis. Reflectance micro-FTIR spectra were taken on a Perkin Elmer Spotlight 400 FT-IR Imaging System (Perkin Elmer, Waltham, MA, USA). Micro Fourier Transform Infrared (FTIR) spectra were collected over the 4000 cm−1 to 700 cm−1 wavenumber range, in reflectance mode, using a liquid nitrogen cooled Mercury–Cadmium–Telluride (MCT) array detector, at a resolution of 8 cm−1 and an aperture of 20 μm. Sixteen scans were taken for each pixel in the infrared maps, where each pixel corresponded to a square of 20 µm per side. A Kramer–Kronig transformation was not needed, as the resulting spectra did not present specular reflectance distortions.
Samples were also analysed on a Perkin Elmer Frontier Fourier Transform Infrared (FTIR) spectrometer (Perkin Elmer, Waltham, MA, USA), using a Perkin Elmer Attenuated Total Reflectance (ATR) accessory, consisting of a diamond crystal at a fixed angle of 45°. One-hundred spectra were collected over the 4000 cm−1 to 650 cm−1 wavenumber range, at a resolution of 4 cm−1.
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5

FTIR Analysis of Protein Structure

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Soon after performing each treatment, all the samples including controls were analyzed by a PerkinElmer Frontier Fourier Transform Infrared (FTIR) spectrometer (PerkinElmer, Waltham, MA) with a combined software of IR Solution (version 1.40, Shimadzu Corporation, Kyoto, Japan), as previously described (Bogahawaththa et al., 2017b) . The samples spectra (range 4,000-600 cm -1 ) were obtained in the absorbance mode by subtracting the background. With the aid of the software, the second derivative of every spectrum was obtained to enhance the resolution. The peaks, which corresponded to the protein secondary structure, were studied within broad amide I region (1,600-1700 cm -1 ).
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