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Chirascan plus spectrometer

Manufactured by Applied Photophysics
Sourced in United Kingdom, United States

The Chirascan Plus spectrometer is a circular dichroism (CD) and UV/Vis spectrometer designed for the characterization of biomolecules and materials. It measures the differential absorption of left and right circularly polarized light, providing information about the secondary structure and conformation of samples. The Chirascan Plus features high sensitivity, rapid data acquisition, and user-friendly software for data analysis.

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63 protocols using chirascan plus spectrometer

1

Circular Dichroism Spectroscopy of SARS-CoV-2 RBD

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An Applied Photophysics Chirascan Plus spectrometer was used to record the CD spectra and thermal denaturation melts for all variants. CD Spectra were obtained for each RBD variant from 190 nm to 260 nm. Protein spectra were recorded with a 0.5 mm cuvette at 5 µM protein concentration in a buffer consisting of 10 mM sodium phosphate, 4 mM NaCl, pH 7.0. Spectra were recorded every 1 nm wavelength and averaged over 2 seconds. Runs were repeated 5 times and averaged.
Thermal denaturation melts were performed using an Applied Photophysics Chirascan Plus spectrometer. All experiments were performed in a 0.5 mm cuvette at a protein concentration of 20 µM in buffer containing 50 mM sodium phosphate, 20 mM NaCl, pH 7.0. Temperature scan rate was 1 °C/min, sample was equilibrated for 30 sec at each temperature increment, and the CD signal at 222 nm was averaged over 2 seconds. Data was plotted and analyzed using the equation.47 (link)
ST=(SN+mNT)+(SU+mUT)e-(ΔHmR1T-1Tm)1+e-(ΔHmR1T-1Tm) where ST is the measured signal as a function of temperature T, SN and SU are the signals corresponding to the native and unfolded baselines, mN and mU are the slopes of linear dependence of SN and SU with temperature, Tm is the midpoint melting temperature, ΔHm is the enthalpy change at the Tm, R is the universal gas constant, and T is the absolute temperature in Kelvin, respectively.
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2

CD Spectra of LHCII Complexes

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CD spectra were detected on a Chirascan-plus spectrometer (Applied Photophysics, UK) in the range of 300–800 nm, at room temperature. The spectra were measured from the LHCII complexes located in a polyacrylamide gel. Gel slices of 1 mm thickness were sandwiched between glass plates.
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3

Thermal (Un)folding of Hip1 Protein

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Thermal un-and refolding was monitored between 15°C and 95°C at 215 nm with a Chirascanplus spectrometer (Applied Photophysics, UK) equipped with a 150-W xenon arc lamp. The heating/cooling rate was 1°C/min. Samples contained about 15 µM Hip1 and were measured using a 1 mm quartz glass cuvette (Hellma, Germany). Traces were normalized by assuming a completely folded state for the first 15 data points and a completely unfolded state for the last 5 data points. The mean of three experiments is shown in bold, individual measurements are displayed on light blue/red.
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4

Far-UV CD Spectroscopy of Protein Samples

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Far-UV CD spectra were measured using a Chirascan plus spectrometer (Applied Photophysics) and a 0.5-mm path-length cuvette at 22°C. Samples were prepared at 15 µM in 5 mM sodium phosphate , 80 mM NaCl pH 8.0. At least three spectra were collected for each sample at 180-260 nm with 1-nm steps and averaged.
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5

Characterization of Oxidized Ag Nanoclusters

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Initial PL measurements of oxidised and un-oxidised Ag NCs were done using an Edinburgh F980 fluorescence spectrophotometer (Edinburgh, UK). Quantum yield (QY) measurements were done using an integrating sphere. MALDI-MS spectra were measured using 3-hydroxypropionic acid (3-HPA) and a combination of anthranilic and nicotinic acids as matrices because they gave clear spectra. CD spectra were measured in an Applied Photophysics Chirascan-plus spectrometer (Surrey, UK).
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6

Determination of IFNA2 Secondary Structure

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To determine IFNA2 secondary structure, CD was used. Far-UV spectra were obtained at room temperature on a Chirascan Plus spectrometer (Applied Photophysics, Surrey, United Kingdom). IFNA2 stock was diluted into water to a concentration of 10 µM and scanned between 190 nm and 250 nm. The mean residue ellipticity (MRE) was calculated using the equation,
MRE=CD in millidegrees/(pathlength in millimeters×the molar concentration of protein×the number of residues)
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7

Spectroscopic Analysis of Molecular Compounds

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Optical rotations were measured on a Rudolph Autopol IV polarimeter. UV spectra were obtained on a UH5300 UV-VIS Double Beam Spectrophotometer. IR spectra were obtained by using a Shimadu Fourier Transform Infrared spectrometer with KBr pellets. NMR spectra were acquired with a Bruker Avance III 600 instrument. ECD spectra were recorded with an Applied Photophysics Chirascan-Plus spectrometer. High resolution electrospray ionization mass spectra (HRESIMS) were recorded on a LC-MS system consisting of a Q Exactive™ Orbitrap mass spectrometer with an ESI ion source used in ultra-high resolution mode (140 000, at m/z 200) and a Dionex UltiMate 3000 RSLC UPLC system. Silica gel (200–300 mesh and 500–800 mesh), RP-18 gel (40–75 μm) and Sephadex LH-20 were used for column chromatography. Preparative HPLC was performed on an Agilent 1260 liquid chromatography system with a Zorbax SB-C18 (5 μm, 9.4 × 150 mm) column and a DAD detector.
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8

Far-UV CD Spectra Measurement

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Far-UV CD spectra were measured using a Chirascan plus spectrometer (Applied Photophysics) and a 0.5-mm path-length cuvette at 22°C. Samples were prepared at 15 µM in 5 mM sodium phosphate, 80 mM NaCl (pH 8.0). At least three spectra were collected for each sample at 180–260 nm with 1-nm steps and averaged.
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9

Far-UV and Near-UV CD Spectroscopy of Proteins

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Far-UV CD spectra
were measured at 25 °C using a Chirascan-plus spectrometer (Applied
Photophysics, UK). Spectra were collected from 195 to 260 nm using
a cylindrical quartz cell with a 1 mm path length. Proteins (0.2 mg/mL)
were dissolved in 10 mM phosphate buffer, 5 mM DTT, and 1 mM EDTA
(pH 7.0). The reported spectra are the average of five scans. Spectra
were analyzed for secondary structure content using the CONTILL curve-fitting
program.23 (link) The near-UV CD spectra were
measured at 25 °C using an identical spectropolarimeter. The
spectra were measured with a 1.0 mg/mL protein solution in 10 mM phosphate
buffer, 5 mM DTT, and 1 mM EDTA (pH 7.0). The reported spectra are
the average of five scans.
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10

Thermal Stability of Acetylated γD-Crystallin

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The structural stability of nonacetylated
and acetylated human
γD-crystallin was also determined using thermally induced unfolding
experiments in a Chirascan-plus spectrometer (Applied Photophysics,
Leatherhead, UK) equipped with a Peltier system. The change in ellipticity
at 218 nm was recorded stepwise between 25 and 90 °C in a quartz
cell with a path length of 2 mm, allowing the samples to equilibrate
at each temperature. The heating rate was set to 0.5 °C/min.
The data were recorded at intervals of 2 °C. A protein concentration
of 0.1 mg/mL in 10 mM phosphate buffer, 5 mM DTT, and 1 mM EDTA (pH
7.0) was used. The values for the fraction unfolded (αU) for both proteins were calculated using the following equation: where θF is the ellipticity
value at 25 °C for completely folded or native protein, θt is the observed ellipticity value at any temperature between
25 and 90 °C, and θU is the ellipticity value
at 90 °C for the completely denatured or unfolded state. The Tm was calculated using sigmoidal analysis as
previously described.24 (link)
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