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Quartz cuvette

Manufactured by Starna Cells
Sourced in United States, Canada, United Kingdom

A quartz cuvette is a transparent container made of high-purity quartz glass that is used in spectroscopy and other laboratory applications to hold liquid samples. The primary function of a quartz cuvette is to provide a stable and optically transparent vessel for measuring the absorption or transmission of light through a sample.

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54 protocols using quartz cuvette

1

Protein Structure Analysis via CD Spectroscopy

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The structure of each protein in solution (0.01 mg/ml) was determined in a quartz cuvette (Starna Cells) of 1.0 cm path length using a standardized methodology for CD spectropolarimeter (Jasco J-810) over a range of temperatures to induce various degrees of protein unfolding.[25 (link)] Briefly, each CD spectrum, consisting of the ellipticity and absorbance values, was obtained over a wavelength range from 190 to 300 nm, at a scan rate of 50 nm/min and a response time of 0.25 sec. Each spectrum represented an accumulation of 6 scans. Temperature control within the CD instrument was done using the Peltier temperature control device that is integrated within our instrument. Thermal-induced denaturation of the proteins was done using an external water bath (Neslab, RTE-111) over a temperature range from 5 to 85 °C. In addition to the plain protein solutions, solutions of proteins with urea at different concentrations in a quartz cuvette (Starna Cells) of 0.01 cm path length were analyzed to provide samples exhibiting strong background absorbance over the range of 190-220 nm that could not be analyzed by conventional full-spectrum-based methods.
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2

Tryptophan Fluorescence and Hydrophobic Surface Analysis of apoLp-III

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Tryptophan fluorescence of apoLp-III was measured in a LS 55 fluorescence spectrometer (PerkinElmer, Waltham, MA). Protein samples of 30 μg/mL in phosphate buffered saline (PBS; 37 mM NaCl, 2.7 mM KCl, 10 mM Na2HPO4, 1.8 mM KH2PO4, pH 7.4) were transferred to a quartz cuvette (Starna Cells, Atascadero, CA), and samples were excited at 280 nm with a slit width of 3 nm. Emission was monitored from 290 to 450 nm at a scan rate of 50 nm/min using five accumulation cycles. The exposed hydrophobic surface was measured with 8-anilinonaphthalene-1-sulfonic acid (ANS)(Sigma-Aldrich, St. Louis, MO). Protein samples (5 μM final concentration) were mixed with ANS (230 μM final concentration) in 1 mL total volume in a quartz cuvette (Starna Cells, Atascadero, CA). Samples were excited at 395 nm, with a slit width of 6 nm, and emission was monitored from 400 to 650 nm, using 3 accumulation cycles at a scan rate of 50 nm/min.
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3

Thermal Stability Analysis of PIR1-C152S-coreFED

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Thermal stability
measurements were
recorded using a Jasco J-810 spectropolarimeter equipped with a Neslab
RTE7 refrigerated recirculator, as previously described.18 (link),19 (link) PIR1-C152S-coreFED dissolved at a final concentration
of 17.0 μM in 20 mM sodium phosphate (pH 7.4) and 50 mM NaCl
was measured using a 1 mm long × 12.5 mm wide quartz cuvette
(Starna Cells, Inc.), which holds 0.4 mL. Variations in ellipticity
at 222 nm as a function of temperature were measured in 0.2 °C
increments between 25 and 90 °C. Slow cooling to 25 °C followed
by a CD scan at 222 nm to assess the presence of secondary structures
demonstrated that PIR1-C152S-coreFED unfolds irreversibly.
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4

CD Spectroscopy of TNIP1 Protein

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CD spectra were collected on a Chirascan V100 spectropolarimeter (Applied photophysics, Surrey, UK) scanning from 190–250 nm with a 1 nm step and 2 nm bandwidth. 400 µL of TNIP1417-509 protein at a final 10 µM (0.13 mg/mL) concentration in 50 mM sodium phosphate buffer (pH 8.0) scanned using a quartz cuvette with a 1 mm pathlength (Starna Cells, Atascadero, CA, USA). All spectra were blanked against spectra collected from buffer-only samples. Scans done at increasing temperatures were performed using a Precision Peltier (Quantum Northwest, Liberty Lake, WA, USA) temperature controller. Secondary structure characterization studies were performed using protein samples under the same conditions as above with the addition of 10, 20, 30 or 40% (v/v) 2,2,2-trifluoroethanol (TFE) for 1 h prior to scanning. Post CD analysis done using the DichroWeb server using the Contin-LL (Provencher and Glockner Method) using database 7 from [55 (link)] and references therein. Standards for comparison of AHD1-UBAN versus random coil and pre-molten globule proteins were taken from [45 (link)].
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5

CD Spectroscopy of Protein Folding

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CD spectroscopy is generally used to study chirality of molecules, especially, protein folding and interaction in aqueous media due to the facile manipulation of the experimental conditions and its high sensitivity towards minute variations in temperature, pH and amphiphiles. The protein’s native CD spectra and the changes upon drug titration were obtained using a Jasco 715 spectro-polarimeter (Mary’s Court Easton, MD, USA) and using a quartz cuvette (Starna Cells, Atascadero, CA) with 2 mm path length. All spectra were acquired from 200 to 260 nm and are indicate as the average of three accumulations with the scanning resolution of 0.5 nm. A 50 μL of PDK2 protein (50 μg at 1.5 mg/mL) was transferred to the cuvette with 500 μL of PBS (1×) and 1 μL of monochloroacetic acid (25 mM in DI water) was titrated to the cuvette at each addition. The drug was mixed properly and was incubated three minutes before data acquisition. The titration was terminated when no noticeable change was observed in the spectra pattern. The measured curves were smoothed using Savitzky- Golay algorithm by taking 10 points fitting a second order polynomial curve.
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6

Circular Dichroism Spectroscopy Analysis

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Circular dichroism (CD) spectra were collected using a Chirascan spectropolarimeter (Applied Photophysics). The samples were analyzed at a concentration of 0.2 mg/mL in 10 mM sodium phosphate, pH 7.9 and were added to a quartz cuvette with a 0.1-cm path length (Starna Cells). Spectra were collected at 10 °C and analyzed using several wavelength ranges, beginning at 190, 195, 200, 205 and 210 nm through 260 nm. Background signal from the solution was subtracted. CDNN software (Applied Photophysics) was used for spectral deconvolution.
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7

Time-Resolved Fluorescence Spectroscopy

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TCSPC
measurements were undertaken using a FluoTime 250 TCSPC spectrometer
(PicoQuant, Berlin, Germany). A pulsed picosecond laser excitation
source of 660 nm was used, and a detection wavelength of 700 nm was
chosen. The repetition rate of the excitation laser was optimized
for each sample, ranging from 26 to 60 MHz. With this excitation source,
the instrument response function (IRF) of the spectrometer has a full-width
at half-maximum of ∼80 ps. The solutions were contained in
a 1 cm path length quartz cuvette (Starna Cells, Atascadero, CA) and
had an optical density below ∼0.1 at 660 nm.
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8

Circular Dichroism Analysis of Protein Samples

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All protein samples were dialysed in 1X Phosphate-buffered saline (PBS) buffer overnight before Circular Dichroism (CD) spectroscopy analysis. Typically, protein samples at 0.01 mg/ml in a quartz cuvette (Starna Cells) of 1.0 cm path length was placed into AVIV 410 spectrometer for CD spectrum acquisition at room temperature (25 °C). Each CD spectrum consisting of the absorbance values was acquired over a wavelength range of 195–260 nm. Each protein sample was measured in three independent scans and the final spectrum is the average of the three scans. To remove absorption background (buffer), three independent scans were made on the 1X PBS buffer. To remove signals from the fused Maltose binding protein (MBP), spectra of independently purified MBP in the same buffer were also acquired that were then subtracted from those of the MBP-Bfr2 fragments. All CD data were expressed as mean residue molar ellipticity in deg × cm2/dmol. The secondary structure content of the proteins was estimated by the deconvolution of far-UV CD spectra according to BeStSel31 (link). PDB2CD32 (link) was used to convert cryoEM models to CD spectrum data.
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9

Circular Dichroism Analysis of Polypeptides

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CD spectra were measured in a quartz cuvette with an optical path length of 0.5 mm (Starna Cells) using a J-815 spectropolarimeter (Jasco, Japan) at room temperature. The far- and near-UV CD spectra were used to identify changes in protein secondary and tertiary structures. The spectral regions were 200–300 nm. The final spectra were obtained as an average of five accumulations. The spectra were corrected for the baseline by subtracting the spectra of the corresponding polypeptide-free solution. Analogs or IGF-II was dissolved and measured in 5% aqueous acetic acid (0.33 mg/ml; 45 μm).
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10

Fluorimetry assay of Rags-Ragulator-SLC38A9 complex

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Fluorimetry experiments were performed in quadruplicates using a FluoroMax-4 instrument (Horiba) and a quartz cuvette compatible with magnetic stirring (Starna Cells) and a 10 mm pathlength. The Trp fluorescence signal was collected using 297 nm excitation (1.5 nm slit) and 340 nm emission (20 nm slit). Experiments were performed in wash buffer at RT with stirring. The final concentration of Rags was 350 nM. 500 μl of wash buffer were added to the cuvette and after baseline equilibration, 20 μl of a protein mixture containing Rags, 1.2x molar excess of Ragulator and with or without 1.2x molar excess of SLC38A9NT were added. After signal equilibration, the assay was started by addition of 20 μl FLCN:FNIP2 to a final concentration 35 nM and the fluorescence signal was recorded in 1 s intervals for 1,800 s. The signal prior to FLCN:FNIP2 addition was used for baseline subtraction and subsequently normalized to the signal right after FLCN:FNIP2 addition. This served also as the t=0 time point. Plotted are the mean and standard deviation of each time point.
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