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Dynapro dls

Manufactured by Wyatt Technology
Sourced in United States

The DynaPro DLS is a dynamic light scattering (DLS) instrument designed for the analysis of particle size and molecular weight distribution in a variety of samples. The DynaPro DLS measures the diffusion of particles or molecules in a liquid medium, allowing it to determine the hydrodynamic size of the analytes.

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4 protocols using dynapro dls

1

Characterizing ApoE Lipid Binding by DLS

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Lipid‐free and lipid‐bound ApoE (0.1 mg·mL−1 in PBS) were analyzed using dynamic light scattering (DLS). DLS experiments were conducted with a DynaPro DLS plate reader (Wyatt Technology) at 25 °C and at a scattering angle of 158°. Data were analyzed using Dynamics® software (Wyatt Technology) and represent the averages of 15 acquisitions (10 s per acquisition).
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2

Measuring TDP-43 LCD Particle Size

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Dynamic light scattering (DLS), also known as photon correlation spectroscopy or quasi-elastic light scattering, measures the fluctuation of intensity of scattered light with time. Using a DynaPro DLS plate reader III instrument (Wyatt, Santa Barbara, CA, USA) equipped with an 830 nm laser source, we determined the hydrodynamic radius of the particles. One hundred microliters of each sample (containing 20 µM of TDP-43 LCD) was placed into a flat-bottom 96-well microclear plate (Greiner, Frickenhausen, Germany). Ten image acquisitions of particles were taken at approximately 150x of data per replicate (replicate n = 3). Data were acquired, and Wyatt Dynamics software 7.8.1.3 was used to calculate the average radius.
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3

Vesicle Size Characterization by DLS

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DLS EV size measurements were performed on AF4 separated vesicular fractions using the DynaPro DLS plate reader (Wyatt Technology Corp., Santa Barbara, CA) in 96-well plates. The DLS data were analyzed using Dynamics version 7.8.1.3. software (Wyatt Technology Corp).
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4

Dynamic Light Scattering Characterization

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DLS was carried out using a 384-well plate DynaPro DLS instrument (Wyatt Technology, Santa Barbara, California) equipped with a 830-nm laser and digital autocorrelator. 35 μL of sample was loaded into each well and the plate was spun at 2000 rpm for 30 s to remove any air bubbles prior to measurement at 20 °C or 25 °C, respectively. The z-average translational diffusion coefficient was determined from cumulant analysis of the autocorrelation function61 (link), and modeled as Dz(ctot)=1+kDM1ctoticiMi2DiiciMi2 using species’ molar concentrations as predicted from sample composition and mass action law (Eq. 17), with species’ diffusion coefficients Dj = sjRT/Mj(1-vρ) and approximating nonideality with a single average nonideality coefficient and total protein weight concentration wtot=M1ctot .
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