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Zetasizer nano zs 3600

Manufactured by Malvern Panalytical
Sourced in United Kingdom

The Zetasizer Nano ZS 3600 is a dynamic light scattering (DLS) instrument used for the measurement of particle size and zeta potential. It can analyze samples with particle sizes ranging from 0.3 nanometers to 10 micrometers. The instrument uses a laser light source and detects the scattered light to determine the size distribution and zeta potential of the particles in a sample.

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14 protocols using zetasizer nano zs 3600

1

Characterizing SPION Nanoparticle Size

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The SPIONs used for this study are commercially available and quoted as being 5 nm in diameter, determined by Transmission Electron Microscopy (TEM) [61 ]. However, the size of the molecules when dispersed in an aqueous solution is unclear. DLS was used to quantify the diameter of hydrodynamic radius and provide detail about the nature of the dispersion.
The experiment was carried out at the National Physical Laboratory, and followed the methods described by Minelli et al. [62 (link)]. This is a validated method for determining nanoparticle size. A Zetasizer (Zetasizer Nano ZS 3600, Malvern Panalytical Ltd, Malvern, UK) was used which performs measurements using a 633 nm Helium-Neon laser, measuring the light at a scattered angle of 173°. The particles were diluted to a range of concentrations; stock dilution, 1:1, 1:4, 1:6 and 1:20, with measurements carried out at temperature of 25°C and 3 repeats for each sample. The average diameter for each sample was noted along with peaks in the measurements to determine any variation in size of agglomeration of the particles.
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2

Zeta Potential Measurement in Colloids

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Zeta potential is the electrokinetic potential in colloidal solutions, which is formed between the electrical bilayer of the particles and the surrounding medium in which they are dispersed. The zeta potential, as the main parameter of colloidal stability, was measured in capillary cells using a Zetasizer NanoZS 3600 (Malvern Instruments) using the principle of Laser Doppler velocimetry combined with electrophoresis.
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3

Measuring Colloidal Particle Size by DLS

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The hydrodynamic diameter of the colloidal MF solution was measured using a Zetasizer NanoZS 3600 (Malvern Instruments, Malvern, UK). This instrument uses the principle of DLS, also known as photon correlation spectroscopy or quasi-elastic light scattering. This method allows the analysis of the intensity of the fluctuation of scattered light from particles in solution, which are undergoing Brownian motion. Measurement of their rate of diffusion in a liquid medium is related to their size, according to the Stokes–Einstein equation. The average hydrodynamic diameter HYDR> was measured using disposable polystyrene cuvettes at 25 °C. The size distribution was plotted using Zetasizer software as a function of the relative number of particles to their size, with the hydrodynamic diameter representing the maximum of the curve. The measurement of each sample’s hydrodynamic size was performed three times; the resulting HYDR> was the average of these values.
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4

Characterization of Nanoparticle Properties

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Particle size, Polydispersity Index, and Zeta Potential were determined by Dynamic Light Scattering (DLS) technique performed by Zetasizer Nano ZS 3600 (Malvern Instruments, Worcestershire, United Kingdom) device. The mentioned factors were measured twice; firstly, immediately after preparation, and secondly, after lyophilization [13 (link)].
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5

Dynamic Light Scattering and Zeta Potential Analysis of MWNT Suspensions

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Dynamic light scattering (DLS) and zeta potential analyses were used as part of a quality control routine for the preparation of all MWNT suspensions, as previously described [50 (link),51 (link),54 (link)]. The particle size distributions, in terms of hydrodynamic diameter, of the BSA-MWNT suspensions were determined by DLS. In brief, aliquots of purified pMWNT or cMWNT suspensions were diluted 1:10 in a 0.10 mg/mL BSA working solution and analyzed with a Zetasizer Nano-ZS 3600 (Malvern Instruments, Worcestershire, UK) using a 633-nm laser and a backscatter measurement angle of 173°. The instrument was calibrated with Polybead® standards (Polysciences, Warrington, PA, USA) and ten consecutive 30-s runs were taken per measurement at 25 °C. The hydrodynamic diameter was calculated using a viscosity and refractive index of 0.8872 cP and 1.330, respectively for deionized water, and an absorption and refractive index of 0.010 and 1.891, respectively, for MWNTs. Zeta potential values were also determined for purified BSA-coated MWNT suspensions that were diluted 1:10 with deionized water. In addition, DLS and zeta potential analyses were performed periodically on purified MWNT suspensions stored at 4 °C. Typically, MWNT suspensions were stable in storage for months, indicated by the lack of aggregates detected by DLS and constant zeta potential results.
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6

Characterization of BSA-coated MWNT Suspensions

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The particle size distributions, in terms of hydrodynamic diameter, of BSA-MWNT suspensions were determined by dynamic light scattering (DLS). In brief, aliquots of purified pMWNT or cMWNT suspensions were diluted 1:10 in a 0.10 mg/mL BSA working solution and analyzed using a 633-nm laser and a backscatter measurement angle of 173° (Zetasizer Nano-ZS 3600, Malvern Instruments, Worcestershire, UK). The instrument was calibrated with Polybead® standards (Polysciences, Warrington, PA, USA) and ten consecutive 30-s runs were taken per measurement at 25 °C. The hydrodynamic diameter was calculated using a viscosity and refractive index of 0.8872 cP and 1.330, respectively, for deionized water, and an absorption and refractive index of 0.010 and 1.891, respectively, for MWNTs. Zeta potential values were also determined for purified BSA-coated MWNT suspensions that were diluted 1:10 with deionized water, medium with serum, or serum-free medium. In addition, DLS and zeta potential analyses were performed periodically on purified MWNT suspensions stored at 4 °C to detect any changes. Typically, MWNT suspensions were stable in storage for months, indicated by the lack of aggregates detected by DLS and constant zeta potential results.
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7

Particle Size Analysis of PF108 and CNT-PF108 Suspensions

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The particle size distributions of polymers in the non-sonicated and sonicated PF108 solutions and CNTs in the undialyzed and dialyzed CNT-PF108 suspensions were analyzed by dynamic light scattering (DLS) using a 633 nm laser source at a fixed angle of 173° (Zetasizer Nano-ZS 3600, Malvern Instrument, Worcestershire, UK). All PF108 solutions were analyzed at a final concentration of 0.1mM in MilliQ water. Aliquots of CNTPF108 suspensions were diluted to a final concentration of 0.1mM PF108 and 50 μg/mL CNTs with MilliQ water immediately prior to analysis. 500 μL of each sample was placed in a disposable polystyrene cuvette and 10 consecutive 30-s runs were taken per measurement at 25 °C. Three independent DLS measurements were acquired per sample, and the average particle size and distribution, in terms of hydrodynamic diameter (HDD) and polydispersibility index (PDI) values, were calculated for each sample (Table S1).
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8

Evaluating CNT-PF108 Surface Charges

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Net surface charges of various undialyzed and dialyzed CNT-PF108 suspensions were analyzed using a Malvern Instrument Zetasizer Nano-ZS 3600. All samples were diluted to a final concentration of 0.1mM PF108 and 50 μg/mL CNTs in MilliQ water. The viscosity of the 0.1mM PF108 was determined with a viscometer to be 0.7327 cP and a transfer standard (DTS 1235, Malvern) was used to verify the correct operation of the instrument that measures zeta potential in a capillary cell, where the temperature was equilibrated to 25 °C throughout the operation.
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9

Oligomer Size Analysis of α-casein

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αS1-casein (1 mL, 50 µM) in phosphate buffer was incubated for 3 h at 37 °C. Samples were transferred into a quartz cuvette. Proteinoligomer diameter and oligomers’ population PI were analyzed by PCS (Zetasizer NanoZS3600, Malvern Instruments, Worcestershire, UK). Before each measurement, samples were equilibrated for at least 2 min. The mean of 15 single measurements was recorded. Samples were recorded with an attenuator value of 8. Temperature denaturation was recorded by a heating rate resolution of 0.5 °C.
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10

Hydrodynamic Diameter of MFer Colloids

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The hydrodynamic diameter for MFer colloidal solutions was determined by dynamic light scattering (DLS) performed at Zetasizer Nano ZS 3600 (Malvern Instruments, Malvern, UK) using the Stokes-Einstein’s equation:
DT=k T6 π η Rh
where DT is the diffusion coefficient, k is the Boltzmann constant, T is the temperature, η is the solvent viscosity, and Rh is the Stokes, or hydrodynamic, radius of a spherical particle. The hydrodynamic diameter DHYDR was measured using disposable polystyrene cuvettes in the protein mode of the data analysis at 25 °C. The size distribution was displayed in the Zetasizer software as a dependence of the relative number of particles on their size, and the hydrodynamic diameter represented the maximum of the curve. The temperature trend was followed using glass cuvettes in the protein mode of the data analysis.
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