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7 protocols using delsa 440sx

1

Liposome Size and Charge Characterization

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The size and surface charge of the empty, functional loaded liposomes were measured by Dynamic Light Scattering, DLS, (Coulter Sub-Micron Particle Analyzer N4SD, equipped with a 4 mW helium-neon laser and 90 u detector) and Zeta potential (Coulter DELSA 440 SX), respectively.
Liposome dispersions were diluted with Tyrode Buffer Saline pH 7.40 and ζ-potential values were measured at 25 °C. As the radii of liposomes were always large enough compared with the Debye–Huckel parameters, the ζ-potentials were calculated directly by means of the Helmoholtz–Smolowkovski equation (by the zetasizer) [44 ].
Size was also calculated in the same experiments, according to the procedure described by Langley [45 ].
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2

Liposomal Characterization: Size, Charge, and Stability

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The complete liposomes with negative surface charges could inhibit the aggregation or surface repulsion due to similarly charged particles [51 (link),52 (link)]. Zeta potential indicates the overall charge present and stability of liposomal systems. The mean size and polydispersity index (P.I.) were calculated by Malvern Zetasizer Nano ZS90 (Malvern Instruments Ltd., Malvern, UK). The zeta potential values were calculated from the electrophoretic mobility by means of the Helmholtz–Smoluchowski relationship [53 (link)]. Zeta potential measurement is also important to monitor liposomal stability during liposomes’ precipitation and fusion control [54 (link)].
The size and surface charge of DIC- and DEX-loaded liposomes were measured by dynamic light scattering (DLS; Delsa™ Nano Particle Analyzer; Beckman Coulter, Fullerton, CA, USA) and zeta potential (Coulter DELSA 440 SX), respectively. The autocorrelation function of the scattered light was analyzed by the cumulant method as described previously [55 (link)].
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3

Characterizing Liposome Size and Charge

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The size and surface charge of the plain, functional loaded liposomes were measured by Dynamic Light Scattering, DLS, (Coulter Sub-Micron Particle Analyzer N4SD, equipped with a 4 mW helium-neon laser and 90u detector) and Zeta potential (Coulter DELSA 440 SX), respectively.
Liposome dispersions were diluted with TBS pH 7.40 and ζ-potential values were measured at 25 °C. As the radii of liposomes were always large enough compared with the Debye-Huckel parameters, the ζ-potentials were calculated directly by means of the Helmoholtz-Smolowkovski equation (by the zetasizer) [28] . Size was also calculated in the same experiments, according to the procedure described by Langley [29] .
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4

Zeta Potential Measurement of -2 μm Pulp

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A Coulter Delsa 440sx zeta analyzer (Beckman Coulter, Brea, CA, USA) was used to perform zeta potential measurement. A KCl solution (1 × 10−3 mol/L) was used as a supporting electrolyte. A total of 30 mg of the −2 μm sample was used for each test. The pulp preparation process for the test was identical to that of the microflotation investigation. Zeta potential was measured using the supernatant liquor after the pulp settled for 10 min. At each reagent condition, at least three independent tests were performed.
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5

Synthesis and Characterization of DMSA-coated Magnetite FeNPs

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The DMSA-coated magnetite FeNPs were synthesized by thermal decomposition [69 (link)]. The size and dispersibility of the FeNPs were evaluated using a transmission electron microscope (JEM-2100). The hydrodynamic size distribution of the FeNPs was analyzed with a submicron particle analyzer (Beckman Coulter N4 Plus). The surface charge of the FeNPs was measured with a zeta potential analyzer (Beckman Coulter Delsa 440SX).
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6

Characterization of Graphene Nanoparticles

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The average particle size
(d50) of graphene was around 1377.5 ±
140.8 nm, which was measured by a particle size analyzer (Coulter
Multisizer II, Beckman Coulter, Fullerton, CA). The surface area of
graphene was measured to be 212.56 m2/g by using a surface
area analyzer (Coulter SA 3100, Beckman Coulter, Fullerton, CA). The
zeta-potential of graphene at pH = 7.0 ± 0.2 was around −19.98
eV by a zeta-potential analyzer (Coulter DELSA 440SX, Beckman Coulter,
Fullerton, CA). The X-ray diffraction pattern of graphene was recorded
by an X-ray powder diffractometer (D8 ADVANCE, Bruker, Germany) (Figure S1). The morphology of graphene was examined
by scanning electron microscopy (SEM) (Hitachi S-4800 FEG SEM, Tokyo,
Japan) (Figure S2) and transmission electron
microscopy (TEM) (Philips Tecnai G220 S-TWIN, Amsterdam, The Netherlands)
(Figure S3).
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7

Multi-Analytical Characterization of Materials

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The Diffuse Reflectance Infrared Fourier Transform Spectroscopy were tested by a Shimadzu FTIR 8120 spectrometer at a wavenumber range between 4000 and 600 cm−1. The SEM images were examined by a Mira3 LMU SEM (Tescan, Czech Republic) with the voltage of 20 kV. The TEM images and EDX mapping analysis were collected with a Titan G2 60-300 with the voltage of 30 kV. The differential thermal analysis was analyzed using the STA449C (NETZSCH, GER), which ranged from 30 to 1000 °C with 5 °C/min rate of rise. XRD measurements were obtained by Rigaku TTR III at range between 5 and 80°. The absorbance (OD) value was obtained from a microplate reader (EnVision Xcite, PerkinElmer). Zeta potentials of samples were measured with a Zeta-sizer Delsa440sx instrument (Beckman Coulter, Brea, CA, USA). The water contact angle was tested with a contact angle goniometer (JY-82C, Chengde Dingsheng Testing Machine Testing Equipment Co., Ltd.). OriginPro (version 8.5) was used to treated the data for materials properties analysis.
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