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. 2017 Jul 7;8:1396–1406. doi: 10.3762/bjnano.8.141

Table 1.

Physicochemical characterisation of the 50 nm and 150 nm SiO2-NPs in different media. Nanoparticle dispersion (100 µg/mL) in water, serum free HBSS and HBSS supplemented with 10% foetal bovine serum (FBS) were characterised by differential centrifugal sedimentation (DCS) and dynamic light scattering (DLS) as described in the Experimental section. The table shows the apparent diameter and peak full width at half maximum (FWHM) obtained by DCS, together with the results obtained by cumulant analysis of the DLS data (z-average diameter and polydispersity index, PDI). The corresponding distributions are shown in Supporting Information File 1, Figures S2 and S3. For DLS results, errors represent standard deviation of 4 replicates (11 runs each).

Nanoparticle Medium DCS apparent diameter (nm) DCS FWHM (nm) Diameter (z-average, nm) PDI

50 nm SiO2 water 41 20 76a 0.159a
HBSS 44 23 79 ± 1b 0.17 ± 0.02b
HBSS, 10% FBS 50 27 102 ± 3c 0.42 ± 0.07c
150 nm SiO2 water 160, 183d 60d 154 ± 4 0.03 ± 0.03
HBSS 159, 181d 60d 190 ± 2 0.02 ± 0.01
HBSS, 10% FBS 149, 170d 60d 209 ± 2 0.18 ± 0.02

aData (for equivalent batch) reproduced from [42]. bThe presence of larger particles in the distribution of sizes (see DCS data in Supporting Information File 1, Figure S3) will bias the DLS average towards larger sizes due to the stronger scattering from larger particles (the scattering intensity grows strongly with particle size). cA second small peak around 10 nm due to the presence of proteins was also visible (Supporting Information File 1, Figure S2) which explains the high average diameter and PDI. This was not visible for the larger particles, likely due to the substantially stronger scattering stemming from them. dMultiple peaks were observed by DCS (Supporting Information File 1, Figure S3) and both peak positions are reported together with the combined width.