Table 2.
Characterization of nanoparticle PEG surface coverage and nanoparticle diffusivity in human CF sputum (Deff) compared to in water (Dw)
| Formulation | Hydrodynamic Diameter a (nm) |
PEG Surface Density b (molecules/100 nm2) |
[Γ/SA] c | PEG Regime d | Dw/Deffe |
|---|---|---|---|---|---|
| CK30PEG10k | 60 | 4.5 ± 0.4 – 9.0 ± 0.8 | 2.1 ± 0.2* – 4.1 ± 0.3* | Brush | 6,000 |
| CK30PEG5k | 56 | 4.3 ± 0.2 – 8.6 ± 0.4 | 0.98 ± 0.05* – 2.0 ± 0.1* | Brush | 5,000 |
| CK30PEG2k | 81 | 5.0 ± 0.1 – 10 ± 0.2 | 0.45 ± 0.01 – 0.9 ± 0.02 | Mushroom | 6,000 |
| PS-PEG2k | 210 | 120 ± 4** | 11 ± 1** | Dense Brush | 30 |
Hydrodynamic diameter measured by dynamic light scattering.
For DNA nanoparticles, PEG surface density calculated assuming stoichiometric ratios of poly-L-lysine ε-amines to DNA phosphate groups (N:P) in the range from 1 to 2. For PS-PEG2k, PEG surface coverage reported previously [19]. ** denotes statistical significance (P < 0.01) as compared to all other groups.
Ratio of total unconstrained PEG surface area coverage [Γ] to total particle surface area [SA]. For DNA nanoparticles, [Γ/SA] calculated assuming N:P ratios in the range from 1 to 2. * denotes statistical significance (P < 0.05) as compared to CK30PEG2k at the same N:P ratio. ** denotes statistical significance (P < 0.01) as compared to all other groups.
PEG regime defined as being mushroom coverage for [Γ/SA] < 1 and brush coverage for [Γ/SA] > 1, as illustrated in Figure 6.
Dw is the theoretical diffusivity of particles in water calculated from the Stokes-Einstein equation and the hydrodynamic diameter measured by dynamic light scattering. Deff is the effective diffusivity in CF sputum measured at a time scale of 1 s. The Dw/Deff ratio indicates by what multiple the average particle movement rate in fresh CF sputum is slower than in pure water.