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. 2021 Nov 30;22(23):12946. doi: 10.3390/ijms222312946

Figure 3.

Figure 3

(a,c,e) Hydrodynamic radii (Rh; filled black circles) and decay rates (Γ; empty red circles) and (b,d,f) form factor (P(q)) and the reciprocal of the excess Rayleigh ratio (ΔR−1) as a function of the square of the scattering vector (q2) for small ENPs (peak 2) in the ascites of ovarian cancer (OC) patient OC3 (a,b) and the plasma of patient with benign ovarian cyst (BP-BOC2) (c,d), and for large ENPs (peak 3) in the filtered ascites (ascitesF) of patient OC6 (e,f). In the calculation of Rh values for large ENPs (Figure 3e), the viscosity value ηo ≈ 1.2 mPa s−1 was considered (see Section 4).