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. 2013 Feb 19;104(4):913-23.
doi: 10.1016/j.bpj.2013.01.007.

Do clustering monoclonal antibody solutions really have a concentration dependence of viscosity?

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Do clustering monoclonal antibody solutions really have a concentration dependence of viscosity?

Jai A Pathak et al. Biophys J. .

Abstract

Protein solution rheology data in the biophysics literature have incompletely identified factors that govern hydrodynamics. Whereas spontaneous protein adsorption at the air/water (A/W) interface increases the apparent viscosity of surfactant-free globular protein solutions, it is demonstrated here that irreversible clusters also increase system viscosity in the zero shear limit. Solution rheology measured with double gap geometry in a stress-controlled rheometer on a surfactant-free Immunoglobulin solution demonstrated that both irreversible clusters and the A/W interface increased the apparent low shear rate viscosity. Interfacial shear rheology data showed that the A/W interface yields, i.e., shows solid-like behavior. The A/W interface contribution was smaller, yet nonnegligible, in double gap compared to cone-plate geometry. Apparent nonmonotonic composition dependence of viscosity at low shear rates due to irreversible (nonequilibrium) clusters was resolved by filtration to recover a monotonically increasing viscosity-concentration curve, as expected. Although smaller equilibrium clusters also existed, their size and effective volume fraction were unaffected by filtration, rendering their contribution to viscosity invariant. Surfactant-free antibody systems containing clusters have complex hydrodynamic response, reflecting distinct bulk and interface-adsorbed protein as well as irreversible cluster contributions. Literature models for solution viscosity lack the appropriate physics to describe the bulk shear viscosity of unstable surfactant-free antibody solutions.

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Figures

Figure 1
Figure 1
Schematic of preferential adsorption of surfactant at air/water interface (orogenic displacement). Surfactant molecules (red) have a hydrophobic head and hydrophilic tail, and monoclonal antibody molecules (green) have a Y-shape (Fab and Fc domains).
Figure 2
Figure 2
(a) Cone-plate rheometry data of as-is solutions (taken from the storage refrigerator and allowed to equilibrate to 23°C in the rheometer). Data are shown on the stock solution (107 g L−1) and diluted (10, 26, 50, and 70 g L−1) solutions. (Inset) Viscosity values at 10.4 s−1 (circles) and 1040 s−1 (squares) as a function of protein concentration. (Solid and open symbols) Unfiltered and filtered solutions, respectively. (b) Flow curves of unfiltered solution (solid symbols) and filtered solution (open symbols) at 23°C for 10 g L−1 and 107 g L−1 mAb solutions. (Inset plot) Shear stress versus shear rate.
Figure 3
Figure 3
Flow curves at 23°C of unfiltered mAb solution (107 g L−1) in the cone-plate geometry (blue squares), unfiltered solution in the double gap (red squares), and filtered solution in the double gap geometry (green squares). (Asterisks; same color code applies) Shear stress.
Figure 4
Figure 4
Effects of filtration on the flow curves of surfactant-spiked antibody solution ([mAb] = 100 g L−1) at 5°C. (Squares and diamonds) Viscosity and shear stress, respectively. (Blue and red symbols) Unfiltered and filtered solutions, respectively.
Figure 5
Figure 5
HP-SEC peaks of filtered and unfiltered solutions showing the presence of peaks due to the monomer and reversible clusters. Monomer content is 98% in both cases. Data are only shown on the unfiltered solution for clarity and space. Filtered solutions gave quantitatively identical HP-SEC data as unfiltered solutions.
Figure 6
Figure 6
Autocorrelation function of intensity fluctuations (from dynamic light scattering) of filtered and unfiltered antibody solutions. (Symbols) Experimental data. (Solid lines) Exponential fits (Eq. 2).
Figure 7
Figure 7
Cluster size distribution (MFI data) of (a) unfiltered surfactant-free, (b) filtered surfactant-free, and (c) unfiltered surfactant-laden antibody solutions with representative optical micrographs (inset). Scale bar for micrograph in panel a also applies to panels b and c.
Figure 8
Figure 8
Peclèt number calculated from MFI data for unfiltered and filtered solutions, plotted versus shear rate.
Figure 9
Figure 9
Surface flow curve (surface viscosity and surface shear stress) of mAb solution, compared to BSA data of Sharma et al. (17).

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