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aggregates and the stress to break up into CB aggregates must be almost the same
for the furnace black samples.
Finally, we mention briefly the reasons why the  y values of the AcB
suspensions are larger than those of CB-76, CB-24-1, and CB-15-2 suspensions.
The surface of AcB develops a graphite structure, although that of the furnace
black does not. The surface structure difference may be attributed to different PS
adsorption behavior and the  eff dependence of the  y values, although we cannot
explain the mechanism yet.
Figure 18. Yield stress  y versus effective volume fraction  eff for the CB-76/(PS/DBP),
CB-24-1/(PS/DBP), CB15-2/(PS/DBP), and AcB/(PS/DBP) suspensions. a 0 100 nm [32].
4.5. Summary
Steady-shear viscosity of CB/(PS/DB) suspensions are reported as a function
of volume fraction () of various kinds of CB aggregates. The effects of the
primary particle size and the structure of CB aggregates on the rheological
properties are clarified. The suspensions show a typical shear-thinning behavior in
the range of a shear rate studied. The Casson model can be applied to evaluate the
viscosity at infinite of shear rate  and the yield stress  y for the suspensions.
Relative viscosity  / m , ( m : medium viscosity) thus obtained are compared to
the high-frequency viscosity for the ideal hard-sphere silica suspensions to
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