“…One might expect the cross-over seen in Figure 5.41 to disappear, and the count rates to be increased in the order of duty cycle 1:7,1:4 and 1:2, with the most luminescence from continuous-wave insonation, the count rate now being simply a function of the total time of insonation. Pickworth et al [261,296] obtained the pulse-energy distribution spectrum in fluid 1.875 g/1 agar at 22° C. This substance had a viscosity of 170 ± 10 cp, and so was still fluid; since viscosity is a second-order effect when describing the actual bubble oscillations (equation (4.81)), then the actual cavitational behaviour will be similar to that in water. What will be different is the scale of the migrations, which will be greatly reduced in agar, because of the increased viscosity [319].…”