“…Positive acoustic contrast, in which case all particles will collect in a nodal plane, requires that Φ = f 0 + 3 2 f 1 > 0. In practice, this is the situation not only for solid particles levitating in air, for which the set of scattering coefficients (f 0 , f 1 ) can be well approximated by (1,1), but also for liquid droplets in air, so long as their shape remains approximately constant (large shape oscillations, breakup and coalescence introduce considerable complications [41,42]). Φ is also positive for solid spheres in water, such as polystyrene particles with (f 0 , f 1 ) = (0.47, 0.038), and for many types of live cells and liquid droplets in water, e.g.…”