“…Specifically, we expand the shape functionr in terms of the spherical harmonics Y m (θ , φ), wherẽ r ≡ r/R, θ and φ are the dimensionless radial distance, polar angle and azimuthal angle, with respect to the centre of the drop. Such expansions have been employed in 10 -1 10 -2 10 1 5 50 0 0.2 0.4 0.6 0.8 1.0 0 0.2 0.4 0.6 0.8 1.0 10 0 10 -1 10 -2 10 2 10 1 10 0 10 -1 10 3 10 2 10 1 (a) ( b) previous works to study the dynamics of drops under sudden increase or decrease, as well as oscillations, of electric fields (Basaran et al 1995), the motion of bubbles in inviscid fluids (Meiron 1989;Kushch et al 2002) and the stability of bubbles under electric fields (Shaw & Spelt 2009). Owing to the axial and mirror symmetry of the drop, the expansion must be φ-independent, and consist only of m = 0 and even = 2j modes, where j is a non-negative integer.…”