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Additional resources for Cinemascope - Issue 44 - Fall 2010 issue 44
Only Felici  seems to make any observations, stating that, perhaps obviously, for a plane-plane gap it is found that turbulence occurs at a field strength considerably lower than the liquid breakdown strength. 5 Current and Voltage The electric Nusselt number was introduced by eqn. 72) 34 Electrostatics, Electrohydrodynamic Flow, Coupling and Instability I0 is usually taken as the maximum conduction current prior to the occurrence of electroconvection; as Felici  comments, the point at which electroconvection starts is identified by the sudden jump in observed current as the voltage is increased.
The overall aim of this section is to address the physics and flow types occurring in the charged liquid upstream of the atomizer and highlight the role that charge has on this when present. ” Chapter 3 Charge Injection into a Quiescent Dielectric Liquid 3 Charge I njection into a Q uiescent Dielectric Liquid 3 Charge Injection into a Quiescent Dielectric Liquid Abstract. Upstream of the atomizer orifice the dielectric liquid remains in a continuous phase. The physics acting on this region were discussed in the preceding sections however the analysis given automatically assumes that an electrical charge is present.
If qvo=ε0V0/l02 is substituted into eqn. 56) another Prandtl number variant, derived by Schneider & Watson , is defined. The M parameter is characterized in many papers and a concise overview of non-dimensionalization, including a discussion of this, can be found in Atten . 57) A limiting value for the hydrodynamic mobility can be obtained if it is assumed that all of the electrical energy (1/2εE2) is converted to kinetic energy (1/2ρu2). As explained by Atten, this parameter is a measure of the extent of turbulence in the system.