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Unsteady flow in an annulus between two concentric rotating spheres
Authors:S. D. Gulwadi and A. F. Elkouh
Affiliation:(1) Dept. of Mechanical and Industrial Engineering, Marquette University, 53233 Milwaukee, WI, USA
Abstract:An analysis is presented for the unsteady laminar flow of an incompressible Newtonian fluid in an annulus between two concentric spheres rotating about a common axis of symmetry. A solution of the Navier-Stokes equations is obtained by employing an iterative technique. The solution is valid for small values of Reynolds numbers and acceleration parameters of the spheres. In applying the results of this analysis to a rotationally accelerating sphere, a virtual moment of intertia is introduced to account for the local inertia of the fluid.Nomenclature Ri radius of the inner sphere - Ro radius of the outer sphere - 
$$bar r$$
radial coordinate - r dimensionless radial coordinate,
$${{bar r} mathord{left/ {vphantom {{bar r} {R_i }}} right. kern-nulldelimiterspace} {R_i }}$$
- theta meridional coordinate - phgr azimuthal coordinate - 
$$bar t$$
time - t dimensionless time,
$${{bar tv} mathord{left/ {vphantom {{bar tv} {R_i^2 }}} right. kern-nulldelimiterspace} {R_i^2 }}$$
- Rei instantaneous Reynolds number of the inner sphere,ohgriRk2/ngr - Reo instantaneous Reynolds number of the outer sphere,ohgroRo2/ngr - 
$$bar V_r $$
radial velocity component - Vr dimensionless radial velocity component,
$${{bar V_r R_i } mathord{left/ {vphantom {{bar V_r R_i } v}} right. kern-nulldelimiterspace} v}$$
- 
$$bar V_theta  $$
meridional velocity component - Vtheta dimensionless meridional velocity component,
$${{bar V_theta  R_i } mathord{left/ {vphantom {{bar V_theta  R_i } v}} right. kern-nulldelimiterspace} v}$$
- 
$$bar V_phi  $$
azimuthal velocity component - Vphgr dimensionless azimuthal velocity component,
$${{bar V_phi  R_i } mathord{left/ {vphantom {{bar V_phi  R_i } v}} right. kern-nulldelimiterspace} v}$$
- 
$$bar T$$
viscous torque - T dimensionless viscous torque,
$${{3bar T} mathord{left/ {vphantom {{3bar T} {8pi mu R_i }}} right. kern-nulldelimiterspace} {8pi mu R_i }}$$
- 
$$bar T_i $$
viscous torque at surface of inner sphere - Ti dimensionless viscous torque at surface of inner sphere,
$$3{{bar T_i } mathord{left/ {vphantom {{bar T_i } {8pi mu vR_i }}} right. kern-nulldelimiterspace} {8pi mu vR_i }}$$
- 
$$bar T_o $$
viscous torque at surface of outer sphere - To dimensionless viscous torque at surface of outer sphere,
$$3{{bar T_o } mathord{left/ {vphantom {{bar T_o } {8pi mu vR_i }}} right. kern-nulldelimiterspace} {8pi mu vR_i }}$$
- 
$$bar T_{p,i} $$
externally applied torque on inner sphere - Tp,i dimensionless applied torque on inner sphere,
$${{3bar T_{p,i} } mathord{left/ {vphantom {{3bar T_{p,i} } {8pi mu vR_i }}} right. kern-nulldelimiterspace} {8pi mu vR_i }}$$
- 
$$bar Z$$
moment of inertia of inner sphere - Zi dimensionless moment of inertia of inner sphere,
$${{3bar Z_i } mathord{left/ {vphantom {{3bar Z_i } {8pi rho R_i^5 }}} right. kern-nulldelimiterspace} {8pi rho R_i^5 }}$$
- 
$$bar Z_{i,v} $$
virtual moment of inertia of inner sphere - Zi,v dimensionless virtual moment of inertia of inner sphere,
$${{3bar Z_{i,v} } mathord{left/ {vphantom {{3bar Z_{i,v} } {8pi rho R_i^5 }}} right. kern-nulldelimiterspace} {8pi rho R_i^5 }}$$
- 
$$bar Z_{o,v} $$
virtual moment of inertia of outer sphere - ohgri instantaneous angular velocity of the inner sphere - ohgro instantaneous angular velocity of the outer sphere - rgr density of fluid - mgr viscosity of fluid - ngr kinematic viscosity of fluid,mgr/rgr - lambda radius ratio,Ri/Ro - 
$$bar Omega $$
swirl function,
$$bar V_phi  bar rsin theta $$
- OHgr dimensionless swirl function,
$${{bar Omega } mathord{left/ {vphantom {{bar Omega } v}} right. kern-nulldelimiterspace} v}$$
- 
$$bar psi $$
stream function - psgr dimensionless stream function,
$${{bar psi } mathord{left/ {vphantom {{bar psi } {R_i v}}} right. kern-nulldelimiterspace} {R_i v}}$$
- gammai acceleration parameter for the inner sphere,
$$left( {{{R_i^4 } mathord{left/ {vphantom {{R_i^4 } {v^2 }}} right. kern-nulldelimiterspace} {v^2 }}} right){{domega _i } mathord{left/ {vphantom {{domega _i } {dbar t}}} right. kern-nulldelimiterspace} {dbar t}} = {d mathord{left/ {vphantom {d {dbar t}}} right. kern-nulldelimiterspace} {dbar t}}left( {operatorname{Re} _i } right)$$
- gammao acceleration parameter for the outer sphere,
$$left( {{{R_i^4 } mathord{left/ {vphantom {{R_i^4 } {v^2 }}} right. kern-nulldelimiterspace} {v^2 }}} right){{domega _i } mathord{left/ {vphantom {{domega _i } {dbar t}}} right. kern-nulldelimiterspace} {dbar t}}$$
- 
$$bar tau _{rphi } $$
shear stress - taurphgr dimensionless shear stress,
$$bar tau _{rphi } {{R_i^2 } mathord{left/ {vphantom {{R_i^2 } {mu v}}} right. kern-nulldelimiterspace} {mu v}}$$
Keywords:
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