Breakup of an anomolously viscous liquid film in a centrifugal force field |
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Authors: | I. M. Nafikov N. Kh. Zinnatullin |
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Affiliation: | (1) S. M. Kirov Kazan' Chemicotechnological Institute, USSR |
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Abstract: | ![]() An equation is obtained for the breakup radius with consideration of tipping moments and Laplacian pressure forces acting on the liquid ridge at the critical point.Notation K, n rhenological constants - density - surface tension - r current cup radius - R maximum cup radius - rc critical radius for film breakup - ¯r=¯r=r/R dimensionless current radius - ¯rc=rc/R dimensionless critical radius - 0, c actual and critical film thicknesses - current thickness - Rr ridge radius - h0 ridge height - h current ridge height - 0 limiting wetting angle - current angle of tangent to ridge surface - angle between axis of rotation and tangent to cup surface - angular velocity of rotation - q volume liquid flow rate - v1 and v meridional and tangential velocities - =4vvlm/ r, =4v m/ r dimensionless velocities - M moments of surface and centrifugal forces - Mv moment from velocity head - pr pressure within ridge - Pvm pressure from velocity head - p m, ppm pressures from centrifugal force components tangent and normal to cup surface - deviation range of breakup radius from calculated value - ¯rmax, ¯rmin limiting deviations of breakup radius - c angle of tangent to curve c/°0=f(¯r) at critical point - t random oscillation of ratio c/ cTranslated from Inzhenerno-Fizicheskii Zhurnal, Vol. 39, No. 1, pp. 51–56, July, 1980. |
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