2016
DOI: 10.1007/978-3-319-20961-6
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Modelling of Convective Heat and Mass Transfer in Rotating Flows

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Cited by 47 publications
(48 citation statements)
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“…The flow structure in the RVR reactor broadly agreed with the Batchelor's predictions and other similar studies [9,10]. The Batchelor's prediction was arrived at by solving a simplified form of Navier-Stokes equation to obtain an approximate flow field Figures 5a-d and 6a-d shows the radial profiles of the circumferential velocity vector fields and contours, and the vorticity vector maps and contours on the rotating disc boundary layer and on three Y-Z planes along the reactor wheelspace, which seems to be consistent with the theoretical descriptions given in Figure 1b and Equations (6) and (7). Away from the boundary layer near the rotor in the radial direction, there was a sharp increase the radial vorticity profile with respect to the radial distance (Figure 6b-d).…”
Section: Radial Distribution Of the Hydrodynamic Quantitiessupporting
confidence: 69%
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“…The flow structure in the RVR reactor broadly agreed with the Batchelor's predictions and other similar studies [9,10]. The Batchelor's prediction was arrived at by solving a simplified form of Navier-Stokes equation to obtain an approximate flow field Figures 5a-d and 6a-d shows the radial profiles of the circumferential velocity vector fields and contours, and the vorticity vector maps and contours on the rotating disc boundary layer and on three Y-Z planes along the reactor wheelspace, which seems to be consistent with the theoretical descriptions given in Figure 1b and Equations (6) and (7). Away from the boundary layer near the rotor in the radial direction, there was a sharp increase the radial vorticity profile with respect to the radial distance (Figure 6b-d).…”
Section: Radial Distribution Of the Hydrodynamic Quantitiessupporting
confidence: 69%
“…The circumferential velocity in a forced vortex flow increases radially outwards with the radius attaining a maximum at the tip of the disc (tip velocity), while the vorticity magnitude is nearly constant with its amplitude twice the angular velocity of the rotating disc. The flow in the reactor system on the boundary layers may be characterized by a certain degree of flow instability when it is above the critical Reynolds number Re ϕ, critical ≈ 2 × 10 5 with small patches of turbulence or oscillating vortex disturbance [7,8]. This can be expressed mathematically for the boundary layer near the rotor using the local rotational Reynolds number Re ϕ, local (Equation (1)).…”
Section: Theoretical Analysis Of the Fluid Flowmentioning
confidence: 99%
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“…Although these early papers are historically consequential, they are practically inaccessible for many readers. The fundamental theory, derivations, and analyses may be found in more recent http texts and monographs on fluid mechanics and boundary layers [29][30][31]30,32]. The mathematical and computational development in the present paper follows most closely that reported by Kee et al [29].…”
Section: Introductionsupporting
confidence: 62%
“…where the Reynolds number is based on the disk radius [55,56,32]. The present analysis is based on a Reynolds number in which the length scale is the separation distance between the inlet manifold and the stagnation surface, L. Correlations are presented for Reynolds numbers up to Re L ¼ 10 4 , which would represent a very high-speed flow.…”
Section: Limitationsmentioning
confidence: 99%