2005
DOI: 10.1017/s0022112005005677
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Migration of a sphere in tube flow

Abstract: The cross-stream migration of a single neutrally buoyant rigid sphere in tube flow is simulated by two packages, one (ALE) based on a moving and adaptive grid and another (DLM) using distributed Lagrange multipliers on a fixed grid. The two packages give results in good agreement with each other and with experiments. A lift law L = CU s (Ω s − Ω se ) analogous to L = ρU Γ which was proposed and validated in two dimensions is validated in three dimensions here; C is a constant depending on material and geometri… Show more

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Cited by 128 publications
(117 citation statements)
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“…In a tube flow, initially randomly distributed particles gradually focus into a narrow annulus at around 0.3 diameter, resulting in the "tubular pinch" effect. This phenomenon was later confirmed in several experimental Matas et al 2004) and analytical (Schonberg & Hinch 1989) and numerical (Feng et al 1994;Yang et al 2005) studies. Similar phenomenon occurs in square-and rectangular-shaped channels, where particles accumulate at 0.3 times the width of the channel away from the centreline (Chun & Ladd 2006;Kim & Yoo 2008;Shao et al 2008;Choi et al 2011).…”
Section: Introductionmentioning
confidence: 54%
“…In a tube flow, initially randomly distributed particles gradually focus into a narrow annulus at around 0.3 diameter, resulting in the "tubular pinch" effect. This phenomenon was later confirmed in several experimental Matas et al 2004) and analytical (Schonberg & Hinch 1989) and numerical (Feng et al 1994;Yang et al 2005) studies. Similar phenomenon occurs in square-and rectangular-shaped channels, where particles accumulate at 0.3 times the width of the channel away from the centreline (Chun & Ladd 2006;Kim & Yoo 2008;Shao et al 2008;Choi et al 2011).…”
Section: Introductionmentioning
confidence: 54%
“…All cases are found to yield a solid-solid clash within a finite scaled time. This can be contrasted and compared with the interesting findings of Yih [34], Korobkin [35], Korobkin & Ohkusu [36], Schonberg & Hinch [19], Newman [37], Tuck [38], Fortes et al [39], Huang et al [40], Yang et al [41] and Ardekani et al [42]. The typical present clash occurs mid-body instead of at the leading edge as in Smith & Ellis [32] and this new form is examined in detail in § §3 and 4.…”
Section: Introductionmentioning
confidence: 82%
“…The lift coefficient is zero at the centerline and is called an unstable equilibrium position. 42 Because the gradient of the force is non-zero, a small disturbance can drive a droplet away from the centerline and toward the wall. Interestingly, the stable zero-lift positions for the two velocity profiles coincide at the same scaled position y/W = 0.3.…”
Section: Theoretical Analysis a Lift Forcementioning
confidence: 99%