2005
DOI: 10.1063/1.1941617
|View full text |Cite
|
Sign up to set email alerts
|

Comparison between Navier-Stokes and DSMC Calculations for Low Reynolds Number Slip Flow Past a Confined Microsphere

Abstract: Abstract. In the present investigation, slip-continuum and molecular (DSMC) flow models have been used to compare the drag coefficient on a confined microsphere over a range of Knudsen numbers between 0.01 and 0.4. The simulations consider a fixed Reynolds number (Re=0.125) and a range of blockage ratios from 2.0 up to 13.0. Two separate problem formulations have been studied; the first considers flow past a confined sphere moving with a constant velocity along the central axis of the pipe while the second con… Show more

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

1
5
0

Year Published

2011
2011
2022
2022

Publication Types

Select...
6

Relationship

0
6

Authors

Journals

citations
Cited by 10 publications
(6 citation statements)
references
References 3 publications
1
5
0
Order By: Relevance
“…The data in best agreement with the model are the D p = 7.6 µm, P = 760 Torr data, which fall within the slip-flow regime (0.01 < M/ √ Re < 0.1). These findings join other studies [1,23,[43][44][45][46] in illustrating that C D is not solely a function of Re, but also of metrics that reflect changing flow conditions, such as M and Kn. The increasing deviation of the M > 1.2 empirical C D data from the Carlson-Hoglund model in Figure 4 is attributed to the suppression of flow characteristics in increasingly rarefied conditions.…”
Section: Resultssupporting
confidence: 87%
See 1 more Smart Citation
“…The data in best agreement with the model are the D p = 7.6 µm, P = 760 Torr data, which fall within the slip-flow regime (0.01 < M/ √ Re < 0.1). These findings join other studies [1,23,[43][44][45][46] in illustrating that C D is not solely a function of Re, but also of metrics that reflect changing flow conditions, such as M and Kn. The increasing deviation of the M > 1.2 empirical C D data from the Carlson-Hoglund model in Figure 4 is attributed to the suppression of flow characteristics in increasingly rarefied conditions.…”
Section: Resultssupporting
confidence: 87%
“…This approximation is provided in Figure 3 and shows reasonable agreement with the subsonic P = 760 Torr results from the present work for M < 0.8. This and other approximations of the standard drag curve [31][32][33][34][35][36][37][38][39][40][41][42] overestimate subsonic C D for the P = 76 Torr condition because they are purely functions of Re and do not account for Kn, where Kn describes the degree of rarefaction by the ratio of the molecular mean free path of the fluid to the diameter of the sphere [1,23,30,[43][44][45][46]. The Kn value for the P = 76 Torr condition was 0.18, corresponding to the transitional-flow regime between slip-flow and free-molecule flow [30].…”
Section: Resultsmentioning
confidence: 99%
“…which is valid for compressible viscous model at small Knudsen numbers (see [25]). The local Mach number has been expressed using nondimensional variables as follows: The square size (equal to 1) compared to examined disturbance length (5000) is small and hardly visible.…”
Section: Resultsmentioning
confidence: 81%
“…A Hard Sphere (HS) model and the No Time Counter (NTC) scheme suggested by Bird [17] are implemented in the collision algorithm. A slight modification is introduced in the calculation of the maximum number of collisions N C in each cell [20], which is calculated…”
Section: Fig 2: Configuration and Geometric Parametersmentioning
confidence: 99%