TABLE 3
Motion of a single spherical particleRep 1 (Stokes) 1 Rep 104 104 Rep (Newton)drag coefficient, CD 24/Rep
055 482. .
Rep
⎛⎝⎜⎜⎞⎠⎟⎟0.44drag force,
RCAf Dpfv
r^2
23 pmDpv
055 48
82
..vDpfr D vp
mpm
⎛
⎝⎜⎞
⎠⎟0.055prf (vDp)^2gravitational settling equation of
motion m v
t
ppmgRf
pfd
d 1r
r⎛
⎝⎜⎞
⎠⎟or,d
dv
t 1 3
4r 2
rr
rf
pf
ppg DCvD⎛
⎝⎜⎞
⎠⎟terminal velocity, vt (dv/dt 0) Dgpp f2
18rr
m() AAA 12 212
11⎛ +⎝⎜⎜⎞⎠⎟⎟
.A(^1) fpD
48. m
r
AgDpf
f
2 ^254 p
.
rr
r
3
12
Dgpp f
f
()
/
rr
r
⎛
⎝⎜
⎞
⎠⎟
unsteady motion
time, t
velocity, v
t vv
g vv
t
t
t 1 n^0
⎛
⎝⎜
⎞
⎠⎟
t
g CC
p
p Dt t D p
p
(^2422)
0
t
dRe
Re Re Re
Re
∫
not simple because of Rep 104
at initiation of motion
falling distance, S
St
t
∫ 0 vd
vttgtv v t
g
t
t
()exp 0 1
⎛
⎝⎜
⎞
⎠⎟
⎡
⎣
⎢
⎢
⎤
⎦
⎥
⎥
vt
tt
tg p
t
gp p p
t
t
Re
/ , Re Re / Re
0 d
0
∫
Re
18
initial velocity, : terminal v
2
p
pf
g
pp
t
vD D
vv
r
m
t
r
m
,,: 0 eelocity
Rep 0 , Rept: Rep at v 0 and at vt respectively, CDt: drag coefficient at terminal velocity
20 AEROSOLS
where A p is the projected area of the particle on the flow (
pDp^2 /4), and C D is the drag coefficient of the particle. The
drag coefficient C D depends on the Reynolds number,
ReuDrpfrm/ (13)
where u r is the relative velocity between the particle and air
( | u v |, u velocity of air flow, v particle velocity),
and m is the viscosity of the fluid.
The motion of a particle having mass m p is expressed by
the equation of motion
m
p t
d
d
v
∑F (14)
where v is the velocity of the particle and F is the force acting
on the particle, such as gravity, drag force, or electrical force.
Table 3 shows the available drag coefficients depending on
C001_002_r03.indd 20C001_002_r03.indd 20 11/18/2005 10:09:10 AM11/18/2005 10:09:10 AM