1 class #4 retarding forces stokes law (viscous drag) 2-d motions with viscous drag newton’s law...
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1
Class #4
Retarding forces Stokes Law (viscous drag) 2-D motions with viscous drag Newton’s Law (inertial drag) Reynolds number Plausibility of Stokes law Plausibility of Newton’s Law Projectile motions with inertial drag
Worked Problems
:10
2
2-D Motion with viscosity
0
ˆ / :
1( ) ( )
:
(1 exp( )) exp( )
( )
z z z z Term
y Term y
xx x x
mmr mgz br Viscous drag w gravity
b
mv mg bv v v v z component
Solution from last timet tv v v
Now solve the x component which is even simpler than zv
mv bv v
0
'
'
0
0
ln( ) ln( )
exp( )
x
x
vx
vx
x x
x x
dv dt
vt
v v
tv v
dragF
gm
z
x :60
3
Velocity Dependent Force
Forces are generally dependent on velocity and time as well as position
Fluid drag force can be approximated with a linear and a quadratic term
= Linear drag factor(Stokes Law, Viscous or “skin” drag)
= Quadratic drag factor( Newton’s Law, Inertial or “form” drag)
2)( rcrbrFr
),,( trrFF
b
c
:15
quad
lin
fRatio
f
is important
4
The Reynolds Number
R < 10 – Linear drag1000< R < 300,000 –
Quadratic R > 300,000 – Turbulent
( )
( )
inertial quad dragR
viscous linear drag
density
viscosity
D
v
Dv
R
:20
5
Reynolds Number Regimes
R < 10 – Linear drag1000< R < 300,000 –
Quadratic R > 300,000 – Turbulent
6
The Reynolds Number II
DR OR
DR where
v
v
v
v
:20
2
2
163
163
inertial
viscous
inertial
viscous
F D
F D
DF DK K R
F D
2
2
v
v
v v
v
vD
density
viscosity
“D”= “characteristic” length
( )
( )
inertial quad dragR
viscous linear drag
7
The Reynolds Number III
R < 10 – Linear drag1000< R < 300,000 –
Quadratic R > 300,000 – Turbulent
1 22
1 222
1 22
1 22
1(1 / #)
R
dD
Linear Regime
D
Quadratic Regime
D
FC
v A
kD v DC
vDv A
Reynolds
kA vC k
v A
D
v
Dv
R
8
Inertial Drag I
Plate with area “An” moves a distance through fluid with density
The mass of the fluid displaced is Mass “M” must acquire a velocity “v” to move
out of the way of the plate.The moving plate is causingRearranging we get
tv An
tv M Av t
( )p Mv Av t v 2p
Avt
2
2
vAkF
rcF
ndrag
drag
:35
9
Inertial Drag II – A sphere
2vAkF ndrag
Previously demonstrated
“An” means “A normal to velocity”
Form factor for sphere
Plug ‘n’ play
2
4
1DAn
vvDFdrag ˆ16
22
4
1k
:40
10
Falling raindrops redux II
1) Newton
2) On z-axis
3) Rewrite in terms of v
4) Rearrange terms
5) Separate variables
2
2
2
2
2
2
2
ˆ
Assume vertical motion
(1 )
(1 )
zz
z z
z
z
mr mgz cr
mz mg cz
dv cg v
dt m
dv vmgDefine v g
c dt v
dvg dt
v
v
dragF
gm
z
x
:45
2
16c D
11
Falling raindrops redux III
2
2(1 )
z
z
dvg dt
v
v
( )
20 0
2(1 )
v t tz
z
t
dvg dt gt
vv
( ) /
20arctanh( ( ) / )
(1 )
( ) tanh( / )
zz
v t v
vu dv v du
v
v duv v t v gt
u
v t v gt v
2arctanh( )
(1 )
dxx
x
:50
12
0 50 100 150 200 250 300 3500
0.5
1
1.5
2
2.5
3
3.5
4
4.5
5
x [degrees]
f(x)
sin, sinh and tanh
sin(x)sinh(x)tanh(x)
Tanh and sinh and cosh
cos2
sin2
tan
cosh2
tanh
ix ix
ix ix
ix ix
ix ix
x x
x x
x x
e ex
e ex
i
e ex
e e
e ex
e ex
e e
:55
sin( )x
sinh( )x
tanh( )x
13
Falling raindrops L4-1
A small raindrop falls through a cloud. It has a 1 mm radius. The density of water is 1 g/cc. The viscosity of air is 180 Poise. The density of air is 1.3 g/liter at STP.
a) What is the Reynolds number of this raindrop? (assume 10 m/s fall velocity)
b) Based on “a”, which type of drag should be more important?
c) What should be the terminal velocity of the raindrop, using quadratic drag?
d) What should be the terminal velocity of the raindrop, using linear drag?
e) Which of the previous of two answers should we use and why?
:70
14
Falling raindrops L4-2
A small raindrop is given an initial horizontal velocity of
and subsequently falls through a cloud. It has a 10 m radius. The density of water is 1 g/cc. The viscosity of air is 180 Poise.
a) Quantify the viscous force on the drop for a velocity of 10 mm/sec as well as the inertial force.
b) Should this drop be analyzed with linear or quadratic drag?
c) What is the Reynolds number of this raindrop?d) Write a formula for the position vector of the
raindrop as a function of time (set the origin to zero at point where it is released)
:50
20 /ˆ3 smxv
15
Pool Ball L4-3
A pool ball 6 cm in diameter falls through a graduated cylinder. The density of the pool ball is 1.57 g/cc. The viscosity of water is approximately 1 CentiPoise.
a) Quantify the force on the ball for a velocity of 100 mm/sec.
b) What should be the terminal velocity of the ball?
c) Quantify the force if we assume quadratic drag
:50
2 2
16dragF D v
16
Lecture #4 Wind-up
.
:72
1gt
vzv v e
vvDFdrag ˆ
1622
Linear Drag (Sphere)
Quadratic Drag (Sphere)
xuDFdrag ˆ3
( ) tanh( / )v t v gt v
2
mg bv
mg cv