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General Physics IGeneral Physics I
Lecture 16: Fluid MechanicsLecture 16: Fluid Mechanics
Prof. WAN, Xin (万歆)
[email protected]://zimp.zju.edu.cn/~xinwan/
MotivationsMotivations
Newton’s laws for fluid statics?– Force → pressure
– Mass → density
How to treat the flow of fluid?– Difficulties:
– Continuous medium– Change of the shape (still incompressible!)
– Frame of reference
DensityDensity
Density (scalar): mass of a small element of material m divided by its volume V
– For infinitesimally small V:
= m / V
– For homogeneous material:
= m / V
PressurePressure
Under static condition, force acts normal or perpendicular to the surface – vector.
Pressure: the magnitude of the normal force per unit surface area – scalar.
A
Δ A⃗
Δ F⃗
Δ F⃗ = pΔ A⃗
p =Δ FΔ A
Common UnitsCommon Units
2
5
5
2
1 1 / [SI]
1 1.01325 10
1 10 1
1 760 760
1 14.7 / .
pascal N m
atmosphere Pa
bar Pa atm
atm mm of Hg torr
atm lb in
Origin of PressureOrigin of Pressure
Microscopic origin: collisions of molecules of the fluid with the surface– Action and reaction: Newton’s third law
liquid
WallΔ v⃗
f⃗ reaction
Pressure in a Fluid at RestPressure in a Fluid at Rest
( ) ( )
( ) 0
dm g Ady g gAdy
pA gAdy p dp A
yy+dy
A
pA
(p+dp)A
(dm)g
dpg
dy
Pressure in a Fluid at RestPressure in a Fluid at Rest
Assumption: , g independent of y
0 0
0 0
0 0 0
' '
( )
( )
p y
p y
dpg dp g dy
dy
p p g y y
p p g y y p gh
Mercury BarometerMercury Barometer
How to measure atmospheric pressure? E. Torricelli (1608-47)
For mercury, h = 760 mm.
How high will water rise?
patm
p=0
atmatm
PP gh h
g
Vacuum!
h
U-Tube ManometerU-Tube Manometer
1 1 2 2A atmp gh p gh
SnorkelingSnorkeling
Can I use a longer snorkel to look closer at the underwater life?
Atmospheric PressureAtmospheric Pressure
Gases are compressible. Thus, varies!
50 sea level
0 0
00
1.013 10
, for constant
p p Pa
ppV nRT T
p
dp pg g
dx p
dy
0 0
0 0
00
0 0
00 0
0
( / )0
''
'
ln ln ( )
p y
p y
g p h
gdp p dpg dy
dx p p p
gp p y y
p
p p e
dy
Atmospheric PressureAtmospheric Pressure
00 0
h p p gh
A.P. – an Improved VersionA.P. – an Improved Version
0 0 0
0 0
00
0 0 0
( )
( )
pV nRT
p T
p T
T T y y
Tdp pg g
dy p T y y
Temperature decreases 6oC for each 1,000 meters of elevation
A.P. – an Improved VersionA.P. – an Improved Version
0 0
0
0 0
0 0
0 0 0
0 0
0 0 0
00
( )
' '
' ( ' )
1
p y
p y
gT p
g T dydp
p p T y y
g Tdp dy
p p T y y
hp p T
0
000
gh
pp e
Temperature CorrectionsTemperature Corrections
0 50 kmT
Pascal’s PrinciplePascal’s Principle
Pressure applied to an enclosed fluid is transmitted undimished to every portion of the fluid and to the walls of the containing vessel.
F
p
d
ext extp p gd p p
pext
Hydraulic LeverHydraulic Lever
/ / ,i i o o i i o oF A F A A d A d
Fi
mgAi Ao
Fo
di
do
Hydraulic BrakeHydraulic Brake
Fred Duesenberg originated hydraulic brakes on his 1914 racing cars and Duesenberg was the first automotive marque to use the technology on a passenger car in 1921. In 1918 Malcolm Lougheed (who later changed the spelling of his name to Lockheed) developed a hydraulic brake system.
Archimedes’ PrincipleArchimedes’ Principle
A body wholly or partially immersed in a fluid is buoyed up by a force equal in magnitude to the weight of the fluid displaced by the body.
FB
mg
B fluid fluid
object
F Vg m g
mg Vg
Two CommentsTwo Comments
Buoyant force volume/density
Center of buoyancy (not fixed)Center of gravity
B fluid fluid
object
F Vg m g
mg Vg
Question: Galileo’s ScaleQuestion: Galileo’s Scale
Can you invent a scale that one can use to read the percentage of silver in the gold crown without explicit calculations?
Fluid DynamicsFluid Dynamics
Aerodynamics (gases in motion) Hydrodynamics (liquids in motion)
– Blaise Pascal
– Daniel Bernoulli, Hydrodynamica (1738)
– Leonhard Euler
– Lagrange, d’Alembert, Laplace, von Helmholtz
Airplane, petroleum, weather, traffic
The Microscopic ApproachThe Microscopic Approach
N particles ri(t), vi(t); interaction V(ri-rj)
The Macroscopic ApproachThe Macroscopic Approach
A fluid is regarded as a continuous medium. Any small volume element in the fluid is always
supposed to be so large that it still contains a very large number of molecules.
When we speak of the displacement of fluid at a point, we meant not the displacement of an individual molecule, but that of a volume element containing many molecules, though still regarded as a point.
Euler’s SolutionEuler’s Solution
For fluid at a point at a time:
State of the fluid: described by parameters p, T.
However, laws of mechanics applied to particles, not to points in space.
Field
ρ(x , y , z ,t ), v⃗ (x , y , z ,t )
Ideal FluidsIdeal Fluids
Steady: velocity, density and pressure not change in time; no turbulence
Incompressible: constant density Nonviscous: no internal friction
between adjacent layers Irrotational: no particle rotation
about the center of mass
StreamlinesStreamlines
Paths of particles
P → Q → R v tangent to the streamline No crossing of streamlines
Pv Rv
Qv
PQ
R
Mass FluxMass Flux
Tube of flow: bundle of streamlines
2v
A1 A2
1vP
Q
11 1 1 1 1 1 1
1
mass flux m
m A v t A vt
Conservation of MassConservation of Mass
IF: no sources and no sinks/drains
– Narrower tube == larger speed, fast
– Wider tube == smaller speed, slow
Example of equation of continuity. Also conservation of charge in E&M
1 1 1 2 2 2
1 1 2 2
constant
co fornstant incompressible fluid,
A v A v
A v A v
What Accelerates the Fluid?What Accelerates the Fluid?
Acceleration due to pressure difference.Bernoulli’s Principle = Work-Energy Theorem
Work-Energy TheoremWork-Energy Theorem
Steady, incompressible, nonviscous, irrotational
Bernoulli’s EquationBernoulli’s Equation
1 1 2 2
2 21 1 1 2 2 2 2 2 1 1
2 21 1 1 2 2 2
2
1 1
2 21 1
2 21
constant2
m A x A x
p A x p A x mv mgy mv mgy
p v gy p v gy
p v gy
kinetic E, potential E, external work
CommentsComments
Restrictions of the Bernoulli’s equation:– Points 1 and 2 lie on the same streamline.
– The fluid has constant density.
– The flow is steady.
– There is no friction.
When streamlines are parallel the pressure is constant across them (if we ignore gravity and assume velocity is constant over the cross-section).
The Venturi MeterThe Venturi Meter
Speed changes as diameter changes. Can be used to measure the speed of the fluid flow.
2 21 1 2 2 1 1 2 2
1 1,
2 2p v p v v A v A
Bend it like BeckhamBend it like Beckham
Dynamic lift
http://www.tudou.com/programs/view/qLaZ-A0Pk_g/
Banana Free KickBanana Free Kick
~ 5mDistance 25 mInitial v = 25 m/sFlight time 1sSpin at 10 rev/sLift force ~ 4 NBall mass ~ 400 g a = 10 m/s2 A swing of 5 m!