© 2006 baylor university slide 1 introduction to fluid mechanics bellagio fountain
TRANSCRIPT
Slide 2© 2006 Baylor University
Lecture 8Introduction to Fluid Mechanics
Approximate Running Time - 21 minutesDistance Learning / Online Instructional Presentation
Presented byDepartment of Mechanical Engineering
Baylor University
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Slide 3© 2006 Baylor University
Dr. Carolyn SkurlaSpeaking
•Outline– Measuring Devices for
Measuring Drag
– Basics of Fluid Mechanics
– Flight Characteristics of Baseballs & Golf Balls
Lecture 8 Topics
Slide 4© 2006 Baylor University
Lab: Drag Force Experiment
• Performing a fluid mechanics experiment– Collect experimental data
– Perform integration of experimental data
• Equipment:– Wind tunnel
– Cylinder
– Pressure
transducer
– Pitot-static
tube
Slide 5© 2006 Baylor University
So, What is Fluid Mechanics?
• The study of fluids in motion– Solid -> Can resist a shear stress by a static deformation
– Fluid -> Cannot resist a shear stress• Any shear stress applied to a fluid will result in motion of that fluid
• There are two classes of fluids:– Liquids
– Gases
(White, 1994)
Slide 6© 2006 Baylor University
Thermodynamic Properties of a Fluid
• Pressure, p
– Compression stress at a point in a fluid
– Differences, or gradients, of pressure often drive
a fluid flow
• Temperature, T
– Measure of internal energy level of a fluid
Slide 7© 2006 Baylor University
Thermodynamic Properties of a Fluid
• Density,
– Mass per unit volume
• Highly variable in gases (i.e., =f(p))
• Nearly constant in liquids
– Almost incompressible
– Assumed to be imcompressible to make
analysis easier
• Specific Weight,
– Weight per unit volume
g
2322 s
m
m
kg
sm
kg
Slide 8© 2006 Baylor University
Pressure Transducer: Manometer
• How do we measure pressure, p ?– Change in elevation of a liquid is equivalent to a change in
pressure• Therefore, a static column of liquid can be used to measure pressure
difference between 2 points
(White, 1994)
)( 2112 zzpp
Slide 9© 2006 Baylor University
Pressure Transducer: Manometer
• Manometer units are in·H2O
– How do I convert in·H2O to more standard units for pressure?
2
2
22
11
)(11
036126.0)(09.2491
s
mkg N
m
NewtonN Pa
in
lb PascalPa OHin
SI Units English
Slide 10© 2006 Baylor University
Pressure – Velocity Relationship
t
v
dt
dva
x
y
maF ds
A1 2
v = Flow velocity
ApF11
ApF22
21FFF
net
AvdtAdsm
Slide 11© 2006 Baylor University
Pressure – Velocity Relationship
ds
A1 2
v = Flow velocity
dt
dvmApAp
21
dt
dvAvdtApp )(
21
dvvppV
V
2
1
)(21
22)(
2
1
2
2
21
VVpp
Slide 12© 2006 Baylor University
Pitot-Static Tube
Stagnation Point
Stagnation Velocity, (v0)
Stagnation Pressure, (p0 )
0p
00v
Static Point
Static Velocity, (vS)
Static Pressure, (pS )
Sp
sv
Differential Pressure Transducer (Manometer)
Slide 13© 2006 Baylor University
Pitot-Static Tubes
• ps = Static pressure (in the moving stream)
– Nominal air pressure in atmosphere
• p0 = Stagnation pressure
– Air pressure in the pitot tube
• vs = Static velocity
– Speed of air passing the pitot tube • Equivalent to speed of plane through the
air
• v0 = Stagnation velocity = 0
2
1
0 )(2
s
s
ppv
Slide 14© 2006 Baylor University
2
1
2
32.1
)9.298(2
Pasm
kg
mkg
Pav
s
2
Pitot-Static Tube Sample Problem
:Given
OHinR2
2.1'
Sv
Find :
OHin
PaOHinpp
S
2
20 1
09.2492.1
PappS
9.2980
:Solution
s
m
s
mv
s3.222.498
2
1
2
2
32.1
m
kgair
Slide 15© 2006 Baylor University
Velocity
• When there is friction between the
fluid and the solid surface
– No slip of the fluid at the
boundary
• Velocity = 0
– A boundary layer forms near the
solid surface
• Shear stress is greatest adjacent
to the boundary layer at the
surface
(White, 1994)
Slide 16© 2006 Baylor University
Laminar vs. Turbulent Flow
• Laminar -> smooth and steady.
• Turbulent -> fluctuating and agitated.
Slide 17© 2006 Baylor University
Reynolds Number
• Dimensionless parameter
– Correlates viscous behavior of all newtonian fluids
= density
= viscosity
– V = characteristic velocity of flow
– L = length scale of flow
• Most important parameter in fluid mechanics
– Governs transition from laminar to turbulent flow
VL
Re