Title: Introduction To Fluids Fluids Fluids are substances that can
1Introduction To
2Fluids
- Fluids are substances that can flow.
- Fluids are liquids and gases, and even some
solids. - In Physics B, we will limit our discussion of
fluids to substances that can easily flow, such
as liquids and gases.
3Density
- ? m/V
- ? density (kg/m3)
- m mass (kg)
- V volume (m3)
- Units
- kg/m3
4Sample Problem
- Given that water has a density of 1,000 kg/m3,
calculate the mass of a barrel full of water.
Assume that the barrel has a diameter of 1.0 m
and a height of 1.5 m.
5Sample Problem
- Given that water has a density of 1,000 kg/m3,
calculate the mass of a barrel full of water.
Assume that the barrel has a diameter of 1.0 m
and a height of 1.5 m.
6Sample Problem
- Given that water has a density of 1,000 kg/m3,
calculate the mass of a barrel full of water.
Assume that the barrel has a diameter of 1.0 m
and a height of 1.5 m.
7Sample Problem
- Given that water has a density of 1,000 kg/m3,
calculate the mass of a barrel full of water.
Assume that the barrel has a diameter of 1.0 m
and a height of 1.5 m.
8Pressure
- P F/A
- P pressure (Pa)
- F force (N)
- A area (m2)
- Pressure unit Pascal
- 1 Pa N/m2
- Atmospheric pressure is about 101,000 Pa
9Sample Problem
- Calculate the net force on an airplane window if
cabin pressure is 90 of the pressure at sea
level, and the external pressure is only 50 of
that at sea level. Assume the window is 0.43 m
tall and 0.30 m wide.
10Sample Problem
- Calculate the net force on an airplane window if
cabin pressure is 90 of the pressure at sea
level, and the external pressure is only 50 of
that at sea level. Assume the window is 0.43 m
tall and 0.30 m wide.
11Sample Problem
- Calculate the net force on an airplane window if
cabin pressure is 90 of the pressure at sea
level, and the external pressure is only 50 of
that at sea level. Assume the window is 0.43 m
tall and 0.30 m wide.
12Sample Problem
- Calculate the net force on an airplane window if
cabin pressure is 90 of the pressure at sea
level, and the external pressure is only 50 of
that at sea level. Assume the window is 0.43 m
tall and 0.30 m wide.
13Pressure
- The force on a surface caused by pressure is
always normal to the surface. - The pressure of a fluid is exerted in all
directions, and is perpendicular to the surface
at every location.
balloon
14The Pressure of a Liquid
- P ?gh
- P pressure (Pa)
- ? density (kg/m3)
- g acceleration constant (9.8 m/s2)
- h height of liquid column (m)
15Absolute Pressure
- P Po ?gh
- p pressure (Pa)
- po atmospheric pressure (Pa)
- ?gh liquid pressure (Pa)
- Po is atmospheric pressure.
- P is commonly referred to as absolute pressure,
and includes atmospheric pressure.
16Gauge Pressure
- Gauge pressure is due to a fluid contained in a
container and excludes atmospheric pressure.
17Sample Problem
- Calculate the pressure at the bottom of a 3 meter
(approx 10 feet) deep swimming pool (a) due to
the water and (b) due to the water plus the
atmosphere.
18Sample Problem
- Calculate the pressure at the bottom of a 3 meter
(approx 10 feet) deep swimming pool (a) due to
the water and (b) due to the water plus the
atmosphere.
19Sample Problem
- Calculate the pressure at the bottom of a 3 meter
(approx 10 feet) deep swimming pool (a) due to
the water and (b) due to the water plus the
atmosphere.
20Sample Problem
Area of piston 8 cm2 Weight of piston 200 N
25 cm
A
- What is the absolute pressure at point A?
21Sample Problem
Area of piston 8 cm2 Weight of piston 200 N
25 cm
A
- What is the absolute pressure at point A?
22Sample Problem
Area of piston 8 cm2 Weight of piston 200 N
25 cm
A
- What is the absolute pressure at point A?
23Sample Problem
Area of piston 8 cm2 Weight of piston 200 N
25 cm
A
- What is the absolute pressure at point A?
24Sample Problem
Area of piston 8 cm2 Weight of piston 200 N
25 cm
A
- What is the absolute pressure at point A?
25Floating is a type of equilibrium
26Floating is a type of equilibrium
- Archimedes Principle a body immersed in a
fluid is buoyed up by a force that is equal to
the weight of the fluid displaced. - Buoyant Force the upward force exerted on a
submerged or partially submerged body.
27Calculating Buoyant Force
- Fbuoy ?Vg
- Fbuoy the buoyant force exerted on a submerged
or partially submerged object. - V the volume of displaced liquid.
- ? the density of the displaced liquid.
- Buoyant force is enough to float iron ships,
automobiles, and brick houses!
28Parking in St. Bernard Parish after Hurricane
Katrina
29Parking in St. Bernard Parish after Hurricane
Katrina
30Parking in St. Bernard Parish after Hurricane
Katrina
31Mobile Homes in St. Bernard Parish after
Hurricane Katrina
32Mobile Homes in St. Bernard Parish after
Hurricane Katrina
33Buoyant force on submerged object
Note if Fbuoy lt mg, the object will sink deeper!
34Buoyant force on submerged object
SCUBA divers use a buoyancy control system to
maintain neutral buoyancy (equilibrium!)
35Buoyant force on floating object
If the object floats, we know for a fact Fbuoy
mg!
36Sample problem
- Assume a wooden raft has 80.0 of the density of
water. The dimensions of the raft are 6.0 meters
long by 3.0 meters wide by 0.10 meter tall. How
much of the raft rises above the level of the
water when it floats?
37Sample problem
- Assume a wooden raft has 80.0 of the density of
water. The dimensions of the raft are 6.0 meters
long by 3.0 meters wide by 0.10 meter tall. How
much of the raft rises above the level of the
water when it floats?
38Sample problem
- Assume a wooden raft has 80.0 of the density of
water. The dimensions of the raft are 6.0 meters
long by 3.0 meters wide by 0.10 meter tall. How
much of the raft rises above the level of the
water when it floats?
39Sample problem
- Assume a wooden raft has 80.0 of the density of
water. The dimensions of the raft are 6.0 meters
long by 3.0 meters wide by 0.10 meter tall. How
much of the raft rises above the level of the
water when it floats?
40Buoyancy Lab
- Using the equipment provided, verify that the
density of water is 1,000 kg/m3. - Report (due Tuesday) must include
- Free body diagrams.
- All data.
- Calculations.
water
air
41Reading a Venier Caliper
42Reading a Venier Caliper
43Reading a Venier Caliper
44Reading a Venier Caliper
45Sample problem
- You want to transport a man and a horse across a
still lake on a wooden raft. The mass of the
horse is 700 kg, and the mass of the man is 75.0
kg. What must be the minimum volume of the raft,
assuming that the density of the wood is 80 of
the density of the water.
46Fluid Flow Continuity
- Conservation of Mass results in continuity of
fluid flow. - The volume per unit time of water flowing in a
pipe is constant throughout the pipe.
47Fluid Flow Continuity
- A1v1 A2v2
- A1, A2 cross sectional areas at points 1 and 2
- v1, v2 speed of fluid flow at points 1 and 2
48Fluid Flow Continuity
- V Avt
- V volume of fluid (m3)
- A cross sectional areas at a point in the pipe
(m2) - v speed of fluid flow at a point in the pipe
(m/s) - t time (s)
49Sample problem
- A pipe of diameter 6.0 cm has fluid flowing
through it at 1.6 m/s. How fast is the fluid
flowing in an area of the pipe in which the
diameter is 3.0 cm?
50Sample problem
- Suppose the current in a river is moving at 0.20
meters per second where the river is 12 meters
deep and 10 meters across. If the depth of the
river is reduced to 1.5 meters at an area where
the channel narrows to 5.0 meters, how fast will
the water be moving through this narrow region?
51Sample problem
- How much water per second is flowing in the river
described in the previous problem?
52Bernoullis Theorem
- The sum of the pressure, the potential energy per
unit volume, and the kinetic energy per unit
volume at any one location in the fluid is equal
to the sum of the pressure, the potential energy
per unit volume, and the kinetic energy per unit
volume at any other location in the fluid for a
non-viscous incompressible fluid in streamline
flow. - All other considerations being equal, when fluid
moves faster, the pressure drops.
53Bernoullis Theorem
- P ? g h ½ ?v2 Constant
- P pressure (Pa)
- ? density of fluid (kg/m3)
- g gravitational acceleration constant (9.8 m/s2)
- h height above lowest point (m)
- v speed of fluid flow at a point in the pipe
(m/s)
54Sample Problem
- Knowing what you know about Bernouillis
principle, design an airplane wing that you think
will keep an airplane aloft. Draw a cross section
of the wing.
55Announcements 5/24/2013
- 6th period only pass photoelectric redo forward
if I didnt get it yesterday. - Buoyancy lab is due today. Put in folders.
- Fluid dynamics project you do today is due
tomorrow, so work efficiently.
56URLs of interest
- Katrina and the Mississippi River Gulf Outlet
- http//www.mvn.usace.army.mil/ChannelSurveys/surve
y.asp?prj_id15 - http//en.wikipedia.org/wiki/Mississippi_River_Gul
f_Outlet - http//www.cclockwood.com/stockimages/hurricanekat
rina_MississippiGulfOutlet.htm - http//www.washingtonpost.com/wp-dyn/content/artic
le/2005/09/13/AR2005091302196.html - http//www.saveourwetlands.org/mrgohastogo.html
57URLs of interest
- Hurricanes - classification
- http//www.ohsep.louisiana.gov/hurricanerelated/HU
RRICANECATEGORIES.htm - http//www.nhc.noaa.gov/aboutsshs.shtml
- Hurricanes - behavior
- http//ww2010.atmos.uiuc.edu/(Gh)/guides/mtr/hurr/
home.rxml - http//science.howstuffworks.com/hurricane.htm
58(No Transcript)