Title: Lec 4: Fluid statics, buoyancy and stability, pressure
1Lec 4 Fluid statics, buoyancy and stability,
pressure
2- For next time
- Read 3-1 to 3-4
- HW 2
- Outline
- Zeroth law of thermodynamics
- Pressure and resulting forces
- Buoyancy and stability
- Important points
- How to calculate pressure force
- How to calculate application point of pressure
force - How to analyze stability
3Fluid statics
- Fluid statics deals with non-flow
situations--fluids at rest. - It is particularly applicable with pressure
measurements in terms of fluid column heights.
4TEAMPLAY
- You accidentally drive your car into a lake and
it submerges but does not admit a significant
amount of water into the passenger compartment. - A. Can you open a door?
- B. How will you get out?
5Fluid statics
- The car door may be regarded as a plane surface
of area about 10 square feet. - In order to study the force on the submerged car
door resisting attempts to open it, we must delve
into - Force magnitude
- Force application point, known as center of
pressure.
6Fluid statics
- Consider the effect of a constant pressure at the
top of the liquid. This could be Patm or some
other pressure P0. - We can neglect P0 as long as it acts on both
sides.
7Fluid statics
- Consider an arbitrary flat shape and orientation
The pressure at any point on the shape
8Fluid statics
- The resultant force FR is given by
9Fluid statics
- The integral is related to the y coordinate of
the centroid (center)
10TEAMPLAY
- Your pickup, named Bigfoot, has a door which is 4
ft high by 3.5 ft wide and all windows are stuck
in the closed position. The bottom of the door
is 4 ft off the ground. You accidentally drive
into a stock tank where it comes to rest on its
wheels in water 10 ft deep. Assume the bottom of
the stock tank is flat. What is the force on the
door? Can you open it?
11Fluid statics
- Now that we know the resultant force on a
submerged plane body is - where yc is the y-coordinate of the centroid.
- it is necessary to know where the center of
pressure is, that is, the point through which it
acts.
12Fluid statics
- In general the location yP of the center of
pressure isbelow the location of the centroid
yC because the pressure increases with depth.
13Fluid statics
- Equate the moment of the resultant force FR to
the moment of the distributed pressure force
about the x-axis. - Where is the second moment
of area (area moment of inertia).
14Fluid statics
- Most area moments of inertia are given about the
centroid of the shape (IXX,C). - They are relate to the moment IXX,0 about the
x-axis by - Area moments of inertia about the centroid are in
Fig. 10-5 for some common shapes. Centroids are
also given there.
15TEAMPLAY
16Buoyancy
- A buoyant force FB is caused by increasing
pressure with depth, so
17Buoyancy
- The upward force from the bottom is obviously
greater, and so the net buoyancy force is - where is the density of the fluid, not the
body, and V is the volume of the body.
18TEAMPLAY
- The previous equation does not depend on the
density of the submerged body. - What changes about a submarine as it goes up and
down (with zero propulsive thrust)? - What is the upward force on a submarine as it
holds a constant depth? - Does this force change as it changes depth (with
zero thrust)?
19Buoyancy and stability
- The buoyant force for a constant volume system is
equal to the weight W of the displaced fluid.
20Buoyancy
- The gravity force downward on a submerged body
acts through the centroid. - Similarly, the buoyant force upward must act
through the centroid or there would be a rolling
moment. - Thus, we have Archimedes Principle
- The buoyant force acting on a body immersed in a
fluid is equal to the weight of the fluid
displaced by the body, and it acts upward through
the centroid of the displaced volume.
21Buoyancy
- For floating bodies, the buoyant force is given
by the weight of the displaced fluid, or
22Stability
- Immersed bodies must be bottom-heavy to be
stable. Thus the center of gravity G must below
the center of buoyancy B so that any disturbance
will provide a restoring moment about G.
23Stability
- Model a submarine as a horizontal tube with the
top half empty and the bottom half filled with
engines, crew quarters, and weaponry. Neglect
the mass of the shell (tube). Where is the
center of gravity G? Where is the center of
buoyancy B? Do the two forces act to restore the
sub to an upright condition if it starts to roll,
or increase its rolling tendency?
24Stability
- Rotational stability criteria are similar for
floating bodies. - However, if the center of buoyancy shifts during
rolling motion, it may be possible to have the
center of gravity G above the center of buoyancy
and still achieve stability.
25Stability
- The metacenter M is required to be above G. The
metacenter height is the vertical distance
between G and M. - For many hull shapes the metacenter is almost a
fixed point for rolling angles up to about 20.
26Pressure
- The normal force exerted on a (small) area.
Small enough that changes over the area are
unimportant, and large enough that molecular
effects also are unimportant.
27Pressures
- For pressures above atmospheric
- For pressures below atmospheric
P1
P1
Pgage
Patm
Patm
Pvac
P2
Pabsolute
Pabsolute
P0
P0
28In the SI system we use
- 1 Pa 1 N/m2
- 1 kPa 1,000 N/m2
- 1 bar 100,000 N/m2
- 1 MPa 1,000,000 N/m2
29In the USCS system we use
- lbf/in2 or psi
- psi is usually written with an asuffix (psia)
or a g suffix, for absolute or gage (psig)
30Atmospheric pressure is
1 atm 14.696 psia 101.325 kPa 1.01
bar 0 psig 14.696 psia
Absolute pressure (Pabs) gage pressure (psig)
atmospheric pressure (Patm)
31For example
A gage pressure of 20.0 psig is an absolute
pressure at standard sea level conditions of
Pabs Patm Pg 14.7 psia 20.0 psig
34.7 psia
32TEAMPLAY
- Consider the bicycle tire, which produces a
pressure reading of 30 psig. What is the
absolute pressure at sea level and at 10,000 ft
altitude where Patm 10 psia?
33Pressure Measurement
34TEAMPLAY
What pressure (above atmospheric) is exerted on
your ears at the bottom of a 12 foot deep
swimming pool?
Assume the density of water is 62.4 lbm/ft3