05-Fluids - Andrews University
Download
Report
Transcript 05-Fluids - Andrews University
Physics
Unit 5
This Slideshow was developed to accompany the textbook
OpenStax Physics
Available for free at https://openstaxcollege.org/textbooks/collegephysics
By OpenStax College and Rice University
2013 edition
Some examples and diagrams are taken from the textbook.
Slides created by
Richard Wright, Andrews Academy
[email protected]
Phases of Matter
Solid
Atoms in close contact so they can’t
move much
Set volume and shape
Can’t compress
Liquid
Atoms move past each other
Set volume
Takes shape of container
Hard to compress
Gas
Atoms far apart
Neither set volume or shape
Compressible
Fluids
Flow
Both liquids and gases
Density
𝜌 =
𝑚
𝑉
Where
𝜌 = density
m = mass
V = Volume
Things with small density
float on things with more
density
Solids most dense
Gases least dense
See Table 11.1
Can use density to determine unknown material
An ornate silver crown is thought to be fake. How could we determine if
is silver without damaging the crown?
Find its mass using a balance. (It is 1.25 kg)
Find its volume by submerging in water and finding volume of displaces
water. (It is 1.60 × 10−4 m3)
Find the density
𝜌 = 7.81 × 103 kg/m3
Table 11.1 says it is steel
Silver’s density is 10.5 × 103 kg/m3
Don’t be dense, you can
solve these problems
11P1-7
Read 11.3, 11.4
11CQ8, 9, 11, 13, 14, 16, 17
Answers:
1) 1.610 cm3
2) 2.54 L
3) 2.58 g
4) 2.70 g/cm3
5) 3.99 cm
6) 0.163 m
7) 2.86 times denser
The molecules in a fluid are free to wander around
In their wanderings they sometimes collide with the
sides of their container (i.e. balloon)
The more the molecules collide with the walls, the more
force is felt
𝐹
𝑃=
𝐴
P = Pressure
F = Force perpendicular to surface
A = Area of surface
Unit: N/m2 = Pa (pascal)
1 Pa is very small so we usually use kPa or atm
In a fluid the pressure is exerted
perpendicularly to all surfaces
A static fluid cannot produce a
force parallel to a surface since it is
not moving parallel to surface
You are drinking a juice box. In the process you suck all the juice
and air out of the box. The top of the box is 7.5 cm by 5 cm. If the
air pressure is 1.013 × 105 Pa, how much force is acting on the top
of the box?
380 N = 85 lbs
Would the force of the side of the box be more or less than the
top?
More because more area
The force that squashes the juice box is from the weight
of all the air above it
Atmospheric Pressure at Sea Level
1.013 × 105 Pa = 1 atmosphere (1 atm)
The column of static fluid
experiences several
vertical forces
Since the fluid is not
moving, it is in
equilibrium and ∑𝐹 = 0
∑𝐹 = 𝑃2 𝐴 − 𝑃1 𝐴 − 𝑚𝑔 = 0
𝑃2 𝐴 = 𝑃1 𝐴 + 𝑚𝑔
𝜌=
𝑃2 𝐴 = 𝑃1 𝐴 + 𝜌𝑉𝑔
𝑉 = 𝐴ℎ
𝑃2 𝐴 = 𝑃1 𝐴 + 𝜌𝑔𝐴ℎ
𝑃2 = 𝑃1 + 𝜌𝑔ℎ
Or 𝑃 = 𝜌𝑔ℎ where P is the pressure due to the fluid at a depth h below the
surface
𝑚
𝑉
→ 𝑚 = 𝜌𝑉
If the pressure is known at a depth, the pressure lower
down can be found by adding ρgh
This assumes ρ is constant with depth
This is a good estimate for liquids, but not for gasses
unless h is small
Would Hoover Dam need to be just as strong if the entire
lake behind the dam was reduced to an inch of water
behind the dam, but the same depth as the lake?
Yes, the pressure depends only on the depth
What is the total pressure at points A and B?
1.55x105 Pa
Yes, there is a lot of pressure
riding on this assignment
11P11-17, 20, 22
Read 11.5, 11.6
11CQ24-27
Answers:
11) 3.59 × 106 Pa
12) 7.80 × 104 Pa
13) 2.36 × 103 N
14) 0.760 m
15) 1.10 × 108 Pa
16) Show work
17) 30.6 m
20) 1.09 × 103 Pa
22) 24.0 N
Pascal’s Principle
A change in pressure applied
to an enclosed fluid is
transmitted undiminished to
all portions of the fluid and
the walls of its container.
Basis of hydraulics
𝐹
Since 𝑃 = , if we change the
𝐴
area, the force is changed
How much force must be exerted at A to support the
850-kg car at B? The piston at A has a diameter of 17
mm and the piston at B a diameter of 300 mm.
F = 26.7 N
A
B
Gauge Pressure
Used by pressure gauges
Measures pressure relative to atmospheric pressure
Absolute Pressure
Sum of gauge pressure and atmospheric pressure
𝑃𝑎𝑏𝑠 = 𝑃𝑔𝑎𝑢𝑔𝑒 + 𝑃𝑎𝑡𝑚
Open-Tube Manometer
U-shaped tube with fluid in
it
One end is connected to the
container of which we want
to measure the pressure
The other end is open to the
air
𝑃2 = 𝑃𝑎𝑏𝑠
𝑃2 = 𝜌𝑔ℎ + 𝑃𝑎𝑡𝑚
𝑃2 − 𝑃𝑎𝑡𝑚 = 𝑃𝑔𝑎𝑢𝑔𝑒
Barometer
Used to measure air pressure
A tube with the top sealed and filled with
mercury
The bottom is open and sitting in a pool of
mercury
Pressure at top = 0
Pressure at bottom = 𝑃𝑎𝑡𝑚
𝑃 = 𝜌𝑔ℎ
Let me pressure you into
solving these problems
11P24-27, 30-34
Read 11.7
11CQ28-31
Answers:
24) 2.55 × 107 Pa, 251 atm
25) 136 N
26) 5.76 × 103 N
27) 100:1, 10:1, 1:100
30) 1.60 × 104 Pa, 1.07 × 104
Pa
31) 4.08 m
32) 1.49 × 106 N
33) 159 / 119
34) 3.99 × 104 N
Think of trying to push a beach ball under water
The water pushes it up
All fluids push things up because the pressure is higher at
greater depths
The upward force is buoyant force
𝐹𝐵 = 𝑃2 𝐴 − 𝑃1 𝐴
𝐹𝐵 = 𝑃2 − 𝑃1 𝐴
𝑃2 = 𝑃1 + 𝜌𝑔ℎ 𝑃2 − 𝑃1 = 𝜌𝑔ℎ
𝐹𝐵 = 𝜌𝑔ℎ 𝐴
𝜌=
𝑉 = 𝐴ℎ
𝑚 = 𝜌ℎ𝐴
𝑚
𝑉
𝑚 = 𝜌𝑉
𝐹𝐵 = 𝑚𝑔 = 𝑊𝑙𝑖𝑞𝑢𝑖𝑑
Archimedes’ Principle
Buoyant force = weight of the displaced fluid
𝐹𝐵 = 𝑊𝑓𝑙
If buoyant force ≥ gravity, then it floats
If buoyant force < gravity, then it sinks
An ice cube is floating in a glass of fresh water. The cube
is 3 cm on each side. If the cube is floating so a flat face
is facing up, what is the distance between the top of the
cube and the water?
h
0.002 m
x
As you might have guessed
An object will float if its average density < density of
the fluid
In other words, it will float if it displaces more fluid
than its own weight
Specific Gravity
𝑠𝑝𝑒𝑐𝑖𝑓𝑖𝑐 𝑔𝑟𝑎𝑣𝑖𝑡𝑦 =
𝜌
𝜌𝑓𝑙
= fraction submerged
If specific gravity < 1 it floats
If specific gravity > 1 it sinks
A man tied a bunch of helium balloons to a lawn chair and
flew to a great altitude. If a single balloon is estimated as a
sphere with a radius of 20 cm and is filled with helium, what
is the net force on one balloon?
0.3648 N
How many balloons would be required to lift a 80 kg man
and chair?
2150 balloons
Be buoyed up the thought of the
joy derived from solving these
problems
11P 37-42, 44, 51
Read 11.8, 11.9
11CQ33-38
Answers:
37) 800 kg/m3
38) 815 kg/m3
39) 99.5%, 96.9%
40) 41.4 g, 41.4 cm3, 1.09 g/cm3
41) 198 g, 198 cm3, 2.73 g/cm3
42) 39.5 g, 50 cm3, 0.79 g/cm3,
ethyl alcohol
44) 8.21 N
51) 2920 N
Cohesive Forces
Forces between
molecules of same type
Holding water together
in cup
Adhesive Forces
Forces between
molecules of different
type
Water drops sticking to
grass
Surface Tension
Cohesive forces at surface
of a liquid cause it to have
smallest surface area
possible
Why drops are round
Sort of like membrane on
top of fluid
Proportional to cohesive
force which varies by fluid
𝛾 =
𝐹
𝐿
𝛾 = surface tension
F = force
L = length on the
surface the force is
applied
Gauge pressure inside spherical bubble
Inward surface tension causes pressure inside a
bubble to be higher than atmospheric pressure
𝑃 =
4𝛾
𝑟
Interaction of cohesion and adhesion
A drop of water on a surface
Cohesion wants to make a spherical drop
Adhesion wants to spread out and stick to surface
Contact angle
Indicates which force is stronger
Capillary Action
Tendency of a fluid to be drawn
up a narrow, capillary, tube
If contact angle is < 90°, then
fluid raised up tube
As the fluid touches the sides of
tube, adhesive forces pull fluid
up, cohesive forces pull the
center up, but not as much
The curved part is called
meniscus
Height that capillary action
can lift fluid
ℎ =
2𝛾 cos 𝜃
𝜌𝑔𝑟
𝛾 = surface tension
𝜌 = density of fluid
𝑔 = acceleration of
gravity
𝑟 = radius of tube
Calculate the gauge pressure inside two soap bubbles
with radii of 3 cm and 1 cm.
3 cm: 4.93 Pa
1 cm: 14.8 Pa
That’s why it’s harder to blow up a small balloon than a
big balloon.
Stick with it, you can do well
11P54-59, 62-63, 68-69, 73-74, 77
Read 12.1, 12.2
12CQ1-5, 9-12, 14
Answers:
54) 592 N/m2
55) 0.0700 N/m, water at 40°C
56) 2.23 × 10−2 mmHg
57) 1.56 × 10−3 N
58) 1.65 × 10−3 m, 3.71 × 10−4 m
59) 0.566 m
62) 14.6 N/m2, 4.46 N/m2, 7.40
N/m2, Alcohol
63) -1.46 cm, 0 cm
68) 479 N
69) 5.00 × 108 Pa
73) 3.81 × 103 N/m2, 28.7 mmHg
74) 27.1 cm
77) 3.98 × 106 Pa, 2.1 × 10−3 cm
Flow Rate
𝑄 =
𝑉
𝑡
Q = Flow rate
V = Volume of fluid
t = time
𝑄=
𝑉
𝑡
=
𝐴𝑑
𝑡
= 𝐴𝑣
A = cross-section area
𝑣 = average velocity of fluid
Since flow rate is constant
for a given moving fluid
Equation of continuity
𝜌1 𝐴1 𝑣1 = 𝜌2 𝐴2 𝑣2
If incompressible
𝐴1 𝑣1 = 𝐴2 𝑣2
If incompressible and
several branches
𝑛1 𝐴1 𝑣1 = 𝑛2 𝐴2 𝑣2
Where does the water flow the fastest?
A
B
C
A garden hose has a diameter of 2 cm and water enters it
at 0.5 m/s. You block 90% of the end of the hose with
your thumb. How fast does the water exit the hose?
v = 5 m/s
When a fluid goes through narrower channel, it speeds
up
It increases kinetic energy
𝑊𝑛𝑒𝑡 =
1
𝑚𝑣 2
2
−
1
𝑚𝑣02
2
Net work comes from pressure pushing the fluid
Derivation
𝑊𝑛𝑒𝑡 = 𝐸𝑓 − 𝐸0
𝐸 = 𝐾𝐸 + 𝑃𝐸
1
= 𝑚𝑣 2 + 𝑚𝑔ℎ
2
𝑊𝑛𝑒𝑡 = 𝐹 ⋅ 𝑥
𝑃=
𝐹
𝐴
→ 𝐹 = 𝑃𝐴 → 𝐹𝑥 = 𝑃𝑉
𝑊𝑛𝑒𝑡 = 𝑃2 − 𝑃1 𝑉
𝑊𝑛𝑒𝑡 = 𝑃2 − 𝑃1 𝑉 =
1
𝑚𝑣12
2
Divide by V and rearrange
𝜌 =
+ 𝑚𝑔ℎ1 −
1
𝑚𝑣22
2
+ 𝑚𝑔ℎ2
𝑚
𝑉
Bernoulli’s Equation
1 2
1 2
𝑃1 + 𝜌𝑣1 + 𝜌𝑔ℎ1 = 𝑃2 + 𝜌𝑣2 + 𝜌𝑔ℎ2
2
2
Think about driving down a road with something in your car
trunk. The object is too large to completely shut the trunk lid.
While the car is stopped, the lid quietly rests as far down as it can
go. As you drive down the road, why does the trunk open?
The air in the trunk is still. The air above the trunk is moving.
The air in the trunk is at a higher pressure than above the trunk.
So the trunk is pushed open.
Demo:
Fold paper into a tunnel and blow through it.
What happens and why?
Why is an aneurysm (enlarged region of a blood vessel)
bad for you?
As the blood enters the enlarged region, it slows.
The slower blood has a higher pressure, and pop!
Why do all houses need a plumbing vent?
Waste water flows through a sewer line.
Something like a sink is connected to the line, but there is a water
trap to keep the sewer gasses from entering the house.
The flowing water in the sewer means the air directly above the
flowing water has a lower pressure than the air above the sink.
This pushes the water in the trap down the pipe and sewer gasses
enter the house
How do airplane wings work (even paper airplanes)?
The top of the wing is curved and the bottom is not. The air flows
faster over the top of the wing, than the bottom. This pushes the
wing up.
How does a curve ball in baseball work?
The faster you work, the less
pressure you’ll feel?
12P2-6, 8, 11, 20-23
Read 12.3
12CQ18-21
Answers:
2) 83.3 cm3/s, 8.33 × 10−5 m3/s
3) 27 cm/s
4) 5.03 cm3/s, 151 cm3
5) 0.75 m/s, 0.13 m/s
6) 0.139𝑣1
8) 0.166 cm/s
11) 12.6 m/s, 0.0800 m3/s
20) 33.1 m, 19.6 cm
21) 2.54 × 105 N
22) 15.3 N
23) 1.58 × 106 N/m2, 163 m
Previous examples of Bernoulli’s Equation had
simplified conditions
Bernoulli’s Equation work in real world
Water circulates throughout a house in a hot-water heating
system. If the water is pumped at a speed of 0.50 m/s
through a 4.0-cm-diameter pipe in the basement under a
pressure of 3.0 atm, what will be the flow speed and pressure
in a 2.6-cm-diameter pipe on the second floor 5.0 m above?
Assume the pipes do not divide into branches.
𝑣2 = 1.2
𝑚
𝑠
𝑃2 = 2.5 𝑎𝑡𝑚
The tank is open to the
atmosphere at the top.
Find an expression for the
speed of the liquid leaving
the pipe at the bottom.
𝑣1 =
2𝑔ℎ
Since Bernoulli’s
Equation is conservation
of energy, the water
would rise up to the same
height as the water in the
tank.
Power in Fluid Flow
Power is rate of work or
energy
Bernoulli’s Equation terms
are in energy per volume
Multiply Bernoulli’s
Equation by volume and
divide by time
Or multiply by flow rate
Q
𝑃𝑜𝑤𝑒𝑟 = 𝑃 +
1
𝜌𝑣 2
2
Apply yourself to these
applications
12P25-28
Read 12.4, 12.5
12CQ22-24, 26-28
Answers:
25) 9.56 × 108 W, 2.12
26) 71.8 m/s, 257 m/s
27) 1.26 W
28) 2.76 × 105 𝑃𝑎, 2.81 ×
105 𝑃𝑎
Viscosity
Fluid friction
Turbulent
Laminar Flow
Smooth flow in layers that
don’t mix
Turbulent Flow
Has eddies and swirls that
mix layers of fluid
Laminar
How viscosity is
measured
Two plates with fluid
between
Top plate moved
Friction causes the
fluid to move
𝜂 =
𝐹𝐿
𝑣𝐴
Laminar flow in tubes
Difference in pressure causes
fluids to flow
𝑃2 − 𝑃1
𝑄=
𝑅
Where
Q is flow rate
𝑃1 and 𝑃2 are pressures
R is resistance
Poiseuille’s law for resistance
8𝜂𝑙
𝑅= 4
𝜋𝑟
Where
𝜂 is viscosity
l is length of tube
r is radius of tube
Since flow rate depends
on pressure
If Q is high, the
pressure must
decrease like
Bernoulli’s equation
If R is high, the pressure
must decrease.
In blood vessels this is
a problem with plaque
on artery walls
How to tell if laminar or
turbulent flow
Low speed with smooth,
streamlined object
laminar
High speed or rough object
turbulent
Reynolds number
Below 2000 laminar
Above 3000 turbulent
Between 2000 and 3000
depends on conditions
2𝜌𝑣𝑟
𝑁𝑅 =
𝜂
A hypodermic syringe is filled
with a solution whose viscosity
is 1.5 × 10−3 Pa ⋅ s. The plunger
area of the syringe is 8.0
× 10−5 m2 , and the length of the
needle is 0.025 m. The internal
radius of the needle is 4.0
× 10−4 m. The gauge pressure in
a vein is 1900 Pa (14 mmHg).
What force must be applied to
the plunger, so that 1.0
× 10−6 m3 of solution can be
injected in 3.0 s?
𝐹 = 0.25 N
Is the flow laminar if the
density is 1000 kg/m3?
𝑁𝑅 = 4.44; Yes
Let the answers flow
12P30-33, 35-37, 51-54, 56
Read 12.6, 12.7
12CQ29-33
Answers:
30) 1.61 × 10−5 𝑁
31) 1.60 cm3/min
32) 0.0314 N, 0.471 mW
33) 8.7 × 10−2 𝑚𝑚3 /𝑠
35) 0.316𝑟1
36) 1.8𝑟1
37) 1.52, higher blood pressure
51) 1990
52) show work
53) 127000, 35100
54) 790000, 1690000
56) 3.16 × 10−4 𝑚3 /𝑠
If object move in fluid (or
fluid moves past object)
Alternate form of
Reynolds number
𝜌𝑣𝐿
′
𝑁𝑅 =
𝜂
𝑁𝑅′ < 1 laminar flow
1 < 𝑁𝑅′ < 10
transition, might have
turbulent wake
10 < 𝑁𝑅′ < 106 either
𝑁𝑅′ > 106 turbulent
Viscous drag
Force trying to stop
object in fluid
If 𝑁𝑅′ < 1, 𝐹𝑉 ∝ v
If 10 < 𝑁𝑅′ < 106 , 𝐹𝑉 ∝
𝑣2
Terminal velocity
Objects falling in fluid
Viscous drag will
increase as speed
increases
Eventually drag force
will = gravity force
No acceleration
Diffusion
Molecules in fluids move
randomly
They will travel some
distance and then hit
another molecule
Average distance
traveled
𝑥𝑟𝑚𝑠 = 2𝐷𝑡
How long will it take hemoglobin to move 1 mm in water
by free diffusion (𝐷 = 6.9 × 10−11 𝑚2 /𝑠)?
t = 7246 s = 2 h
Diffusion
Goes from high
concentration to low
Faster with higher
difference of
concentrations
Diffusion across
Membranes
Membranes are barriers
They are semipermeable
Some molecules can
cross, but others can’t
Osmosis
Transport of water through
membrane from differences in
concentration
Dialysis
Transport of other molecules
through membrane from
differences in concentration
Reverse osmosis/reverse dialysis
Sufficient pressure is applied to reverse normal
direction of substance through membrane
Can be used to purify a fluid
Water pushed through a membrane that won’t let
salt through
You cannot learn by
osmosis since knowledge is
not water, you must study
12P38-39, 62-64, 66
Answers:
38) 𝑣 =
2𝑅 2 𝑔 𝜌2 −𝜌1
9𝜂
39) 225 mPa⋅s
62) 1.41 mm
63) 130
64) 130 s
66) 0.391 s