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2/27/2012 1 Fluids and Elasticity Chapter 15 Density ( ) = mass/volume Rho ( ) Greek letter for density Units - kg/m 3 Specific Gravity = Density of substance Density of water (4 o C) Unitless ratio Ex: Lead has a sp. Gravity of 11.3 (11.3 times denser than water Ex: 1 Estimate the mass of air in this classroom Pressure Force per unit area P = F/A Unit - N/m 2 (Pascal) The larger the area, the less the pressure Shoeshoes Elephant feet Bed of nails Fluid Pressure A fluid exerts the same pressure in all directions at a given depth P = P o + gh The atmosphere is a fluid Po often 1 atm (101.3 kPa)
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  • 2/27/2012

    1

    Fluids and Elasticity

    Chapter 15

    Density ( )

    = mass/volume

    Rho ( ) Greek letter for density

    Units - kg/m3

    Specific Gravity = Density of substance

    Density of water (4oC)

    Unitless ratio

    Ex: Lead has a sp. Gravity of 11.3 (11.3 times

    denser than water

    Ex: 1

    Estimate the mass of air in this classroom

    Pressure

    Force per unit area

    P = F/A

    Unit - N/m2 (Pascal)

    The larger the area, the less the pressure

    Shoeshoes

    Elephant feet

    Bed of nails

    Fluid Pressure

    A fluid exerts the same pressure in all directions

    at a given depth

    P = Po + gh

    The atmosphere is a fluid

    Po often 1 atm (101.3 kPa)

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    2

    Pressure: Example 1

    A water storage tank is 30 m above the water faucet

    in a house. Calculate the pressure at the faucet:

    We will neglect the atmospheric pressure since it is

    the same at the tank and at the surface

    P = gh = (1000 kg/m3)(9.8 m/s2)(30 m)

    P = 29,000 kgm2/m3s2 = 29,000 kg m/s2m2

    P = 29,000 N/m2

    Pressure: Example 2 The Kraken can live at a depth of 200 m. Calculate

    the pressure the creature can withstand (neglect

    atmospheric pressure)

    Pressure: Example 2

    P = gh = (1000 kg/m3)(g)(200 m)

    P = 1.96 X 106 N/m2

    Atmospheric Pressure

    1 atm = 1.013 X 105 N/m2 = 101.3 kPa

    1 bar = 1 X 105 N/m2 (used by meteorologists)

    Gauge pressure

    P = Patm + PG

    Absolute pressure atmospheric pressure Gauge pressure

    We usually measure gauge pressure

    Ex: A tire gauge reads 220 kPa, what is the

    absolute pressure?

    P = Patm + PG

    P = 101.3 kPa + 220 kPa = 321 ka

    Straw Example

    You can pick up soda in a

    straw using your finger. Why

    doesnt the soda fall out?

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    3

    Another Straw Example

    What pushes soda up a straw when you drink

    through it?

    Torrecillis Work

    P = Patm + PG

    P = Patm + gh

    What is the highest column of water

    that the atmosphere can support?

    P = Patm + gh

    0 = 1.013 X 105 N/m2 + (1000kg/m3)(9.8m/s2)(h)

    h = 10.3 m

    No vacuum pump can pump more than ~30 feet

    Try the same calculation with mercury

    P = Patm + gh

    0 = 1.013 X 105 N/m2 + (13,600kg/m3)(9.8m/s2)(h)

    h = 0.760 m (760 mm)

    1 atm = 760 mm Hg (760 torr)

    Can an astronaut attach suction cups to the boots of

    his spacesuit to help him climb around the space

    shuttle while in space?

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    4

    Pascals Principle

    Pressure applied to a confined fluid increases the

    pressure the same throughout

    Pin = Pout

    Fin = Fout

    Ain Aout

    for pistons:

    F = g(A1 + A2)d2

    Pascals Principle: Ex 1

    A hydraulic lift can produce 200 lb of force. How

    heavy a car can be lifted if the area of the lift is

    20 times larger that the input of the Force?

    Fin = Fout

    Ain Aout

    Fout = Fin Aout = (200 lb) (20) = 4000 lbs

    Ain 1

    Pascals Principle: Ex 1

    A hydraulic lift has the car rest ona 25 cm pipe.

    The lift the car, compressed air pushes on a 6.0

    cm pipe.

    a. Calculate the force needed to lift a 1300 kg car.

    b. Calculate how much the air pressure force must

    be increased to lift the car 2.0 m.

    Buoyancy

    Buoyancy

    The lift provided by water

    Objects weight less in water than out

    Caused by pressure differential between top and

    bottom of an object.

    Fbouyant = gV

    Derivation of the Buoyancy Formula

    Fb = F2 F1

    P = F/A

    F = PA

    F = ghA

    Fb = gh2A gh1A

    Fb = gA(h2 - h1)

    Fb = gV

    Archimedes Principle

    The bouyant force on an

    object equals the weight

    of fluid displaced by the

    object

    w = weight of an object in

    water (or any liquid)

    w = mg - Fb

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    5

    Buoyancy: Example 1

    A 7000-kg ancient statue lies at the bottom of the

    sea. Its volume is 3.0 m3. How much force is

    needed to lift it?

    Fb = gV

    Fb = (1000 kg/m3)(9.8 m/s2)(3.0m3)

    Fb = 2.94 X 104 kg-m/s2

    Fb = 2.94 X 104 N mg

    Fb

    w = mg - Fb

    w = (7000 kg)(9.8m/s2) - 2.94 X 104 N

    w = 3.92 X 104 N

    Say, isnt w just the sum of the forces?

    Yep.

    F = w mg

    Fb

    Buoyancy: Example 2

    Archimedes tested a crown for the king. Out of

    water, it masses 14.7 kg. In water, it massed 13.4

    kg. Was the crown gold?

    w = mcrg Fb

    w = mcrg gVcr

    (13.4 kg)(g) = (14.7 kg)(g) (1000 kg/m3)(g)(Vcr)

    131 N = 144 N (9800 kg/ms2)(Vcr)

    Vcr = 0.00133 m3

    Now we can calculate the density of the crown:

    = m/V = 14.7 kg/0.00133 m3

    = 11,053 kg/m3

    Golds density is about 19,000kg/m3. This is much

    closer to lead.

    Example 3

    A cube of wood that is 10 cm on a side is held

    underwater by tying a string to the cube and the

    bottom on the container. The wood has a density

    of 700 kg/m3.

    a. Draw a free body diagram showing all the forces

    on the block.

    b. Calculate the force of bouyancy

    c. Calculate the tension in the string.

    Floating Objects that are less dense than water will float

    Part of the object will be above the water line

    A case of static equilibrium

    F = 0

    mg

    Fb

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    6

    Floating: Example 1

    A 1200 kg log is floating in water. What volume of

    the log is under water?

    F = 0

    F = 0 = mg Fb

    mg = Fb

    mg = gVlog

    Vlog = mg

    g mg

    Fb

    Vlog = m (Hey, the gs cancel!)

    Vlog = 1200 kg = 1.2 m3

    1000 kg/m3

    Floating: Example 1

    A wooden raft has a density of 600 kg/m3, an area

    of 5.7 m2, and a volume of 0.60 m3. How much

    of the raft is below water in a freshwater lake?

    Lets first calculate the mass of the raft:

    = m/V

    m = V = (600 kg/m3)(0.60 m3) = 360 kg

    Now we can worry about the raft.

    F = 0

    F = 0 = mg Fb

    mg = Fb

    mg = gVsubmerged

    mg = ghsubmergedA

    mg = ghsubmergedA

    m = hsubmergedA (Hey, the gs cancelled!)

    hsubmerged = m/ A

    hsubmerged = 360 kg = 0.063 m

    (1000 kg/m3)(5.7 m2)

    Floating: Example 3

    Suppose a continent is floating on the mantle rock.

    Estimate the height of the continent above the

    mantle (assume the continent is 35 km thick).

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    7

    F = 0 = mg Fb

    0 = mcg mangVc(submerged)

    mcg = mangVc(submerged)

    mc = manVc(submerged)

    We dont know the mass of the continent

    c = mc/Vc(total)

    mc = cVc(total)

    mc = manVc(submerged)

    mc = manVc(submerged)

    mc = cVc(total)

    manVc(submerged) = cVc(total)

    Vc(submerged) = c = (2800 kg/m3) = 0.85

    Vc(total) man (3300 kg/m3)

    This means that 85% of the continent is submerged, and only 15% is above:

    (0.15)(35 km) = 5.25 km

    Floating: Ex 4

    A block is placed in water and 5.8 cm is

    submerged. The same block is placed in an

    unknown liquid and 4.6 cm is submerged.

    Calculate the density of the unknown liquid.

    Assume the same face of the block pointed

    downward in both cases (A).

    Fluid Flow

    Laminar Flow Smooth, streamline flow

    (laminar means in layers)

    Turbulent Flow erratic flow with eddies

    Viscosity Internal friction of a liquid

    High viscosity = slow flow

    Viscosity is NOT the same as density

    Equation of Continuity

    A1v1 = A2v2

    A = Area of a pipe

    v = velocity of the liquid

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    8

    Equation of Continuity

    v1A1 = v2A2

    Fluid will flow faster through a smaller opening

    Placing your finger over a hose opening.

    The term vA is the volume rate of flow

    A = m2

    v = m/s

    vA = m3/s

    Q = vA

    Eqn. Of Continuity: Example 1

    A garden hose has a radius of 1.00 cm and the

    water flows at a speed of 0.80 m/s. What will be

    the velocity if you place your finger over the hose

    and narrow the radius to 0.10 cm?

    A1 = r2 = (3.14)(0.01 m)2 = 3.14 X 10-4 m2

    A2 = r2 = (3.14)(0.001 m)2 = 3.14 X 10-6 m2

    A1v1 = A2v2

    v2 = A1v1

    A2

    v2 = (3.14 X 10-4 m2)(0.80 m/s) = 80 m/s

    (3.14 X 10-6 m2)

    Eqn. Of Continuity: Example 2

    A water hose 1.00 cm in radius fills a 20.0-liter

    bucket in one minute. What is the speed of water

    in the hose?

    A1 = r2 = (3.14)(1 cm)2 = 3.14 cm2

    Remember that Av is volume rate of flow.

    A2v2=20.0 L 1 min 1000 cm3 = 333 cm3/s

    1 min 60 s 1 L

    A1v1 = A2v2

    v1 = A2v2/A1

    v1 = 333 cm3/s = 160 cm/s or 1.60 m/s

    3.14 cm2

  • 2/27/2012

    9

    Eqn. Of Continuity: Example 3

    A sink has an area of about 0.25 m2. The drain has

    a diameter of 5 cm. If the sink drains at 0.03 m/s,

    how fast is water flowing down the drain?

    Ad = r2 = ( )(0.025 m)2 = 1.96 X 10-3 m3

    Advd = Asvs

    vd = Asvs/Ad=[(0.25 m2)(0.03 m/s)]/(1.96 X 10-3 m3)

    vd = 3.82 m/s

    Eqn. Of Continuity: Example 4

    The radius of the aorta is about 1.0 cm and blood

    passes through it at a speed of 30 cm/s. A typical

    capillary has a radius of about 4 X 10-4 cm and

    blood flows through it at a rate of 5 X 10-4 m/s.

    Estimate how many capillaries there are in the

    human body.

    Aava = NAcvc (N is the number of capillaries)

    Aa = r2 = (3.14)(0.01 m)2 = 3.14 X 10-4 m2

    Ac = r2 = (3.14)(4 X 10-6 cm)2 = 5.0 X 10-11 cm2

    N = Aava/ Acvc

    N = (3.14 X 10-4 m2)(0.30 m/s) = ~ 4 billion

    (5.0 X 10-11 cm2)(5 X 10-4 m/s)

    Eqn. Of Continuity: Example 5

    How large must a heating duct be to replenish the

    air in a room 300 m3 every 15 minutes? Assume

    air moves through the vent at 3.0 m/s.

    Advd = Arvr

    Arvr = volume rate of flow:

    Arvr = 300 m3 1 min = 0.333 m3/s

    15 min 60 s

    Ad = Arvr/vd

    Ad = 0.333 m3/s = 0.11 m2

    3.0 m/s

    Bernoullis Principle

    The velocity and

    pressure of a fluid are

    inversely related.

  • 2/27/2012

    10

    Why does a shower curtain sometimes attack a

    person taking a shower?

    What will happen to closed windows during a

    tornado? Will they blow in or out?

    Applications of Bernoullis Principle

    1. Airplane wing

    Applications of Bernoullis Principle

    2. Prairie Dog Burrows

    1. Air moves faster (lower pressure) at the top

    2. Draws air through the burrow

    3. The exact same thing happens with our chimneys

    Applications of Bernoullis Principle

    3. Spray Paint Flow of air (low pressure)

    Applications of Bernoullis Principle

    4. Dime in a cup

    Bernoullis Equation

    Pt + vt2 + gyt = Pb + vb

    2 + gyb

    (note: you often have to use the Eqn. Of Continuity

    in these situations:)

    A1v1 = A2v2

  • 2/27/2012

    11

    Often useful when you have both a change in

    height and area:

    Pipe from a water

    reservoir to a house Pipe from a house into

    a sewer pipe

    If there is no change in altitude, the equation

    simplifies:

    Pt + vt2 + gyt = Pb + vb

    2 + gyb

    Pt + vt2 = Pb + vb

    2

    Bernoullis Equation: Example 1

    A water heater in the basement of a house pumps

    water through a 4.0 cm pipe at 0.50 m/s and 3.0

    atm. What will be the flow speed and pressure

    through a 2.6 cm spigot on the second floor, 5.0

    m above?

    3.0 atm 1.013 X 105 N/m2 = 3.0 X 105 N/m2

    1 atm

    Flow speed:

    Atvt = Abvb

    vt = Abvb/At (Remember A = r2)

    vt = r2bvb (Hey, the s cancel!)

    r2t

    vt = r2

    bvb = (0.02 m)2(0.50m/s) = 1.2 m/s

    r2t (0.013 m)

    2

    Now the pressure:

    Pt + vt2 + gyt = Pb + vb

    2 + gyb

    Pt + (1000)(1.2)2 + (1000)(9.8)(5) = 3.0X105 +

    (1000)(0.50)2 + (1000)(9.8)(0)

    Pt = 2.5 X 105 N/m2

    Bernoullis Equation: Example 2

    A drunken redneck shoots a hole in the bottom of

    an aboveground swimming pool. The hole is 1.5

    m from the top of the tank. Calculate the speed

    of the water as it comes out of the hole.

    yt = 1.5 m

    yb = 0 m

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    12

    The top of the pool is a much larger area than the

    hole. We will assume that the vt = 0.

    Pt + vt2 + gyt = Pb + vb

    2 + gyb

    Pt + gyt = Pb + vb2 + gyb

    Also, both the top and the hole are open to the

    atmosphere, so Pt = Pb

    Pt + gyt = Pb + vb2 + gyb

    gyt = vb2 + gyb

    Set the bottom of the pool as yb = 0.

    gyt = vb2 + gyb

    gyt = vb2

    vb2 = 2 gyt/

    vb2 = 2gyt

    vb2 = (2)(9.8m/s2)(1.5 m)

    vb = 5.42 m/s

    Example 3

    A hydroelectric dam is 200 m above the power

    plant. The inlet hose at the top has a diameter of

    100 cm, and the outlet hose to the turbine has a

    diameter of 50 cm.

    a. Calculate the speed of the water into the turbine

    (both are open to the atmosphere)

    Elasticity: Hookes Law

    Hookes Law usually

    used with a spring

    Can consider anything to be

    like a spring

    F = k L (F=kxspring)

    k = proportionality (spring)

    constant

    Cant stretch things forever

    Elastic region material will still bounce back

    Plastic region material will not return to original

    length (but has not broken)

    F = k L

    This is only linear

    in the proportional

    region

    HOPE I DONT REACH MY

    ELASTIC LIMIT!

  • 2/27/2012

    13

    Elastic Region: Youngs

    Modulus(E) Stress = Force = F

    Area A

    Strain = Change in length = L

    Original length Lo

    Y = stress

    strain

    Y = F/A or F = Y L

    L/Lo A Lo

    Youngs Modulus: Example 1

    A 1.60 m long steel piano wire has a diameter of

    0.20 cm. How great is the tension in the wire if it

    stretches 0.30 cm when tightened?

    A = r2 = (0.0010 m)2 = 3.1 X 10-6 m2

    F = Y L

    A Lo

    F = AY L

    Lo

    F = AY L

    Lo

    F = (3.1 X 10-6m2)(200 X 1011N/m2)(0.0030 m)

    1.60 m

    F = 1200 N

    Youngs Modulus: Example 2

    A steel support rod of radius 9.5 mm and length 81

    cm is stretched by a force of 6.2 X 104 N (about 7

    tons).

    a. Calculate the stress.

    b. Calculate the elongation.

    Area = r2 = (0.0095 m2

    Stress = Force = 6.2 X 10-4m = 2.2 X 108 N/m2

    Area 2.84 X 10-4 m2

    F = Y L

    A Lo

    L = FL = (6.2 X 104 N)(0.81m)

    YA (200 X 109 N/m2)(2.84 X 10-4 m2)

    L = 8.84 X 10-4 m = 0.89 mm

  • 2/27/2012

    14

    Youngs Modulus: Example 2

    A 2.0 m long, 1.0 mm diameter wire is suspended.

    Hanging a 4.5 kg mass stretches the wire length

    by 1.00 mm.

    a. Calculate Youngs modulus

    b. Identify the material from the table.

    The Three Types of Stress

    Stretching Squeezing Horizontal

    Other Modulus

    Shear Modulus Used for shear stress

    Bulk Modulus Used for even compression on all

    sides (an object when submerged)

    Fracture

    Breaking Point

    Uses

    Tensile Strength Stretching

    Compressive Strength under a load

    Shear Stress Shearing

    Safety Factor reciprocal that is multiplied by

    the tensile strength

    Ex: A safety factor of 3 means you will only use

    1/3 of the maximum stress

    Fracture: Example 1

    A concrete column 5 m tall will have to support 1.2

    X 105 N (compression). What area must it have

    to have a safety factor of 6?

    Max stress = (1/6)(compressive strength)

    Max stress = (1/6)(20 X 106 N/m2)= 3.3X106 N/m2

    Stress = F

    A

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    15

    Stress = F

    A

    Area = F = (1.2 X 105 N) = 3.64 X 10-2 m

    Stress 3.3 X 106N/m2

    How much will the column compress under the

    load?

    F = E L

    A Lo

    L = FL = (1.2 X 105 N)(5 m)

    EA (20 X 109 N/m2)(3.64 X 10-2 m2)

    L = 8.3 X 10-4 m = 0.83 mm

    Fracture: Example 2

    Spider-mans webbing has

    a tensile strength of 600

    X 106 N/m2 and he

    wishes to use a safety

    factor of 3. What is the

    diameter of the webbing

    if the maximum force at

    the bottom of a swing is

    1500 N?

    Maximum Stress

    (1/3)(600 X 106 N/m2) = 200 X 106 N/m2

    Stress = Force

    Area

    Area = Force = 1500 N = 7.5 X 10-6m2

    Stress 200X106N/m2

    Area = r2

    r = (A/ )1/2 = 1.55 X 10-3 m or 1.55 mm

    Diameter = 3.10 mm

    Concrete

    Concrete is much stronger under compression

    than tension

    Tensile Strength 2 X 106N/m2

    Compressive Strength 20 X 106N/m2

    Prestressed concrete rods or mesh are stretched

    when the concrete is poured. Released after

    concrete dries.

    Now under compression