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  • Fluids

Physics for Scientists and Engineers with Modern Physics

Douglas C. Giancoli

Chapter 13

Fluids - all with Video Answers

Educators

JC

Chapter Questions

00:37

Problem 1

(I) The approximate volume of the granite monolith known
as El Capitan in Yosemite National Park (Fig. 47) is about
$10^{8} \mathrm{m}^{3} .$ What is its approximate mass?

Averell Hause
Averell Hause
Carnegie Mellon University
00:42

Problem 2

(I) What is the approximate mass of air in a living room
5.6 $\mathrm{m} \times 3.8 \mathrm{m} \times 2.8 \mathrm{m} ?$

Averell Hause
Averell Hause
Carnegie Mellon University
00:44

Problem 3

(I) If you tried to smuggle gold bricks by filling your back-
pack, whose dimensions are $56 \mathrm{cm} \times 28 \mathrm{cm} \times 22 \mathrm{cm},$ what
would its mass be?

Averell Hause
Averell Hause
Carnegie Mellon University
01:01

Problem 4

(I) State your mass and then estimate your volume. [Hint:
Because you can swim on or just under the surface of the
water in a swimming pool, you have a pretty good idea of
your density.]

Averell Hause
Averell Hause
Carnegie Mellon University
01:15

Problem 5

(II) A bottle has a mass of 35.00 $\mathrm{g}$ when empty and 98.44 $\mathrm{g}$
when filled with water. When filled with another fluid, the
mass is 89.22 $\mathrm{g}$ . What is the specific gravity of this other fluid?

Averell Hause
Averell Hause
Carnegie Mellon University
02:42

Problem 6

(II) If 5.0 $\mathrm{L}$ of antifreeze solution (specific gravity $=0.80 )$
is added to 4.0 $\mathrm{L}$ of water to make a $9.0-\mathrm{L}$ mixture, what is
the specific gravity of the mixture?

Averell Hause
Averell Hause
Carnegie Mellon University
08:06

Problem 7

(III) The Earth is not a uniform sphere, but has regions of
varying density. Consider a simple model of the Earth
divided into three regions-inner core, outer core, and
mantle. Each region is taken to have a unique constant
density (the average density of that region in the real Earth):
(a) Use this model to predict the average density of the entire
Earth. (b) The measured radius of the Earth is 6371 $\mathrm{km}$ and
its mass is $5.98 \times 10^{24} \mathrm{kg} .$ Use these data to determine the
actual average density of the Earth and compare it (as a
percent difference) with the one you determined in (a).

Averell Hause
Averell Hause
Carnegie Mellon University
00:39

Problem 8

(I) Estimate the pressure needed to raise a column of water
to the same height as a 35 -m-tall oak tree.

Averell Hause
Averell Hause
Carnegie Mellon University
02:01

Problem 9

(I) Estimate the pressure exerted on a floor by $(a)$ one pointed
chair leg $\left(66 \mathrm{kg}$ on all four legs) of area $=0.020 \mathrm{cm}^{2},$ and \right.
(b) a 1300 -kg elephant standing on one foot (area $=800 \mathrm{cm}^{2} )$

Averell Hause
Averell Hause
Carnegie Mellon University
01:43

Problem 10

(I) What is the difference in blood pressure $(\mathrm{mm}-\mathrm{Hg})$
between the top of the head and bottom of the feet of a
1.70 -m-tall person standing vertically?

Averell Hause
Averell Hause
Carnegie Mellon University
01:04

Problem 11

(II) How high would the level be in an alcohol barometer at normal atmospheric pressure?

Averell Hause
Averell Hause
Carnegie Mellon University
02:06

Problem 12

(II) In a movie, Tarzan evades his captors by hiding underwater for many minutes while breathing through a long, thin reed. Assuming the maximum pressure difference his lungs can manage and still breathe is $-85 \mathrm{mm}$ -Hg, calculate the deepest he could have been.

Averell Hause
Averell Hause
Carnegie Mellon University
01:09

Problem 13

(II) The maximum gauge pressure in a hydraulic lift is 17.0 atm. What is the largest-size vehicle $(\mathrm{kg})$ it can lift if the diameter of the output line is 22.5 $\mathrm{cm} ?$

Averell Hause
Averell Hause
Carnegie Mellon University
01:28

Problem 14

(II) The gauge pressure in each of the four tires of an automobile is 240 $\mathrm{kPa}$ . If each tire has a "footprint" of 220 $\mathrm{cm}^{2}$ , estimate the mass of the car.

Averell Hause
Averell Hause
Carnegie Mellon University
02:38

Problem 15

(II) $(a)$ Determine the total force and the absolute pressure on the bottom of a swimming pool 28.0 $\mathrm{m}$ by 8.5 $\mathrm{m}$ whose uniform depth is 1.8 $\mathrm{m} .(b)$ What will be the pressure against the side of the pool near the bottom?

Averell Hause
Averell Hause
Carnegie Mellon University
01:22

Problem 16

(II) A house at the bottom of a hill is fed by a full tank of water 5.0 $\mathrm{m}$ deep and connected to the house by a pipe that is 110 $\mathrm{m}$ long at an angle of $58^{\circ}$ from the horizontal
(Fig. $48 ) .$ (a) Determine the water gauge pressure at the house. (b) How high could the
water shoot if it came vertically out of a broken pipe in front of the house?e

Averell Hause
Averell Hause
Carnegie Mellon University
01:30

Problem 17

(II) Water and then oil (which don't mix) are poured into a U-shaped tube, open at both ends. They come to equilibrium as shown in Fig. $49 .$ What is the density of the oil? [Hint: Pressures at points a and b are equal. Why? $]$

Averell Hause
Averell Hause
Carnegie Mellon University
01:45

Problem 18

(II) In working out his principle, Pascal showed dramatically how force can be multiplied with fluid pressure. He placed a long, thin tube of radius $r=0.30 \mathrm{cm}$ vertically into a wine barrel of radius $R=21 \mathrm{cm},$ Fig. $50 .$ He found that when the barrel was filled with water and the tube filled to a height of $12 \mathrm{m},$ the barrel burst. Calculate $(a)$ the mass of water in the tube, and $(b)$ the net force exerted by the water in the barrel on the lid just before rupture.

Averell Hause
Averell Hause
Carnegie Mellon University
01:47

Problem 19

(II) What is the normal pressure of the atmosphere at the
summit of Mt. Everest, 8850 $\mathrm{m}$ above sea level?

Averell Hause
Averell Hause
Carnegie Mellon University
05:33

Problem 20

(II) A hydraulic press for compacting powdered samples has a
large cylinder which is 10.0 $\mathrm{cm}$ in diameter, and a small
cylinder with a diameter of 2.0 $\mathrm{cm}$ (Fig. $51 ) .$ A lever is attached
to the small cylinder as shown. The sample, which is placed on
the large cylinder, has an area of 4.0 $\mathrm{cm}^{2} .$ What is the pressure
on the sample if 350 $\mathrm{N}$ is applied to 0 the lever?

Donald Albin
Donald Albin
Numerade Educator
03:35

Problem 21

(II) An open-tube mercury manometer is used to measure the pressure in an oxygen tank. When the atmospheric pressure is 1040 mbar, what is the absolute pressure (in Pa) in the tank if the height of the mercury in the open tube is (a) 21.0 $\mathrm{cm}$ higher, $(b) 5.2 \mathrm{cm}$ lower, than the mercury in the tube connected to the tank?

Mathis Ernst
Mathis Ernst
Numerade Educator
02:48

Problem 22

(III) A beaker of liquid accelerates from rest, on a horizontal surface, with acceleration $a$ to the right. (a) Show that the surface of the liquid makes an angle $\theta=\tan ^{-1}(a / g)$ with
the horizontal. (b) Which edge of the water surface is higher? (c) How does the pressure vary with depth below the surface?

Averell Hause
Averell Hause
Carnegie Mellon University
05:50

Problem 23

(III) Water stands at a height $h$ behind a vertical dam of uniform width $b .(a)$ Use integration to show that the total force of the water on the dam is $F=\frac{1}{2} \rho g h^{2} b .$ (b) Show
that the torque about the base of the dam due to this force can be considered to act with a lever arm equal to $h / 3$ . (c) For a freestanding concrete dam of uniform thickness $t$ and
height $h,$ what minimum thickness is needed to prevent overturning? Do you need to add in atmospheric pressure for this last part? Explain.

Averell Hause
Averell Hause
Carnegie Mellon University
04:09

Problem 24

(III) Estimate the density of the water 5.4 $\mathrm{km}$ deep in the sea. By what fraction does it differ from the density at the surface?

Averell Hause
Averell Hause
Carnegie Mellon University
08:39

Problem 25

(III) A cylindrical bucket of liquid (density $\rho )$ is rotated about its symmetry axis, which is vertical. If the angular velocity is $\omega,$ show that the pressure at a distance $r$ from the
rotation axis is
$$P=P_{0}+\frac{1}{2} \rho \omega^{2} r^{2}$$
where $P_{0}$ is the pressure at $r=0$

JC
James Casino
Numerade Educator
01:59

Problem 26

(I) What fraction of a piece of iron will be submerged when it floats in mercury?

Averell Hause
Averell Hause
Carnegie Mellon University
01:35

Problem 27

(I) A geologist finds that a Moon rock whose mass is 9.28 $\mathrm{kg}$
has an apparent mass of 6.18 $\mathrm{kg}$ when submerged in water.
What is the density of the rock?

Averell Hause
Averell Hause
Carnegie Mellon University
03:01

Problem 28

(II) A crane lifts the $16,000$ -kg steel hull of a sunken ship
out of the water. Determine $(a)$ the tension in the crane's
cable when the hull is fully submerged in the water, and
(b) the tension when the hull is completely out of the water.

Averell Hause
Averell Hause
Carnegie Mellon University
03:07

Problem 29

(II) A spherical balloon has a radius of 7.35 $\mathrm{m}$ and is filled
with helium. How large a cargo can it lift, assuming that the
skin and structure of the balloon have a mass of 930 $\mathrm{kg}$ ?
Neglect the buoyant force on the cargo volume itself.

Averell Hause
Averell Hause
Carnegie Mellon University
01:37

Problem 30

(II) $\mathrm{A} 74$ -kg person has an apparent mass of 54 $\mathrm{kg}$ (because
of buoyancy) when standing in water that comes up to the
hips. Estimate the mass of each leg. Assume the body has
$\mathrm{SG}=1.00 .$

Averell Hause
Averell Hause
Carnegie Mellon University
02:21

Problem 31

(II) What is the likely identity of a metal (see Table 1$)$ if a
sample has a mass of 63.5 $\mathrm{g}$ when measured in air and an
apparent mass of 55.4 $\mathrm{g}$ when submerged in water?

Averell Hause
Averell Hause
Carnegie Mellon University
01:24

Problem 32

(II) Calculate the true mass (in vacuum) of a piece of
aluminum whose apparent mass is 3.0000 $\mathrm{kg}$ when weighed
in air.

Averell Hause
Averell Hause
Carnegie Mellon University
02:06

Problem 33

(II) Because gasoline is less dense than water, drums
containing gasoline will float in water. Suppose a 230 -L steel
drum is completely full of gasoline. What total volume of
steel can be used in making the drum if the gasoline-filled
drum is to float in fresh water?

Averell Hause
Averell Hause
Carnegie Mellon University
01:50

Problem 34

(II) A scuba diver and her gear displace a volume of 65.0 $\mathrm{L}$
and have a total mass of 68.0 $\mathrm{kg}$ . $(a)$ What is the buoyant force
on the diver in seawater? (b) Will the diver sink or float?

Averell Hause
Averell Hause
Carnegie Mellon University
02:34

Problem 35

(II) The specific gravity of ice is $0.917,$ whereas that of
seawater is $1.025 .$ What percent of an iceberg is above the
surface of the water?

Averell Hause
Averell Hause
Carnegie Mellon University
02:15

Problem 36

(II) Archimedes' principle can be used not only to determine the specific gravity of a solid using a known liquid (Example 10 of "Fluids"); the reverse can be done as well. (a) As an example, a $3.80-$ kg aluminum ball has an apparent mass of 2.10 $\mathrm{kg}$ when submerged in a particular liquid: calculate the density of the liquid. (b) Derive a formula for determining the density of a liquid using this procedure.

Averell Hause
Averell Hause
Carnegie Mellon University
03:25

Problem 37

(II) $(a)$ Show that the buoyant force $F_{B}$ on a partially submerged object such as a ship acts at the center of gravity of the fluid before it is displaced. This point is called the center of buoyancy. (b) To ensure that a ship is in stable equilibrium, would it be better if its center of buoyancy was
above, below, or at the same point above, below, or at the same point as, its center of gravity? Explain.

Averell Hause
Averell Hause
Carnegie Mellon University
03:24

Problem 38

(II) A cube of side length 10.0 $\mathrm{cm}$ and made of unknown
material floats at the surface between water and oil. The oil
has a density of 810 $\mathrm{kg} / \mathrm{m}^{3} .$ If the cube floats so that it is
72$\%$ in the water and 28$\%$ in the oil, what is the mass of the cube and what is the buoyant force on the cube?

Averell Hause
Averell Hause
Carnegie Mellon University
01:58

Problem 39

(II) How many helium-filled balloons would it take to lift a
person? Assume the person has a mass of 75 $\mathrm{kg}$ and that each
helium-filled balloon is spherical with a diameter of 33 $\mathrm{cm} .$

Averell Hause
Averell Hause
Carnegie Mellon University
03:16

Problem 40

(II) A scuba tank, when fully submerged, displaces 15.7 $\mathrm{L}$ of
seawater. The tank itself has a mass of 14.0 $\mathrm{kg}$ and, when
"full," contains 3.00 $\mathrm{kg}$ of air. Assuming only a weight and
buoyant force act, determine the net force (magnitude and
direction) on the fully submerged tank at the beginning of a
dive (when it is full of air) and at the end of a dive (when it
no longer contains any air).

Averell Hause
Averell Hause
Carnegie Mellon University
03:17

Problem 41

(III) If an object floats in water, its density can be determined by tying a sinker to it so that both the object and the sinker are submerged. Show that the specific gravity is given by $w /\left(w_{1}-w_{2}\right),$ where $w$ is the weight of the object alone in air, $w_{1}$ is the apparent weight when a sinker is tied to it and the sinker only is submerged, and $w_{2}$ is the apparent weight when both the object and the sinker are submerged.

Averell Hause
Averell Hause
Carnegie Mellon University
03:30

Problem 42

(III) A 3.25 -kg piece of wood $(\mathrm{SG}=0.50)$ floats on water.
What minimum mass of lead, hung from the wood by a
string, will cause it to sink?

Averell Hause
Averell Hause
Carnegie Mellon University
02:06

Problem 43

(I) A 15 -cm-radius air duct is used to replenish the air of a
room 8.2 $\mathrm{m} \times 5.0 \mathrm{m} \times 3.5 \mathrm{m}$ every 12 $\mathrm{min.}$ How fast does the air flow in the duct?

Averell Hause
Averell Hause
Carnegie Mellon University
01:16

Problem 44

(1) Using the data of Example 13 of "Fluids," calculate the
average speed of blood flow in the major arteries of the body
which have a total cross-sectional area of about 2.0 $\mathrm{cm}^{2} .$

Averell Hause
Averell Hause
Carnegie Mellon University
00:53

Problem 45

(I) How fast does water flow from a hole at the bottom of a very
wide, 5.3 -m-deep storage tank filled with water? Ignore viscosity.

Averell Hause
Averell Hause
Carnegie Mellon University
01:51

Problem 46

(II) A fish tank has dimensions 36 $\mathrm{cm}$ wide by 1.0 $\mathrm{m}$ long by
0.60 $\mathrm{m}$ high. If the filter should process all the water in the
tank once every $4.0 \mathrm{h},$ what should the flow speed be in the
3.0 -cm-diameter input tube for the filter?

Averell Hause
Averell Hause
Carnegie Mellon University
01:41

Problem 47

(II) What gauge pressure in the water mains is necessary if a
firehose is to spray water to a height of 18 $\mathrm{m} ?$

Averell Hause
Averell Hause
Carnegie Mellon University
01:38

Problem 48

(II) $\mathrm{A} \frac{5}{8}$ -in. (inside) diameter garden hose is used to fill a
round swimming pool 6.1 $\mathrm{m}$ in diameter. How long will it
take to fill the pool to a depth of 1.2 $\mathrm{m}$ if water flows from
the hose at a speed of 0.40 $\mathrm{m} / \mathrm{s} ?$

Averell Hause
Averell Hause
Carnegie Mellon University
02:31

Problem 49

(II) A $180-\mathrm{km} / \mathrm{h}$ wind blowing over the flat roof of a house
causes the roof to lift off the house. If the house is
6.2 $\mathrm{m} \times 12.4 \mathrm{m}$ in size, estimate the weight of the roof.
Assume the roof is not nailed down.

Averell Hause
Averell Hause
Carnegie Mellon University
05:59

Problem 50

(II) A 6.0 -cm-diameter horizontal pipe gradually narrows to
4.5 $\mathrm{cm} .$ When water flows through this pipe at a certain rate,
the gauge pressure in these two sections is 32.0 $\mathrm{kPa}$ and
24.0 $\mathrm{kPa}$ , respectively. What is the volume rate of flow?

Averell Hause
Averell Hause
Carnegie Mellon University
03:11

Problem 51

(II) Estimate the air pressure inside a category 5 hurricane, where the wind speed is 300 $\mathrm{km} / \mathrm{h}$ (Fig. $53 ) .$

Guilherme Barros
Guilherme Barros
Numerade Educator
02:02

Problem 52

(II) What is the lift (in newtons) due to Bernoulli's principle on a wing of area 88 $\mathrm{m}^{2}$ if the air passes over the top and bottom surfaces at speeds of 280 $\mathrm{m} / \mathrm{s}$ and $150 \mathrm{m} / \mathrm{s},$ respectively?

Averell Hause
Averell Hause
Carnegie Mellon University
01:33

Problem 53

(II) Show that the power needed to drive a fluid through a
pipe with uniform cross-section is equal to the volume rate
of flow, $Q$ , times the pressure difference, $P_{1}-P_{2}$ .

Averell Hause
Averell Hause
Carnegie Mellon University
05:10

Problem 54

(II) Water at a gauge pressure of 3.8 atm at street level flows into an office building at a speed of 0.68 $\mathrm{m} / \mathrm{s}$ through a pipe 5.0 $\mathrm{cm}$ in diameter. The pipe tapers down to 2.8 $\mathrm{cm}$ in diameter by the top floor, 18 $\mathrm{m}$ above (Fig. 54 , where the faucet has been left open. Calculate the flow velocity and the gauge pressure in the pipe
on the top floor. Assume no branch pipes and ignore viscosity.

Averell Hause
Averell Hause
Carnegie Mellon University
02:43

Problem 55

(1I) In Fig. $55,$ take into account the speed of the top surface of the tank and show that the speed of fluid leaving the opening at the bottom is
$$v_{1}=\sqrt{\frac{2 g h}{\left(1-A_{1}^{2} / A_{2}^{2}\right)}}$$
where $h=y_{2}-y_{1},$ and $A_{1}$ and $A_{2}$ are the areas of the opening and of the top surface, respectively. Assume $A_{1} \ll A_{2}$ so that the flow remains nearly steady and laminar.

Averell Hause
Averell Hause
Carnegie Mellon University
02:33

Problem 56

(II) Suppose the top surface of the vessel in Fig. 55 is
subjected to an external gauge pressure $P_{2} .(a)$ Derive a
formula for the speed, $v_{1},$ at which the liquid flows from the
opening at the bottom into atmospheric pressure, $P_{0}$ .
Assume the velocity of the liquid surface, $v_{2},$ is approxi-
mately zero. $(b)$ If $P_{2}=0.85$ atm and $y_{2}-y_{1}=2.4 \mathrm{m}$
determine $v_{1}$ for water.

Averell Hause
Averell Hause
Carnegie Mellon University
02:23

Problem 57

(II) You are watering your lawn with a hose when you put
your finger over the hose opening to increase the distance
the water reaches. If you are pointing the hose at the same
angle, and the distance the water reaches increases by a
factor of $4,$ what fraction of the hose opening did you block?

Averell Hause
Averell Hause
Carnegie Mellon University
05:34

Problem 58

(III) Suppose the opening in the tank of Fig. 55 is a height $h_{1}$
above the base and the liquid surface is a height $h_{2}$ above the
base. The tank rests on level ground. (a) At what horizontal distance from the base of the
tank will the fluid strike the ground? (b) At what other height, $h_{1}^{\prime}$ , can a hole be
placed so that the emerging liquid will have the same $"$ range $^{\prime \prime} ?$ Assume $v_{2} \approx 0$

Averell Hause
Averell Hause
Carnegie Mellon University
08:27

Problem 59

(III) $(a)$ In Fig. $55,$ show that Bernoulli's principle predicts
that the level of the liquid, $h=y_{2}-y_{1},$ drops at a rate
$$\frac{d h}{d t}=-\sqrt{\frac{2 g h A_{1}^{2}}{A_{2}^{2}-A_{1}^{2}}}$$
where $A_{1}$ and $A_{2}$ are the areas of the opening and the top
surface, respectively, assuming $A_{1} \ll A_{2},$ and viscosity is
ignored. $(b)$ Determine $h$ as a function of time by integrating.
Let $h=h_{0}$ at $t=0 .$ (c) How long would it take to empty
a 10.6 -cm-tall cylinder filled with 1.3 $\mathrm{L}$ of water if the
opening is at the bottom and has a 0.50 -cm diameter?

Averell Hause
Averell Hause
Carnegie Mellon University
05:32

Problem 60

(III) (a) Show that the flow speed measured by a venturi meter (see Fig. 32$)$ is given by the relation
$$v_{1}=A_{2} \sqrt{\frac{2\left(P_{1}-P_{2}\right)}{\rho\left(A_{1}^{2}-A_{2}^{2}\right)}}$$
(b) A venturi meter is measuring the flow of water; it has a
main diameter of 3.0 $\mathrm{cm}$ tapering down to a throat diameter
of 1.0 $\mathrm{cm} .$ If the pressure difference is measured to be $18 \mathrm{mm}-$
Hg, what is the speed of the water entering the venturi
throat?

Averell Hause
Averell Hause
Carnegie Mellon University
05:15

Problem 61

(III) Thrust of a rocket. (a) Use Bernoulli's equation and the equation of continuity to show that the emission speed of the propelling gases of a rocket is $$v=\sqrt{2\left(P-P_{0}\right) / \rho}$$
where $\rho$ is the density of the gas, $P$ is the pressure of the gas inside the rocket, and $P_{0}$ is atmospheric pressure just outside the exit orifice. Assume that the gas density stays approximately constant, and that the area of the exit orifice, $A_{0},$ is much smaller than the cross-sectional area, $A,$ of the inside of the rocket (take it to be a large cylinder). Assume also that the gas speed is not so high that significant turbulence or nonsteady flow sets in. (b) Show that the thrust force on the rocket due to the emitted gases is $$F=2 A_{0}\left(P-P_{0}\right)$$

Averell Hause
Averell Hause
Carnegie Mellon University
02:59

Problem 62

(III) A fire hose exerts a force on the person holding it. This
is because the water accelerates as it goes from the hose
through the nozzle. How much force is required to hold
a 7.0 -cm-diameter hose delivering 450 $\mathrm{L} / \mathrm{min}$ through a
0.75 -cm-diameter nozzle?

Averell Hause
Averell Hause
Carnegie Mellon University
02:23

Problem 63

(II) A viscometer consists of two concentric cylinders, 10.20 $\mathrm{cm}$
and 10.60 $\mathrm{cm}$ in diameter. A liquid fills the space between them
to a depth of 12.0 $\mathrm{cm} .$ The outer cylinder is fixed, and a torque of 0.024 $\mathrm{m} \cdot \mathrm{N}$ keeps the inner cylinder turning at a steady rotational speed of 57 $\mathrm{rev} / \mathrm{min}$ . What is the viscosity of the liquid?

Averell Hause
Averell Hause
Carnegie Mellon University
02:24

Problem 64

(III) A long vertical hollow tube with an inner diameter of
1.00 $\mathrm{cm}$ is filled with SAE 10 motor oil. A $0.900-$ cm-diameter,
30.0 -cm-long 150 -g rod is dropped vertically through the oil in the
tube. What is the maximum speed attained by the rod as it falls?

Averell Hause
Averell Hause
Carnegie Mellon University
02:08

Problem 65

(I) Engine oil (assume SAE $10,$ Table 3$)$ passes through a
fine 1.80 -mm-diameter tube that is 8.6 $\mathrm{cm}$ long. What pressure
difference is needed to maintain a flow rate of 6.2 $\mathrm{mL} / \mathrm{min}$ ?

Averell Hause
Averell Hause
Carnegie Mellon University
01:33

Problem 66

(I) A gardener feels it is taking too long to water a garden with
$\mathrm{a} \frac{3}{8}$ -in.--diameter hose. By what factor will the time be cut using a
$\frac{5}{8}$ -in.-diameter hose instead? Assume nothing else is changed.

Averell Hause
Averell Hause
Carnegie Mellon University
02:16

Problem 67

(II) What diameter must a 15.5 -m-long air duct have if the
ventilation and heating system is to replenish the air in a
room 8.0 $\mathrm{m} \times 14.0 \mathrm{m} \times 4.0 \mathrm{m}$ every 12.0 $\mathrm{min}$ ? Assume the pump can exert a gauge pressure of $0.710 \times 10^{-3} \mathrm{atm.}$

Averell Hause
Averell Hause
Carnegie Mellon University
01:31

Problem 68

(II) What must be the pressure difference between the two ends
of a 1.9 -km section of pipe, 29 $\mathrm{cm}$ in diameter, if it is to transport
oil $\left(\rho=950 \mathrm{kg} / \mathrm{m}^{3}, \eta=0.20 \mathrm{Pa} \cdot \mathrm{s}\right)$ at a rate of 650 $\mathrm{cm}^{3} / \mathrm{s} ?$

Averell Hause
Averell Hause
Carnegie Mellon University
01:43

Problem 69

(II) Poiseuille's equation does not hold if the flow velocity is high enough that turbulence sets in. The onset of turbulence occurs when the Reynolds number, Re, exceeds approximately $2000 .$ Re is defined as
$$R e=\frac{2 \overline{v} r \rho}{\eta}$$
where $\overline{v}$ is the average speed of the fluid, $\rho$ is its density, $\eta$
is its viscosity, and $r$ is the radius of the tube in which the fluid
is flowing. (a) Determine if blood flow through the aorta is
laminar or turbulent when the average speed of blood in the
aorta $(r=0.80 \mathrm{cm})$ during the resting part of the heart's
cycle is about 35 $\mathrm{cm} / \mathrm{s}$ . (b) During exercise, the blood-flow
speed approximately doubles. Calculate the Reynolds number
in this case, and determine if the flow is laminar or turbulent.

Averell Hause
Averell Hause
Carnegie Mellon University
01:10

Problem 70

(II) Assuming a constant pressure gradient, if blood flow is
reduced by $85 \%,$ by what factor is the radius of a blood
vessel decreased?

Averell Hause
Averell Hause
Carnegie Mellon University
03:54

Problem 71

(III) A patient is to be given a blood transfusion. The blood is to flow through a tube from a raised bottle to a needle inserted in the vein (Fig. $56 ) .$ The inside diameter of the $25-$
$\mathrm{mm}$ -long needle is 0.80 $\mathrm{mm}$ and the required flow rate is
2.0 $\mathrm{cm}^{3}$ of blood per minute. How high $h$ should the bottle be placed above the
needle? Obtain $\rho$ and $\eta$ from the Tables. Assume the blood pressure is 78
torr above atmospheric pressure.

Averell Hause
Averell Hause
Carnegie Mellon University
00:29

Problem 72

(I) If the force $F$ needed to move the wire in Fig. 35 is
$3.4 \times 10^{-3} \mathrm{N},$ calculate the surface tension $\gamma$ of the
enclosed fluid. Assume $\ell=0.070 \mathrm{m} .$

Averell Hause
Averell Hause
Carnegie Mellon University
00:43

Problem 73

(I) Calculate the force needed to move the wire in Fig. 35 if it
is immersed in a soapy solution and the wire is 24.5 $\mathrm{cm}$ long.

Averell Hause
Averell Hause
Carnegie Mellon University
01:34

Problem 74

(II) The surface tension of a liquid can be determined by measuring the force $F$ needed to just lift a circular platinum ring of radius $r$ from the surface of the liquid. (a) Find a formula for $\gamma$ in terms of $F$ and $r .$ (b) At $30^{\circ} \mathrm{C},$ if $F=5.80 \times 10^{-3} \mathrm{N}$ and $r=2.8 \mathrm{cm},$ calculate $\gamma$ for the tested liquid.

Averell Hause
Averell Hause
Carnegie Mellon University
01:40

Problem 75

(III) Estimate the diameter of a steel needle that can just "float" on water due to surface tension.

Averell Hause
Averell Hause
Carnegie Mellon University
00:39

Problem 76

(III) Show that inside a soap bubble, there must be a pressure $\Delta P$ in excess of that outside equal to $\Delta P=4 \gamma / r,$ where $r$ is the radius of the bubble and $\gamma$ is the surface tension. [Hint: Think of the bubble as two hemispheres in contact with each other; and remember that there are two surfaces to the bubble. Note that this result applies to any kind of membrane, where 2$\gamma$ is the tension per unit length in that membrane.

Averell Hause
Averell Hause
Carnegie Mellon University
01:05

Problem 77

(III) A common effect of surface tension is the ability of a liquid to rise up a narrow tube due to what is called capillary action. Show that for a narrow tube of radius $r$ placed in a liquid of density $\rho$ and surface tension $\gamma,$ the liquid in the tube will reach a height $h=2 \gamma / \rho g r$ above the level of the liquid outside the tube, where $g$ is the gravitational acceleration. Assume that the liquid "wets" the capillary (the liquid surface is vertical at the contact with the inside of the tube).

Averell Hause
Averell Hause
Carnegie Mellon University
02:30

Problem 78

A 2.8 -N force is applied to the plunger of a hypodermic
needle. If the diameter of the plunger is 1.3 $\mathrm{cm}$ and that
of the needle 0.20 $\mathrm{mm}$ , (a) with what force does the fluid leave
the needle? (b) What force on the plunger would be needed to
push fluid into a vein where the gauge pressure is 75 $\mathrm{mm}$ -Hg?
Answer for the instant just before the fluid starts to move.

Averell Hause
Averell Hause
Carnegie Mellon University
03:24

Problem 79

Intravenous infusions are often made under gravity, as shown in Fig. $56 .$ Assuming the fluid has a density of $1.00 \mathrm{g} / \mathrm{cm}^{3},$ at what height $h$ should the bottle be placed so
the liquid pressure is $(a) 55 \mathrm{mm}-\mathrm{Hg},$ and $(b) 650 \mathrm{mm}-\mathrm{H}_{2} \mathrm{O}$ ? (c) If the blood pressure is 78 $\mathrm{mm}$ -Hg above atmospheric
pressure, how high should the bottle be placed so that the fluid just barely enters the vein?

Averell Hause
Averell Hause
Carnegie Mellon University
04:08

Problem 80

A beaker of water rests on an electronic balance that reads 998.0 g. A 2.6 -cm-diameter solid copper ball attached to a string is submerged in the water, but does not touch the bottom. What are the tension in the string and the new balance reading?

Averell Hause
Averell Hause
Carnegie Mellon University
01:07

Problem 81

Estimate the difference in air pressure between the top and the bottom of the Empire State building in New York City. It is 380 $\mathrm{m}$ tall and is located at sea level. Express as a fraction of atmospheric pressure at sea level.

Averell Hause
Averell Hause
Carnegie Mellon University
05:32

Problem 82

A hydraulic lift is used to jack a $920-\mathrm{kg}$ car 42 $\mathrm{cm}$ off the
floor. The diameter of the output piston is $18 \mathrm{cm},$ and the
input force is 350 $\mathrm{N}$ (a) What is the area of the input piston?
(b) What is the work done in lifting the car 42 $\mathrm{cm} ?(c)$ If the input piston moves 13 $\mathrm{cm}$ in each stroke, how high does the car move up for each stroke? (d) How many strokes are required to jack the car up 42 $\mathrm{cm} ?(e)$ Show that energy is conserved.

Averell Hause
Averell Hause
Carnegie Mellon University
01:07

Problem 83

When you ascend or descend a great deal when driving in a
car, your ears "pop," which means that the pressure behind
the eardrum is being equalized to that outside. If this did
not happen, what would be the approximate force on an
eardrum of area 0.20 $\mathrm{cm}^{2}$ if a change in altitude of 950 $\mathrm{m}$
takes place?

Averell Hause
Averell Hause
Carnegie Mellon University
01:06

Problem 84

Giraffes are a wonder of cardiovascular engineering. Calcu-
late the difference in pressure (in atmospheres) that the
blood vessels in a giraffe's head must accommodate as the
head is lowered from a full upright position to ground level
for a drink. The height of an average giraffe is about 6 $\mathrm{m} .$

Averell Hause
Averell Hause
Carnegie Mellon University
01:05

Problem 85

Suppose a person can reduce the pressure in his lungs to
$-75 \mathrm{mm}$ -Hg gauge pressure. How high can water then be
"sucked" up a straw?

Averell Hause
Averell Hause
Carnegie Mellon University
01:12

Problem 86

Airlines are allowed to maintain a minimum air pressure
within the passenger cabin equivalent to that at an altitude
of 8000 $\mathrm{ft}(2400 \mathrm{m})$ to avoid adverse health effects among
passengers due to oxygen deprivation. Estimate this
minimum pressure (in atm).

Averell Hause
Averell Hause
Carnegie Mellon University
01:31

Problem 87

A simple model (Fig. 57$)$ considers a continent as a block (density $\approx 2800 \mathrm{kg} / \mathrm{m}^{3}$ ) floating in the mantle rock around it (density $\approx 3300 \mathrm{kg} / \mathrm{m}^{3} ) .$ Assuming the continent is 35 $\mathrm{km}$ thick (the average thickness of the Earth's continental crust), estimate the height of the continent above the surrounding rock.

Averell Hause
Averell Hause
Carnegie Mellon University
01:47

Problem 88

A ship, carrying fresh water to a desert island in the
Caribbean, has a horizontal cross-sectional area of 2240 $\mathrm{m}^{2}$
at the waterline. When unloaded, the ship rises 8.50 $\mathrm{m}$
higher in the sea. How many cubic meters of water was
delivered?

Averell Hause
Averell Hause
Carnegie Mellon University
02:26

Problem 89

During ascent, and especially during descent, volume changes
of trapped air in the middle ear can cause ear discomfort
until the middle-ear pressure and exterior pressure are
equalized. (a) If a rapid descent at a rate of 7.0 $\mathrm{m} / \mathrm{s}$ or
faster commonly causes ear discomfort, what is the
maximum rate of increase in atmospheric pressure (that is,
$d P / d t$ ) tolerable to most people? $(b)$ In a 350 -m-tall
building, what will be the fastest possible descent time for
an elevator traveling from the top to ground floor, assuming
the elevator is properly designed to account for human
physiology?

Averell Hause
Averell Hause
Carnegie Mellon University
02:18

Problem 90

A raft is made of 12 logs lashed together. Each is 45 $\mathrm{cm}$ in
diameter and has a length of 6.1 $\mathrm{m}$ . How many people can the
raft hold before they start getting their feet wet, assuming the
average person has a mass of 68 $\mathrm{kg}$ ? Do not neglect the weight
of the logs. Assume the specific gravity of wood is $0.60 .$

Averell Hause
Averell Hause
Carnegie Mellon University
01:37

Problem 91

Estimate the total mass of the Earth's atmosphere, using
the known value of atmospheric pressure at sea level.

Averell Hause
Averell Hause
Carnegie Mellon University
01:19

Problem 92

During each heartbeat, approximately 70 $\mathrm{cm}^{3}$ of blood is
pushed from the heart at an average pressure of $105 \mathrm{mm}-\mathrm{Hg}$ .
Calculate the power output of the heart, in watts, assuming
70 beats per minute.

Averell Hause
Averell Hause
Carnegie Mellon University
03:47

Problem 93

Four lawn sprinkler heads are fed by a 1.9 -cm-diameter
pipe. The water comes out of the heads at an angle of $35^{\circ}$
to the horizontal and covers a radius of 7.0 $\mathrm{m} .$ (a) What is
the velocity of the water coming out of each sprinkler
head? (Assume zero air resistance.) (b) If the output diam-
eter of each head is 3.0 $\mathrm{mm}$ , how many liters of water do
the four heads deliver per second? (c) How fast is the
water flowing inside the 1.9 -cm-diameter pipe?

Averell Hause
Averell Hause
Carnegie Mellon University
03:21

Problem 94

A bucket of water is accelerated upward at 1.8 $\mathrm{g} .$ What is
the buoyant force on a 3.0 -kg granite rock $(\mathrm{SG}=2.7)$
submerged in the water? Will the rock float? Why or why not?

Averell Hause
Averell Hause
Carnegie Mellon University
02:50

Problem 95

The stream of water from a faucet decreases in diameter as it falls (Fig. 58 . Derive an equation for the diameter of the stream as a function of the distance$y$ below the faucet, given that the
water has speed $v_{0}$ when it leaves the faucet, whose diameter is $d$ .

Averell Hause
Averell Hause
Carnegie Mellon University
02:29

Problem 96

You need to siphon water from a clogged sink. The sink has
an area of 0.38 $\mathrm{m}^{2}$ and is filled to a height of 4.0 $\mathrm{cm} .$ Your
siphon tube rises 45 $\mathrm{cm}$ above the bottom of the sink and then descends 85 $\mathrm{cm}$ to a pail as shown in Fig. $59 .$ The siphon
tube has a diameter of 2.0 $\mathrm{cm} .$ (a) Assuming that the water
level in the sink has almost zero velocity, estimate the
water velocity when it enters the pail. (b) Estimate how
long it will take to cmpty the sink.

Averell Hause
Averell Hause
Carnegie Mellon University
03:12

Problem 97

An airplane has a mass of $1.7 \times 10^{6} \mathrm{kg},$ and the air flows
past the lower surface of the wings at 95 $\mathrm{m} / \mathrm{s} .$ If the wings
have a surface area of 1200 $\mathrm{m}^{2}$ , how fast must the air flow
over the upper surface of the wing if the plane is to stay in
the air?

Averell Hause
Averell Hause
Carnegie Mellon University
07:25

Problem 98

A drinking fountain shoots water about 14 $\mathrm{cm}$ up in the air
from a nozzle of diameter 0.60 $\mathrm{cm}$ . The pump at the base of
the unit $(1.1 \mathrm{m}$ below the nozzle) pushes water into a $1.2-$
$\mathrm{cm}$ -diameter supply pipe that goes up to the nozzle, What
gauge pressure does the pump have to provide? Ignore the
viscosity; your answer will therefore be an underestimate.

Averell Hause
Averell Hause
Carnegie Mellon University
02:08

Problem 99

A hurricane-force wind of 200 $\mathrm{km} / \mathrm{h}$ blows across the face
of a storefront window. Estimate the force on the 2.0 $\mathrm{m} \times 3.0 \mathrm{m}$ window due to the difference in air pressure
inside and outside the window. Assume the store is airtight so
the inside pressure remains at 1.0 atm. (This is why you should
not tightly seal a building in preparation for a hurricane).

Averell Hause
Averell Hause
Carnegie Mellon University
02:30

Problem 100

Blood from an animal is placed in a bottle 1.30 $\mathrm{m}$ above a
3.8 -cm-long needle, of inside diameter $0.40 \mathrm{mm},$ from
which it flows at a rate of 4.1 $\mathrm{cm}^{3} / \mathrm{min} .$ What is the
viscosity of this blood?

Averell Hause
Averell Hause
Carnegie Mellon University
04:09

Problem 101

Three forces act significantly on a freely floating helium-
filled balloon: gravity, air resistance (or drag force), and a
buoyant force. Consider a spherical helium-filled balloon
of radius $r=15 \mathrm{cm}$ rising upward through $0^{\circ} \mathrm{C}$ air,
and $m=2.8 \mathrm{g}$ is the mass of the (deflated) balloon itself.
For all speeds $v,$ except the very slowest ones, the flow of
air past a rising balloon is turbulent, and the drag force $F_{\mathrm{D}}$
is given by the relation
$$F_{\mathrm{D}}=\frac{1}{2} C_{\mathrm{D}} \rho_{\mathrm{air}} \pi r^{2} v^{2}$$
where the constant $C_{D}=0.47$ is the "drag coefficient"
for a smooth sphere of radius $r .$ If this balloon is released
from rest, it will accelerate very quickly $($ in a few tenths
of a second) to its terminal velocity $v_{T},$ where the
buoyant force is cancelled by the drag force and the
balloon's total weight. Assuming the balloon's accelera-
tion takes place over a negligible time and distance, how
long does it take the released balloon to rise a distance
$h=12 \mathrm{m} ?$

Averell Hause
Averell Hause
Carnegie Mellon University
01:13

Problem 102

If cholesterol buildup reduces the diameter of an artery by
$15 \%,$ by what $\%$ will the blood flow rate be reduced,
assuming the same pressure difference?

Averell Hause
Averell Hause
Carnegie Mellon University
05:07

Problem 103

A two-component model used to determine percent body
fat in a human body assumes that a fraction $f(<1)$ of the
body's total mass $m$ is composed of fat with a density of
$0.90 \mathrm{g} / \mathrm{cm}^{3},$ and that the remaining mass of the body is
composed of fat-free tissue with a density of 1.10 $\mathrm{g} / \mathrm{cm}^{3} .$ If
the specific gravity of the entire body's density is $X,$ show
that the percent body fat $(=f \times 100)$ is given by
$$\% \text { Body fat }=\frac{495}{X}-450$$

Averell Hause
Averell Hause
Carnegie Mellon University
05:56

Problem 104

(III) Air pressure decreases with altitude. The following data
show the air pressure at different altitudes.
(a) Determine the best-fit quadratic equation that shows
how the air pressure changes with altitude. $(b)$ Determine
the best-fit exponential equation that describes the change
of air pressure with altitude. (c) Use each fit to find the air
pressure at the summit of the mountain $\mathrm{K} 2$ at $8611 \mathrm{m},$ and
give the \% difference.

Averell Hause
Averell Hause
Carnegie Mellon University

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