Applications to Physics and Engineering

Section 7.5 Applications to Physics and Engineering

Applications to Physics and Engineering

Work

The term work is used in everyday language to mean the total amount of effort required to perform a task.In physics it has a technical meaning that depends on the idea of a force. Intuitively, you can think of aforce as describing a push or pull on an object — for example, a horizontal push of a book across a tableor the downward pull of the Earth’s gravity on a ball. In general, if an object moves along a straight linewith position function s(t), then the force F on the object (in the same direction) is defined by Newton’sSecond Law of Motion as the product of its mass m and its acceleration:

F = md2s

dt2(1)

In the SI metric system, the mass is measured in kilograms (kg), the displacement in meters (m), the timein seconds (s), and the force in newtons (N = kg · m/s2). Thus a force of 1 N acting on a mass of 1 kgproduces an acceleration of 1 m/s2. In the US Customary system the fundamental unit is chosen to bethe unit of force, which is the pound.

In the case of constant acceleration, the force F is also constant and the work done is defined to be theproduct of the force F and the distance d that the object moves:

W = Fd work = force × distance (2)

If F is measured in newtons and d in meters, then the unit for W is a newton-meter, which is called ajoule (J). If F is measured in pounds and d in feet, then the unit for W is a foot-pound (ft-lb), which isabout 1.36 J.

EXAMPLE:

(a) How much work is done in lifting a 1.2-kg book off the floor to put it on a desk that is 0.7 m high?Use the fact that the acceleration due to gravity is g = 9.8 m/s2.

(b) How much work is done in lifting a 20-lb weight 6 ft off the ground?

1


EXAMPLE:

(a) How much work is done in lifting a 1.2-kg book off the floor to put it on a desk that is 0.7 m high?Use the fact that the acceleration due to gravity is g = 9.8 m/s2.

(b) How much work is done in lifting a 20-lb weight 6 ft off the ground?

Solution:

(a) The force exerted is equal and opposite to that exerted by gravity, so Equation 1 gives

F = mg = (1.2)(9.8) = 11.76 N

and then Equation 2 gives the work done as

W = Fd = (11.76)(0.7) ≈ 8.2 J

(b) Here the force is given as F = 20 lb, so the work done is

W = Fd = 20 · 6 = 120 ft-lb

Notice that in part (b), unlike part (a), we did not have to multiply by g because we were given the weight

(which is a force) and not the mass of the object.

Equation 2 defines work as long as the force is constant, but what happens if the force is variable? Let’ssuppose that the object moves along the x-axis in the positive direction, from x = a to x = b, and at eachpoint x between a and b a force f(x) acts on the object, where f is a continuous function. We divide theinterval [a, b] into n subintervals with end points x0, x1, . . . , xn and equal width ∆x. We choose a samplepoint x∗

i in the ith subinterval [xi−1, xi]. Then the force at that point is f(x∗

i ). If n is large, then ∆x issmall, and since f is continuous, the values of f don’t change very much over the interval [xi−1, xi]. Inother words, f is almost constant on the interval and so the work Wi that is done in moving the particlefrom xi−1 to xi is approximately given by Equation 2:

Wi ≈ f(x∗

i )∆x

Thus we can approximate the total work by

W ≈n∑

i=1

f(x∗

i )∆x (3)

It seems that this approximation becomes better as we make n larger. Therefore, we define the work

done in moving the object from a to b as the limit of this quantity as n → ∞. Since the right sideof (3) is a Riemann sum, we recognize its limit as being a definite integral and so

W = limn→∞

n∑

i=1

f(x∗

i )∆x =

∫ b

a

f(x)dx (4)

EXAMPLE: When a particle is located a distance x feet from the origin, a force of x2 + 2x pounds actson it. How much work is done in moving it from x = 1 to x = 3?

2


EXAMPLE: When a particle is located a distance x feet from the origin, a force of x2 + 2x pounds actson it. How much work is done in moving it from x = 1 to x = 3?

Solution: We have

W =

∫ 3

1

(x2 + 2x)dx =

[x3

3+ x2

]3

1

=50

3

The work done is 1623

ft-lb.

In the next example we use a law from physics: Hooke’s Law states that the force required to maintaina spring stretched x units beyond its natural length is proportional to x:

f(x) = kx

where k is a positive constant (called the spring constant). Hooke’s Law holds provided that x is nottoo large.

EXAMPLE: A force of 40 N is required to hold a spring that has been stretched from its natural lengthof 10 cm to a length of 15 cm. How much work is done in stretching the spring from 15 cm to 18 cm?

3


EXAMPLE: A force of 40 N is required to hold a spring that has been stretched from its natural lengthof 10 cm to a length of 15 cm. How much work is done in stretching the spring from 15 cm to 18 cm?

Solution: According to Hooke’s Law, the force required to hold the spring stretched x meters beyond itsnatural length is f(x) = kx. When the spring is stretched from 10 cm to 15 cm, the amount stretched is5 cm = 0.05 m. This means that f(0.05) = 40, so

0.05k = 40 =⇒ k =40

0.05= 800

Thus f(x) = 800x and the work done in stretching the spring from 15 cm to 18 cm is

W =

∫ 0.08

0.05

800xdx = 800x2

2

]0.08

0.05

= 400[(0.08)2 − (0.05)2

]= 1.56 J

EXAMPLE: A 200-lb cable is 100 ft long and hangs vertically from the top of a tall building. How muchwork is required to lift the cable to the top of the building?

Solution: Here we don’t have a formula for the force function, but we can use an argument similar to theone that led to Definition 4.

Let’s place the origin at the top of the building and the x-axis pointing downward as in the figure above.We divide the cable into small parts with length ∆x. If x∗

i is a point in the ith such interval, then allpoints in the interval are lifted by approximately the same amount, namely x∗

i . The cable weighs 2 poundsper foot, so the weight of the ith part is 2∆x. Thus the work done on the ith part, in foot-pounds, is

(2∆x)︸︷︷︸

force

· x∗

i︸︷︷︸

distance

= 2x∗

i ∆x

We get the total work done by adding all these approximations and letting the number of parts becomelarge (so ∆x → 0):

W = limn→∞

n∑

i=1

2x∗

i ∆x =

∫ 100

0

2xdx = x2]100

0= 10, 000 ft-lb

EXAMPLE: A tank has the shape of an inverted circular cone with height 10 m and base radius 4 m. Itis filled with water to a height of 8 m. Find the work required to empty the tank by pumping all of thewater to the top of the tank. (The density of water is 1000 kg/m3.)

4


EXAMPLE: A tank has the shape of an inverted circular cone with height 10 m and base radius 4 m. Itis filled with water to a height of 8 m. Find the work required to empty the tank by pumping all of thewater to the top of the tank. (The density of water is 1000 kg/m3.)

Solution: Let’s measure depths from the top of the tank by introducing a vertical coordinate line. Thewater extends from a depth of 2 m to a depth of 10 m and so we divide the interval [2, 10] into n subintervalswith endpoints x0, x1, . . . , xn and choose x∗

i in the ith subinterval. This divides the water into n layers.The ith layer is approximated by a circular cylinder with radius ri and height ∆x. We can compute ri

from similar triangles as follows:

ri

10 − x∗

i

=4

10=⇒ ri =

2

5(10 − x∗

i )

Thus an approximation to the volume of the ith layer of water is

Vi ≈ πr2i ∆x =

4π

25(10 − x∗

i )2 ∆x

and so its mass is

mi = density × volume ≈ 1000 ·4π

25(10 − x∗

i )2 ∆x = 160π (10 − x∗

i )2 ∆x

The force required to raise this layer must overcome the force of gravity and so

Fi = mig ≈ 9.8 · 160π (10 − x∗

i )2 ∆x ≈ 1568π (10 − x∗

i )2 ∆x

Each particle in the layer must travel a distance of approximately x∗

i . The work Wi done to raise this layerto the top is approximately the product of the force Fi and the distance x∗

i :

Wi ≈ Fix∗

i ≈ 1568πx∗

i (10 − x∗

i )2 ∆x

To find the total work done in emptying the entire tank, we add the contributions of each of the n layersand then take the limit as n → ∞:

W = limn→∞

n∑

i=1

1568πx∗

i (10 − x∗

i )2 ∆x =

∫ 10

2

1568πx (10 − x)2 dx

= 1568π

∫ 10

2

(100x − 20x2 + x3

)dx = 1568π

[

50x2 −20x3

3+

x4

4

]10

2

= 1568π ·2048

3≈ 3.4 × 106 J

5


Hydrostatic Pressure and Force

Deep-sea divers realize that water pressure increases as they dive deeper. This is because the weight ofthe water above them increases.

In general, suppose that a thin horizontal plate with area A square meters is submerged in a fluid ofdensity ρ kilograms per cubic meter at a depth d meters below the surface of the fluid.

The fluid directly above the plate has volume V = Ad, so its mass is m = ρV = ρAd. The force exertedby the fluid on the plate is therefore

F = mg = ρgAd

where g is the acceleration due to gravity. The pressure P on the plate is defined to be the force per unitarea:

P =F

A= ρgd

The SI unit for measuring pressure is newtons per square meter, which is called a pascal (abbreviation: 1N/m2 = 1 Pa). Since this is a small unit, the kilopascal (kPa) is often used. For instance, because thedensity of water is ρ = 1000 kg/m3, the pressure at the bottom of a swimming pool 2 m deep is

P = ρgd = 1000 kg/m3 × 9.8 m/s2 × 2 m = 19, 600 Pa = 19.6 kPa

An important principle of fluid pressure is the experimentally verified fact that at any point in a liquid the

pressure is the same in all directions. (A diver feels the same pressure on nose and both ears.) Thus, thepressure in any direction at a depth d in a fluid with mass density ρ is given by

P = ρgd = δd (5)

This helps us determine the hydrostatic force against a vertical plate or wall or dam in a fluid. This is nota straightforward problem because the pressure is not constant but increases as the depth increases.

EXAMPLE: A dam has the shape of the trapezoid shown in the figure below. The height is 20 m and thewidth is 50 m at the top and 30 m at the bottom. Find the force on the dam due to hydrostatic pressureif the water level is 4 m from the top of the dam.

6


EXAMPLE: A dam has the shape of the trapezoid shown in the figure below. The height is 20 m and thewidth is 50 m at the top and 30 m at the bottom. Find the force on the dam due to hydrostatic pressureif the water level is 4 m from the top of the dam.

Solution: We choose a vertical x-axis with origin at the surface of the water:

The depth of the water is 16 m, so we divide the interval [0, 16] into subintervals of equal length withendpoints xi and we choose x∗

i ∈ [xi−1, xi]. The ith horizontal strip of the dam is approximated by arectangle with height ∆x and width wi, where, from similar triangles,

a

16 − x∗

i

=10

20=⇒ a =

16 − x∗

i

2= 8 −

1

2x∗

i

and so

wi = 2(15 + a) = 2

(

15 + 8 −1

2x∗

i

)

= 46 − x∗

i

If Ai is the area of the ith strip, then

Ai ≈ wi∆x = (46 − x∗

i ) ∆x

If ∆x is small, then the pressure Pi on the ith strip is almost constant and we can use Equation 5 to write

Pi ≈ 1000gx∗

i

The hydrostatic force Fi acting on the ith strip is the product of the pressure and the area:

Fi = PiAi ≈ 1000gx∗

i (46 − x∗

i )∆x

Adding these forces and taking the limit as n → ∞, we obtain the total hydrostatic force on the dam:

F = limn→∞

n∑

i=1

1000gx∗

i (46 − x∗

i )∆x =

∫ 16

0

1000gx(46− x)dx

= 1000 · 9.8∫ 16

0

(46x − x2

)dx = 9800

[

23x2 −x3

3

]16

0

≈ 4.43 × 107 N

7


EXAMPLE: Find the hydrostatic force on one end of a cylindrical drum with radius 3 ft if the drum issubmerged in water 10 ft deep.

Solution: In this example it is convenient to choose the axes as in figure above so that the origin is placedat the center of the drum. Then the circle has a simple equation, x2 + y2 = 9. We divide the circularregion into horizontal strips of equal width. From the equation of the circle, we see that the length of theith strip is 2

√

9 − (y∗

i )2 and so its area is

Ai = 2√

9 − (y∗

i )2∆y

The pressure on this strip is approximately

δdi = 62.5 (7 − y∗

i )

and so the force on the strip is approximately

δdiAi = 62.5 (7 − y∗

i ) 2√

9 − (y∗

i )2∆y

The total force is obtained by adding the forces on all the strips and taking the limit:

F = limn→∞

n∑

i=1

62.5 (7 − y∗

i ) 2√

9 − (y∗

i )2∆y

= 125

∫ 3

−3

(7 − y)√

9 − y2dy

= 125 · 7∫ 3

−3

√

9 − y2dy − 125

∫ 3

−3

y√

9 − y2dy

The second integral is 0 because the integrand is an odd function. The first integral can be evaluated usingthe trigonometric substitution y = 3 sin θ, but it’s simpler to observe that it is the area of a semicirculardisk with radius 3. Thus

F = 875

∫ 3

−3

√

9 − y2dy = 875 ·1

2π · 32 =

7875π

2≈ 12, 370 lb

8


Moments and Centers of Mass

Our main objective here is to find the point P on which a thin plate of any given shape balances horizontally.This point is called the center of mass (or center of gravity) of the plate.

We first consider the simpler situation illustrated in the figure below, where two masses m1 and m2 areattached to a rod of negligible mass on opposite sides of a fulcrum and at distances d1 and d2 from thefulcrum.

The rod will balance ifm1d1 = m2d2 (6)

This is an experimental fact discovered by Archimedes and called the Law of the Lever.

Now suppose that the rod lies along the x-axis with m1 at x1 and m2 at x2 and the center of mass at x.If we compare the figure above and the figure below, we see that d1 = x − x1 and d2 = x2 − x and soEquation 6 gives

m1(x − x1) = m2(x2 − x) =⇒ m1x + m2x = m1x1 + m2x2 =⇒ x =m1x1 + m2x2

m1 + m2(7)

The numbers m1x1 and m2x2 are called the moments of the masses m1 and m2 (with respect to theorigin), and Equation 7 says that the center of mass x is obtained by adding the moments of the massesand dividing by the total mass m = m1 + m2.

9


In general, if we have a system of n particles with masses m1, m2, . . . , mn located at the points x1, x2, . . . , xn

on the x-axis, it can be shown similarly that the center of mass of the system is located at

x =

n∑

i=1

mixi

n∑

i=1

mi

=

n∑

i=1

mixi

m(8)

where m =

n∑

i=1

mi is the total mass of the system, and the sum of the individual moments M =

n∑

i=1

mixi is

called the moment of the system about the origin. Then Equation 8 could be rewritten as mx = M,which says that if the total mass were considered as being concentrated at the center of mass, then itsmoment would be the same as the moment of the system.

Now we consider a system of n particles with masses m1, m2, . . . , mn located at the points (x1, y1), (x2, y2),. . . , (xn, yn) in the xy-plane:

By analogy with the one-dimensional case, we define the moment of the system about the y-axis tobe

My =

n∑

i=1

mixi (9)

and the moment of the system about the x-axis as

Mx =n∑

i=1

miyi (10)

Then My measures the tendency of the system to rotate about the y-axis and Mx measures the tendencyto rotate about the x-axis. As in the one-dimensional case, the coordinates (x, y) of the center of mass aregiven in terms of the moments by the formulas

x =My

mand y =

Mx

m(11)

where m =n∑

i=1

mi is the total mass. Since mx = My and my = Mx, the center of mass (x, y) is the point

where a single particle of mass m would have the same moments as the system.

EXAMPLE: Find the moments and center of mass of the system of objects that have masses 3, 4, and 8at the points (−1, 1), (2,−1), and (3, 2).

10


EXAMPLE: Find the moments and center of mass of the system of objects that have masses 3, 4, and 8at the points (−1, 1), (2,−1), and (3, 2).

Solution: We use Equations 9 and 10 to compute the moments:

My = 3 · (−1) + 4 · 2 + 8 · 3 = 29

Mx = 3 · 1 + 4 · (−1) + 8 · 2 = 15

Since m = 3 + 4 + 8 = 15, we use Equations 11 to obtain

x =My

m=

29

15and y =

Mx

m=

15

15= 1

Thus the center of mass is(114

15, 1

).

Next we consider a flat plate (called a lamina) with uniform density ρ that occupies a region R of theplane. We wish to locate the center of mass of the plate, which is called the centroid of R. In doing sowe use the following physical principles: The symmetry principle says that if R is symmetric about aline l, then the centroid of R lies on l. (If R is reflected about l, then R remains the same so its centroidremains fixed. But the only fixed points lie on l.) Thus the centroid of a rectangle is its center. Momentsshould be defined so that if the entire mass of a region is concentrated at the center of mass, then itsmoments remain unchanged. Also, the moment of the union of two nonoverlapping regions should be thesum of the moments of the individual regions.

Suppose that the region R is of the type shown in first figure below; that is, R lies between the lines x = aand x = b, above the x-axis, and beneath the graph of f, where f is a continuous function.

We divide the interval [a, b] into n subintervals with endpoints x0, x1, . . . , xn, and equal width ∆x. Wechoose the sample point x∗

i to be the midpoint xi of the ith subinterval, that is, xi = (xi−1 + xi)/2. Thisdetermines the polygonal approximation to R shown in the second figure above. The centroid of the ithapproximating rectangle Ri is its center Ci

(xi,

12f(xi)

). Its area is f(xi)∆x, so its mass is

ρf(xi)∆x

The moment of Ri about the y-axis is the product of its mass and the distance from Ci, to the y-axis,which is xi. Thus

My(Ri) = [ρf(xi)∆x]xi = ρxif(xi)∆x

11


Adding these moments, we obtain the moment of the polygonal approximation to R, and then by takingthe limit as n → ∞ we obtain the moment of R itself about the y-axis:

My = limn→∞

n∑

i=1

ρxif(xi)∆x = ρ

∫ b

a

xf(x)dx

In a similar fashion we compute the moment of Ri about the x-axis as the product of its mass and thedistance from Ci to the x-axis:

Mx(Ri) = [ρf(xi)∆x]1

2f(xi) = ρ ·

1

2[f(xi)]

2∆x

Again we add these moments and take the limit to obtain the moment of R about the x-axis:

Mx = limn→∞

n∑

i=1

ρ ·1

2[f(xi)]

2∆x = ρ

∫ b

a

1

2[f(x)]2dx

Just as for systems of particles, the center of mass of the plate is defined so that mx = My and my = Mx.But the mass of the plate is the product of its density and its area:

m = ρA = ρ

∫ b

a

f(x)dx

and so

x =My

m=

ρ

∫ b

a

xf(x)dx

ρ

∫ b

a

f(x)dx

=

∫ b

a

xf(x)dx

∫ b

a

f(x)dx

y =Mx

m=

ρ

∫ b

a

1

2[f(x)]2dx

ρ

∫ b

a

f(x)dx

=

∫ b

a

1

2[f(x)]2dx

∫ b

a

f(x)dx

Notice the cancellation of the ρ’s. The location of the center of mass is independent of the density.

In summary, the center of mass of the plate (or the centroid of R) is located at the point (x, y), where

x =1

A

∫ b

a

xf(x)dx y =1

A

∫ b

a

1

2[f(x)]2dx (12)

EXAMPLE: Find the center of mass of a semicircular plate of radius r.

12


EXAMPLE: Find the center of mass of a semicircular plate of radius r.

Solution: In order to use (12) we place the semicircle as in the figure above so that f(x) =√

r2 − x2 anda = −r, b = r. Here there is no need to use the formula to calculate x because, by the symmetry principle,the center of mass must lie on the y-axis, so x = 0. The area of the semicircle is A = 1

2πr2, so

y =1

A

∫ r

−r

1

2[f(x)]2dx =

112πr2

.1

2

∫ r

−r

(√

r2 − x2)2dx

=2

πr2

∫ r

0

(r2 − x2)dx =2

πr2

[

r2x −x3

3

]r

0

=2

πr2·2r3

3=

4r

3π

The center of mass is located at the point(0, 4r

3π

).

EXAMPLE: Find the centroid of the region bounded by the curves y = cos x, y = 0, x = 0, and x = π/2.

13


EXAMPLE: Find the centroid of the region bounded by the curves y = cos x, y = 0, x = 0, and x = π/2.

Solution: The area of the region is

A =

∫ π/2

0

cos xdx = sin x]π/20 = 1

so Formulas 12 give

x =1

A

∫ π/2

0

xf(x)dx =

∫ π/2

0

x cos xdx = x sin x]π/20 −

∫ π/2

0

sin xdx =π

2− 1

and

y =1

A

∫ π/2

0

1

2[f(x)]2dx =

1

2

∫ π/2

0

cos2 xdx =1

4

∫ π/2

0

(1 + cos 2x)dx =1

4

[

x +1

2sin 2x

]π/2

0

=π

8

The centroid is(

12π − 1, 1

8π).

If the region R lies between two curves y = f(x) and y = g(x), where f(x) ≥ g(x), then the same sort of

argument that led to Formulas 12 can be used to show that the centroid of R is (x, y), where

x =1

A

∫ b

a

x[f(x) − g(x)]dx y =1

A

∫ b

a

1

2

{[f(x)]2 − [g(x)]2

}dx (13)

EXAMPLE: Find the centroid of the region bounded by the line y = x and the parabola y = x2.

14


EXAMPLE: Find the centroid of the region bounded by the line y = x and the parabola y = x2.

Solution: We take f(x) = x, g(x) = x2, a = 0, and b = 1 in Formulas 13. First we note that the area ofthe region is

A =

∫ 1

0

(x − x2)dx =

[x2

2−

x3

3

]1

0

=1

6

Therefore

x =1

A

∫ 1

0

x[f(x) − g(x)]dx =1

1/6

∫ 1

0

x(x − x2)dx = 6

∫ 1

0

(x2 − x3)dx = 6

[x3

3−

x4

4

]1

0

=1

2

and

y =1

A

∫ 1

0

1

2

{[f(x)]2 − [g(x)]2

}dx =

1

1/6

∫ 1

0

1

2(x2 − x4)dx = 3

[x3

3−

x5

5

]1

0

=2

5

The centroid is(

12, 2

5

).

We end this section by showing a surprising connection between centroids and volumes of revolution.

THEOREM OF PAPPUS: Let R be a plane region that lies entirely on one side of a line l in the plane.If R is rotated about l, then the volume of the resulting solid is the product of the area A of R and thedistance d traveled by the centroid of R.

Proof: We give the proof for the special case in which the region lies between y = f(x) and y = g(x) andthe line l is the y-axis. Using the method of cylindrical shells we have

V =

∫ b

a

2πx[f(x) − g(x)]dx = 2π

∫ b

a

x[f(x) − g(x)]dx(13)= 2π(xA) = (2πx)A = Ad

where d = 2πx is the distance traveled by the centroid during one rotation about the y-axis. �

EXAMPLE: A torus is formed by rotating a circle of radius r about a line in the plane of the circle thatis a distance R (> r) from the center of the circle. Find the volume of the torus.

Solution: The circle has area A = πr2. By the symmetry principle, its centroid is its center and so thedistance traveled by the centroid during a rotation is d = 2πR. Therefore, by the Theorem of Pappus, thevolume of the torus is

V = Ad =(πr2

)(2πR) = 2π2r2R

15

Applications to Physics and Engineering

Documents