A fundamental concept in classical physics is **work**: If an object is moved in a straight line against
a force $F$ for a distance $s$ the work done is $W=Fs$.

Example 8.5.1 How much work is done in lifting a 10 pound weight vertically a distance of 5 feet? The force due to gravity on a 10 pound weight is 10 pounds at the surface of the earth, and it does not change appreciably over 5 feet. The work done is $W=10\cdot 5=50$ foot-pounds. $\square$

In reality few situations are so simple. The force might not be constant over the range of motion, as in the next example.

Example 8.5.2 How much work is done in lifting a 10 pound weight from the surface of the earth to an orbit 100 miles above the surface? Over 100 miles the force due to gravity does change significantly, so we need to take this into account. The force exerted on a 10 pound weight at a distance $r$ from the center of the earth is $\ds F=k/r^2$ and by definition it is 10 when $r$ is the radius of the earth (we assume the earth is a sphere). How can we approximate the work done? We divide the path from the surface to orbit into $n$ small subpaths. On each subpath the force due to gravity is roughly constant, with value $\ds k/r_i^2$ at distance $\ds r_i$. The work to raise the object from $\ds r_i$ to $\ds r_{i+1}$ is thus approximately $\ds k/r_i^2\Delta r$ and the total work is approximately $$\sum_{i=0}^{n-1} {k\over r_i^2}\Delta r,$$ or in the limit $$W=\int_{r_0}^{r_1} {k\over r^2}\,dr,$$ where $\ds r_0$ is the radius of the earth and $\ds r_1$ is $\ds r_0$ plus 100 miles. The work is $$W=\int_{r_0}^{r_1} {k\over r^2}\,dr= -\left.{k\over r}\right|_{r_0}^{r_1}=-{k\over r_1}+{k\over r_0}.$$ Using $\ds r_0=20925525$ feet we have $\ds r_1=21453525$. The force on the 10 pound weight at the surface of the earth is 10 pounds, so $\ds 10=k/20925525^2$, giving $k=4378775965256250$. Then $$-{k\over r_1}+{k\over r_0}={491052320000\over 95349}\approx 5150052 \quad\hbox{foot-pounds}.$$ Note that if we assume the force due to gravity is 10 pounds over the whole distance we would calculate the work as $\ds 10(r_1-r_0)=10\cdot100\cdot 5280=5280000$, somewhat higher since we don't account for the weakening of the gravitational force. $\square$

Example 8.5.3 How much work is done in lifting a 10 kilogram object from the surface of the earth to a distance $D$ from the center of the earth? This is the same problem as before in different units, and we are not specifying a value for $D$. As before $$W=\int_{r_0}^{D} {k\over r^2}\,dr= -\left.{k\over r}\right|_{r_0}^{D}=-{k\over D}+{k\over r_0}.$$ While "weight in pounds'' is a measure of force, "weight in kilograms'' is a measure of mass. To convert to force we need to use Newton's law $F=ma$. At the surface of the earth the acceleration due to gravity is approximately 9.8 meters per second squared, so the force is $F=10\cdot 9.8=98$. The units here are "kilogram-meters per second squared'' or "kg m/s$^2$'', also known as a Newton (N), so $F=98$ N. The radius of the earth is approximately 6378.1 kilometers or 6378100 meters. Now the problem proceeds as before. From $\ds F=k/r^2$ we compute $k$: $\ds 98=k/6378100^2$, $\ds k= 3.986655642\cdot 10^{15}$. Then the work is: $$W=-{k\over D}+6.250538000\cdot 10^8\quad\hbox{Newton-meters.}$$ As $D$ increases $W$ of course gets larger, since the quantity being subtracted, $-k/D$, gets smaller. But note that the work $W$ will never exceed $\ds 6.250538000\cdot 10^8$, and in fact will approach this value as $D$ gets larger. In short, with a finite amount of work, namely $\ds 6.250538000\cdot 10^8$ N-m, we can lift the 10 kilogram object as far as we wish from earth; we might also say that this is the work required to lift the object to infinity. $\square$

Next is an example in which the force is constant, but there are many objects moving different distances.

Example 8.5.4 Suppose that a water tank is shaped like a right circular cone with the tip at the bottom, and has height 10 meters and radius 2 meters at the top. If the tank is full, how much work is required to pump all the water out over the top? Here we have a large number of atoms of water that must be lifted different distances to get to the top of the tank. Fortunately, we don't really have to deal with individual atoms—we can consider all the atoms at a given depth together.

To approximate the work, we can divide the water in the tank into horizontal sections, approximate the volume of water in a section by a thin disk, and compute the amount of work required to lift each disk to the top of the tank. As usual, we take the limit as the sections get thinner and thinner to get the total work.

At depth $h$ the circular cross-section through the tank has radius $r=(10-h)/5$, by similar triangles, and area $\ds \pi(10-h)^2/25$. A section of the tank at depth $h$ thus has volume approximately $\ds \pi(10-h)^2/25\Delta h$ and so contains $\ds \sigma\pi(10-h)^2/25\Delta h$ kilograms of water, where $\sigma$ is the density of water in kilograms per cubic meter; $\sigma\approx 1000$. The force due to gravity on this much water is $\ds 9.8\sigma\pi(10-h)^2/25\Delta h$, and finally, this section of water must be lifted a distance $h$, which requires $\ds h9.8\sigma\pi(10-h)^2/25\Delta h$ Newton-meters of work. The total work is therefore $$W={9.8\sigma\pi\over 25} \int_0^{10} h(10-h)^2\,dh={980000\over3}\pi\approx 1026254\quad\hbox{Newton-meters.}$$ $\square$

A spring has a "natural length,'' its length if nothing is stretching
or compressing it. If the spring is either stretched or compressed the
spring provides an opposing force; according to **Hooke's
Law** the magnitude of this force is proportional to the
distance the spring has been stretched or compressed: $F=kx$.
The constant of proportionality, $k$, of course depends on the
spring. Note that $x$ here represents the *change* in length from the
natural length.

Example 8.5.5 Suppose $k=5$ for a given spring that has a natural length of $0.1$ meters. Suppose a force is applied that compresses the spring to length $0.08$. What is the magnitude of the force? Assuming that the constant $k$ has appropriate dimensions (namely, kg/s$^2$), the force is $5(0.1-0.08)=5(0.02)=0.1$ Newtons. $\square$

Example 8.5.6 How much work is done in compressing the spring in the previous example from its natural length to $0.08$ meters? From $0.08$ meters to $0.05$ meters? How much work is done to stretch the spring from $0.1$ meters to $0.15$ meters? We can approximate the work by dividing the distance that the spring is compressed (or stretched) into small subintervals. Then the force exerted by the spring is approximately constant over the subinterval, so the work required to compress the spring from $\ds x_i$ to $\ds x_{i+1}$ is approximately $\ds 5(x_i-0.1)\Delta x$. The total work is approximately $$\sum_{i=0}^{n-1} 5(x_i-0.1)\Delta x$$ and in the limit $$W=\int_{0.1}^{0.08} 5(x-0.1)\,dx=\left.{5(x-0.1)^2\over2}\right|_{0.1}^{0.08}= {5(0.08-0.1)^2\over2}-{5(0.1-0.1)^2\over2}={1\over1000}\,\hbox{N-m}.$$ The other values we seek simply use different limits. To compress the spring from $0.08$ meters to $0.05$ meters takes $$W=\int_{0.08}^{0.05} 5(x-0.1)\,dx=\left.{5(x-0.1)^2\over2}\right|_{0.08}^{0.05}= {5(0.05-0.1)^2\over2}-{5(0.08-0.1)^2\over2}={21\over4000}\,\hbox{N-m}$$ and to stretch the spring from $0.1$ meters to $0.15$ meters requires $$W=\int_{0.1}^{0.15} 5(x-0.1)\,dx=\left.{5(x-0.1)^2\over2}\right|_{0.1}^{0.15}= {5(0.15-0.1)^2\over2}-{5(0.1-0.1)^2\over2}={1\over160}\,\hbox{N-m}.$$ $\square$

## Exercises 8.5

You can use Sage to help check your work.

**Ex 8.5.1**
How much work is done in lifting a 100 kilogram weight from
the surface of the earth to an orbit 35,786 kilometers above the
surface of the earth?
(answer)

**Ex 8.5.2**
How much work is done in lifting a 100 kilogram weight from
an orbit 1000 kilometers above the surface of the earth to an orbit
35,786 kilometers above the surface of the earth?
(answer)

**Ex 8.5.3**
A water tank has the shape of an upright cylinder with radius $r=1$
meter and height 10 meters. If the depth of the water is 5 meters, how
much work is required to pump all the water out the top of the tank?
(answer)

**Ex 8.5.4**
Suppose the tank of the previous problem is lying on its
side, so that the circular ends are vertical, and that it has the same
amount of water as before. How much work is required to pump the water
out the top of the tank (which is now 2 meters above the bottom of the
tank)?
(answer)

**Ex 8.5.5**
A water tank has the shape of the bottom half of a sphere
with radius $r=1$ meter. If the tank is full,
how much work is required to pump all the water out
the top of the tank?
(answer)

**Ex 8.5.6**
A spring has constant $k=10$ kg/s$^2$. How much work is done
in compressing it $1/10$ meter from its natural length?
(answer)

**Ex 8.5.7**
A force of 2 Newtons will compress a spring from 1 meter
(its natural length) to
0.8 meters. How much work is required to stretch the spring from
1.1 meters to 1.5 meters?
(answer)

**Ex 8.5.8**
A 20 meter long steel cable has density 2 kilograms per
meter, and is hanging straight down. How much work is required to lift
the entire cable to the height of its top end?
(answer)

**Ex 8.5.9**
The cable in the previous problem has a 100 kilogram bucket
of concrete attached to its lower end. How much work is required to lift
the entire cable and bucket to the height of its top end?
(answer)

**Ex 8.5.10**
Consider again the cable and bucket of the previous problem.
How much work is required to lift the bucket 10 meters by raising the
cable 10 meters? (The top half of the cable ends up at the height of
the top end of the cable, while the bottom half of the cable is lifted
10 meters.)
(answer)