I apologize for the outage on the site yesterday and today. Lamar University is in Beaumont Texas and Hurricane Laura came through here and caused a brief power outage at Lamar. Things should be up and running at this point and (hopefully) will stay that way, at least until the next hurricane comes through here which seems to happen about once every 10-15 years. Note that I wouldn't be too suprised if there are brief outages over the next couple of days as they work to get everything back up and running properly. I apologize for the inconvienence.

Paul

August 27, 2020

*i.e.*you are probably on a mobile phone). Due to the nature of the mathematics on this site it is best views in landscape mode. If your device is not in landscape mode many of the equations will run off the side of your device (should be able to scroll to see them) and some of the menu items will be cut off due to the narrow screen width.

### Section 6-6 : Work

This is the final application of integral that we’ll be looking at in this course. In this section we will be looking at the amount of work that is done by a force in moving an object.

In a first course in Physics you typically look at the work that a constant force, \(F\), does when moving an object over a distance of \(d\). In these cases the work is,

\[W = Fd\]However, most forces are not constant and will depend upon where exactly the force is acting. So, let’s suppose that the force at any \(x\) is given by \(F\left( x \right)\). Then the work done by the force in moving an object from \(x = a\) to \(x = b\) is given by,

\[W = \int_{{\,a}}^{{\,b}}{{F\left( x \right)\,dx}}\]To see a justification of this formula see the Proof of Various Integral Properties section of the Extras chapter.

Notice that if the force is constant we get the correct formula for a constant force.

\[\begin{align*}W & = \int_{{\,a}}^{{\,b}}{{F\,dx}}\\ & = \left. {Fx} \right|_a^b\\ & = F\left( {b - a} \right)\end{align*}\]where \(b - a\) is simply the distance moved, or \(d\).

So, let’s take a look at a couple of examples of non-constant forces.

This example will require Hooke’s Law to determine the force. Hooke’s Law tells us that the force required to stretch a spring a distance of \(x\) meters from its natural length is,

\[F\left( x \right) = k\,x\]where \(k > 0\) is called the spring constant. It is important to remember that the \(x\) in this formula is the distance the spring is stretched from its natural length and not the actual length of the spring.

So, the first thing that we need to do is determine the spring constant for this spring. We can do that using the initial information. A force of 40 N is required to stretch the spring

\[30cm - 20cm = 10cm = 0.1m\]from its natural length. Using Hooke’s Law we have,

\[40 = 0.10k\hspace{0.25in} \Rightarrow \hspace{0.25in}\,k = 400\]So, according to Hooke’s Law the force required to hold this spring \(x\) meters from its natural length is,

\[F\left( x \right) = 400x\]We want to know the work required to stretch the spring from 35cm to 38cm. First, we need to convert these into distances from the natural length in meters. Doing that gives us \(x\)’s of 0.15m and 0.18m.

The work is then,

\[\begin{align*}W & = \int_{{\,0.15}}^{{\,0.18}}{{400x\,dx}}\\ & = \left. {200{x^2}} \right|_{0.15}^{0.18}\\ & = 1.98\,{\mbox{J}}\end{align*}\]- Determine the amount of work required to lift the bucket to the midpoint of the shaft.
- Determine the amount of work required to lift the bucket from the midpoint of the shaft to the top of the shaft.
- Determine the amount of work required to lift the bucket all the way up the shaft.

Before answering either part we first need to determine the force. In this case the force will be the weight of the bucket and cable at any point in the shaft.

To determine a formula for this we will first need to set a convention for \(x\). For this problem we will set \(x\) to be the amount of cable that has been pulled up. So at the bottom of the shaft \(x = 0\), at the midpoint of the shaft \(x = 250\) and at the top of the shaft \(x = 500\). Also, at any point in the shaft there is \(500 - x\) feet of cable still in the shaft.

The force then for any \(x\) is then nothing more than the weight of the cable and bucket at that point. This is,

\[\begin{align*}F\left( x \right) & = {\mbox{weight of cable}} + {\mbox{ weight of bucket/coal}}\\ & = 2\left( {500 - x} \right) + 800\\ & = 1800 - 2x\end{align*}\]We can now answer the questions.

a Determine the amount of work required to lift the bucket to the midpoint of the shaft. Show Solution

In this case we want to know the work required to move the cable and bucket/coal from \(x = 0\) to \(x = 250\). The work required is,

\[\begin{align*}W & = \int_{{\,0}}^{{\,250}}{{F\left( x \right)\,dx}}\\ & = \int_{{\,0}}^{{\,250}}{{1800 - 2x\,dx}}\\ & = \left. {\left( {1800x - {x^2}} \right)} \right|_0^{250}\\ & = 387500\,\,{\mbox{ft - lb}}\end{align*}\]b Determine the amount of work required to lift the bucket from the midpoint of the shaft to the top of the shaft. Show Solution

In this case we want to move the cable and bucket/coal from \(x = 250\) to \(x = 500\). The work required is,

\[\begin{align*}W & = \int_{{\,250}}^{{\,500}}{{F\left( x \right)\,dx}}\\ & = \int_{{\,250}}^{{\,500}}{{1800 - 2x\,dx}}\\ & = \left. {\left( {1800x - {x^2}} \right)} \right|_{250}^{500}\\ & = 262500\,\,{\mbox{ft - lb}}\end{align*}\]c Determine the amount of work required to lift the bucket all the way up the shaft. Show Solution

In this case the work is,

\[\begin{align*}W & = \int_{{\,0}}^{{\,500}}{{F\left( x \right)\,dx}}\\ & = \int_{{\,0}}^{{\,500}}{{1800 - 2x\,dx}}\\ & = \left. {\left( {1800x - {x^2}} \right)} \right|_0^{500}\\ & = 650000\,\,{\mbox{ft - lb}}\end{align*}\]Note that we could have instead just added the results from the first two parts and we would have gotten the same answer to the third part.

First, we need to determine the weight per foot of the cable. This is easy enough to get,

\[\frac{{80{\mbox{ lbs}}}}{{20{\mbox{ ft}}}} = 4{\mbox{ lb/ft}}\]Next, let \(x\) be the distance from the ceiling to any point on the cable. Using this convention we can see that the portion of the cable in the range \(10 < x \le 20\) will actually be lifted. The portion of the cable in the range \(0 \le x \le 10\) will not be lifted at all since once the bottom of the cable has been lifted up to the ceiling the cable will be doubled up and each portion will have a length of 10 ft. So, the upper 10 foot portion of the cable will never be lifted while the lower 10 ft portion will be lifted.

Now, the very bottom of the cable, \(x = 20\), will be lifted 10 feet to get to the midpoint and then a further 10 feet to get to the ceiling. A point 2 feet from the bottom of the cable, \(x = 18\) will lift 8 feet to get to the midpoint and then a further 8 feet until it reaches its final position (if it is 2 feet from the bottom then its final position will be 2 feet from the ceiling). Continuing on in this fashion we can see that for any point on the lower half of the cable, *i.e.* \(10 \le x \le 20\) it will be lifted a total of \(2\left( {x - 10} \right)\).

As with the previous example the force required to lift any point of the cable in this range is simply the distance that point will be lifted times the weight/foot of the cable. So, the force is then,

\[\begin{align*}F\left( x \right) & = \left( {{\mbox{distance lifted}}} \right)\left( {{\mbox{weight per foot of cable}}} \right)\\ & = 2\left( {x - 10} \right)\left( 4 \right)\\ & = 8\left( {x - 10} \right)\end{align*}\]The work required is now,

\[\begin{align*}W & = \int_{{\,10}}^{{\,20}}{{8\left( {x - 10} \right)\,dx}}\\ & = \left. {\left( {4{x^2} - 80x} \right)} \right|_{10}^{20}\\ & = 400\,\,{\mbox{ft - lb}}\end{align*}\]Provided we can find the force, \(F\left( x \right)\), for a given problem then using the above method for determining the work is (generally) pretty simple. However, there are some problems where this approach won’t easily work. Let’s take a look at one of those kinds of problems.

^{3}.

Okay, in this case we cannot just determine a force function, \(F\left( x \right)\) that will work for us. So, we are going to need to approach this from a different standpoint.

Let’s first set \(x = 0\) to be the lower end of the tank/cone and \(x = 15\) to be the top of the tank/cone. With this *definition* of our \(x\)’s we can now see that the water in the tank will correspond to the interval \(\left[ {0,12} \right]\).

So, let’s start off by dividing \(\left[ {0,12} \right]\) into \(n\) subintervals each of width \(\Delta x\) and let’s also let \(x_i^*\) be any point from the \(i\)^{th} subinterval where \(i = 1,2, \ldots n\). Now, for each subinterval we will approximate the water in the tank corresponding to that interval as a cylinder of radius \({r_i}\) and height \(\Delta x\).

Here is a quick sketch of the tank. Note that the sketch really isn’t to scale and we are looking at the tank from directly in front so we can see all the various quantities that we need to work with.

The red strip in the sketch represents the “cylinder” of water in the \(i\)^{th} subinterval. A quick application of similar triangles will allow us to relate \({r_i}\) to \(x_i^*\) (which we’ll need in a bit) as follows.

Okay, the mass, \({m_i}\), of the volume of water, \({V_i}\), for the \(i\)^{th} subinterval is simply,

We know the density of the water (it was given in the problem statement) and because we are approximating the water in the \(i\)^{th} subinterval as a cylinder we can easily approximate the volume as,

We can now approximate the mass of water in the \(i\)^{th} subinterval,

To raise this volume of water we need to overcome the force of gravity that is acting on the volume and that is, \(F = {m_i}g\), where \(g = 9.8\,m/s^{2}\) is the gravitational acceleration. The force to raise the volume of water in the \(i\)^{th} subinterval is then approximately,

Next, in order to reach to the top of the tank the water in the \(i\)^{th} subinterval will need to travel approximately \(15 - x_i^*\) to reach the top of the tank. Because the volume of the water in the \(i\)^{th} subinterval is constant the force needed to raise the water through any distance is also a constant force.

Therefore, the work to move the volume of water in the \(i\)^{th} subinterval to the top of the tank, *i.e.* raise it a distance of \(15 - x_i^*\), is then approximately,

The total amount of work required to raise all the water to the top of the tank is then approximately the sum of each of the \({W_i}\) for \(i = 1,2, \ldots n\). Or,

\[W \approx \sum\limits_{i = 1}^n {\left( {9.8} \right)\frac{{640}}{9}\pi {{\left( {x_i^*} \right)}^2}\left( {15 - x_i^*} \right)\Delta x} \]To get the actual amount of work we simply need to take \(n \to \infty \). *I.e.* compute the following limit,

This limit of a summation should look somewhat familiar to you. It’s probably been some time, but recalling the definition of the definite integral we can see that this is nothing more than the following definite integral,

\[\begin{align*}W &= \int_{0}^{{12}}{{\left( {9.8} \right)\frac{{640}}{9}\pi {x^2}\left( {15 - x} \right)\,dx}} = \left( {9.8} \right)\frac{{640}}{9}\pi \int_{0}^{{12}}{{15{x^2} - {x^3}\,dx}}\\ & = \left. {\left( {9.8} \right)\frac{{640}}{9}\pi \left( {5{x^3} - \frac{1}{4}{x^4}} \right)} \right|_0^{12} = 7,566,362.543\,{\mbox{J}}\end{align*}\]As we’ve seen in the previous example we sometimes need to compute “incremental” work and then use that to determine the actual integral we need to compute. This idea does arise on occasion and we shouldn’t forget it!