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0.2 Introduction to differential equations

Note: more than 1 lecture, §1.1 in [EP], chapter 1 in [BD]

0.2.1 Differential equations

The laws of physics are generally written down as differential equations. Therefore, all of science and engineering use differential equations to some degree. Understanding differential equations is essential to understanding almost anything you will study in your science and engineering classes. You can think of mathematics as the language of science, and differential equations are one of the most important parts of this language as far as science and engineering are concerned. As an analogy, suppose all your classes from now on were given in Swahili. It would be important to first learn Swahili, or you would have a very tough time getting a good grade in your classes.

You have already seen many differential equations without perhaps knowing about it. And you have even solved simple differential equations when you were taking calculus. Let us see an example you may not have seen:

dx-+ x = 2 cost. dt
(1)

Here x is the dependent variable and t is the independent variable. Equation (1) is a basic example of a differential equation. In fact it is an example of a first order differential equation, since it involves only the first derivative of the dependent variable. This equation arises from Newton’s law of cooling where the ambient temperature oscillates with time.

0.2.2 Solutions of differential equations

Solving the differential equation means finding x in terms of t . That is, we want to find a function of t , which we will call x , such that when we plug x , t , and dx dt into (1), the equation holds. It is the same idea as it would be for a normal (algebraic) equation of just x and t . We claim that

x = x(t) = co st + sin t

is a solution. How do we check? We simply plug x into equation (1)! First we need to compute dx dt . We find that dx dt = - sin t + cos t . Now let us compute the left hand side of (1).

dx-+ x = (- sint + co st) + (cost + sint) = 2 cost. dt

Yay! We got precisely the right hand side. But there is more! We claim x = cos t + sin t + e-t is also a solution. Let us try,

dx-= - sint + c ost - e-t. dt

Again plugging into the left hand side of (1)

dx- -t -t dt + x = (- sint + co st - e ) + (cost + sint + e ) = 2 cost.

And it works yet again!

So there can be many different solutions. In fact, for this equation all solutions can be written in the form

x = cost + sin t + Ce-t

for some constant C . See Figure 1 for the graph of a few of these solutions. We will see how we find these solutions a few lectures from now.


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Figure 1: Few solutions of dx dt + x = 2 cost .


It turns out that solving differential equations can be quite hard. There is no general method that solves every differential equation. We will generally focus on how to get exact formulas for solutions of certain differential equations, but we will also spend a little bit of time on getting approximate solutions.

For most of the course we will look at ordinary differential equations or ODEs, by which we mean that there is only one independent variable and derivatives are only with respect to this one variable. If there are several independent variables, we will get partial differential equations or PDEs. We will briefly see these near the end of the course.

Even for ODEs, which are very well understood, it is not a simple question of turning a crank to get answers. It is important to know when it is easy to find solutions and how to do so. Although in real applications you will leave much of the actual calculations to computers, you need to understand what they are doing. It is often necessary to simplify or transform your equations into something that a computer can understand and solve. You may need to make certain assumptions and changes in your model to achieve this.

To be a successful engineer or scientist, you will be required to solve problems in your job that you have never seen before. It is important to learn problem solving techniques, so that you may apply those techniques to new problems. A common mistake is to expect to learn some prescription for solving all the problems you will encounter in your later career. This course is no exception.

0.2.3 Differential equations in practice

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So how do we use differential equations in science and engineering? First, we have some real world problem we wish to understand. We make some simplifying assumptions and create a mathematical model. That is, we translate the real world situation into a set of differential equations. Then we apply mathematics to get some sort of a mathematical solution. There is still something left to do. We have to interpret the results. We have to figure out what the mathematical solution says about the real world problem we started with.

Learning how to formulate the mathematical model and how to interpret the results is what your physics and engineering classes do. In this course we will focus mostly on the mathematical analysis. Sometimes we will work with simple real world examples, so that we have some intuition and motivation about what we are doing.

Let us look at an example of this process. One of the most basic differential equations is the standard exponential growth model. Let P denote the population of some bacteria on a Petri dish. We assume that there is enough food and enough space. Then the rate of growth of bacteria is proportional to the population—a large population grows quicker. Let t denote time (say in seconds) and P the population. Our model is

dP- = kP, dt

for some positive constant k > 0 .

Example 0.2.1: Suppose there are 100 bacteria at time 0 and 200 bacteria 10 seconds later. How many bacteria will there be 1 minute from time 0 (in 60 seconds)?

First we have to solve the equation. We claim that a solution is given by

P (t) = Cekt,

where C is a constant. Let us try:

dP ---= Ckekt = kP. dt

And it really is a solution.

OK, so what now? We do not know C and we do not know k . But we know something. We know P (0 ) = 100 , and we also know P(10) = 200 . Let us plug these conditions in and see what happens.

 k0 100 = P(0) = Ce = C, 200 = P(10) = 100ek10.
Therefore,  10k 2 = e or ln2 10-= k ≈ 0.069 . So we know that
 (ln2)t∕10 0.069t P (t) = 100e ≈ 100e .

At one minute, t = 60 , the population is P (6 0) = 64 00 . See Figure 2.


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Figure 2: Bacteria growth in the first 60 seconds.


Let us talk about the interpretation of the results. Does our solution mean that there must be exactly 6400 bacteria on the plate at 60s? No! We made assumptions that might not be true exactly, just approximately. If our assumptions are reasonable, then there will be approximately 6400 bacteria. Also, in real life P is a discrete quantity, not a real number. However, our model has no problem saying that for example at 61 seconds, P(61) ≈ 6859.35 .

Normally, the k in P′ = kP is known, and we want to solve the equation for different initial conditions. What does that mean? Take k = 1 for simplicity. Now suppose we want to solve the equation dP = P dt subject to P (0 ) = 1000 (the initial condition). Then the solution turns out to be (exercise)

 t P(t) = 1 000e .

We call P(t) = Cet the general solution, as every solution of the equation can be written in this form for some constant C . You will need an initial condition to find out what C is, in order to find the particular solution we are looking for. Generally, when we say “particular solution,” we just mean some solution.

Let us get to what we will call the four fundamental equations. These equations appear very often and it is useful to just memorize what their solutions are. These solutions are reasonably easy to guess by recalling properties of exponentials, sines, and cosines. They are also simple to check, which is something that you should always do. There is no need to wonder if you have remembered the solution correctly.

First such equation is,

dy ---= ky, dx

for some constant k > 0 . Here y is the dependent and x the independent variable. The general solution for this equation is

y(x) = Cekx.

We have already seen that this function is a solution above with different variable names.

Next,

dy- dx = - ky,

for some constant k > 0 . The general solution for this equation is

y(x) = Ce -kx.

Exercise 0.2.1: Check that the y given is really a solution to the equation.

Next, take the second order differential equation

 2 d-y-= - k2y, dx2

for some constant k > 0 . The general solution for this equation is

y(x) = C1 cos(kx ) + C2 sin(kx).

Note that because we have a second order differential equation, we have two constants in our general solution.

Exercise 0.2.2: Check that the y given is really a solution to the equation.

And finally, take the second order differential equation

 2 d-y-= k2y, dx2

for some constant k > 0 . The general solution for this equation is

 kx -kx y(x) = C1e + C 2e ,

or

y(x) = D cosh(kx ) + D sin h(kx ). 1 2

For those that do not know, co sh and sinh are defined by

 ex + e-x cosh x = -------, x 2 -x e---e--- sinh x = 2 .
These functions are sometimes easier to work with than exponentials. They have some nice familiar properties such as cosh0 = 1 , sin h0 = 0 , and ddx-coshx = sinhx (no that is not a typo) and ddx sinh x = coshx .

Exercise 0.2.3: Check that both forms of the y given are really solutions to the equation.

An interesting note about cosh : The graph of cosh is the exact shape a hanging chain will make. This shape is called a catenary. Contrary to popular belief this is not a parabola. If you invert the graph of cosh it is also the ideal arch for supporting its own weight. For example, the gateway arch in Saint Louis is an inverted graph of cosh —if it were just a parabola it might fall down. The formula used in the design is inscribed inside the arch:

y = -127.7ft ⋅ cosh(x∕12 7.7ft) + 757.7ft.

0.2.4 Exercises

Exercise 0.2.4: Show that x = e4t is a solution to x′′′ - 12x ′′ + 4 8x′ - 64x = 0 .

Exercise 0.2.5: Show that x = et is not a solution to x′′′ - 12x′′ + 48x ′ - 64x = 0 .

Exercise 0.2.6: Is y = sint a solution to (dy)2 2 dt = 1 - y ? Justify.

Exercise 0.2.7: Let y′′ + 2y′ - 8y = 0 . Now try a solution of the form y = erx for some (unknown) constant r . Is this a solution for some r ? If so, find all such r .

Exercise 0.2.8: Verify that x = Ce-2t is a solution to x′ = - 2x . Find C to solve for the initial condition x (0) = 100 .

Exercise 0.2.9: Verify that  -t 2t x = C1e + C 2e is a solution to  ′′ ′ x - x - 2x = 0 . Find C1 and C 2 to solve for the initial conditions x(0) = 10 and  ′ x (0) = 0 .

Exercise 0.2.10: Find a solution to  ′2 2 (x ) + x = 4 using your knowledge of derivatives of functions that you know from basic calculus.

Exercise 0.2.11: Solve:

a) dA-= -10A dt ,  A(0) = 5 b) dH--= 3H dx ,  H (0) = 1
c)  2 d-y-= 4y dx 2 ,  y(0) = 0 ,  y′(0) = 1 d)  2 d--x = -9x dy2 ,  x(0) = 1 ,  x′(0) = 0

Exercise 0.2.12: Is there a solution to y′ = y , such that y(0) = y(1) ?

Note: Exercises with numbers 101 and higher have solutions in the back of the book.

Exercise 0.2.101: Show that x = e-2t is a solution to x′′ + 4x′ + 4x = 0 .

Exercise 0.2.102: Is y = x2 a solution to x2y′′ - 2y = 0 ? Justify.

Exercise 0.2.103: Let  ′′ ′ xy - y = 0 . Try a solution of the form  r y = x . Is this a solution for some r ? If so, find all such r .

Exercise 0.2.104: Verify that x = C1et + C 2 is a solution to x′′ - x′ = 0 . Find C 1 and C 2 so that x satisfies x(0) = 10 and x′(0) = 100 .

Exercise 0.2.105: Solve dφ ds = 8φ and φ (0) = -9 .