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You may remember that we have studied the differential equation
and that solutions of this equation were exponential functions
of the form
We found this relationship between the exponential function and the
differential equation above by examining derivatives and noticing a connection
between the exponential function and its derivative. But for many differential
equations that crop up in scientific applications, it is not very easy to
see such relationships. It is thus useful to build some tools
for understanding solutions to differential equations when they are not
known or easily found in advance. Below we will build some tools for
doing this.
Things to notice
If we look at the differential equation
we observe that it is making a statement about the slope
of a tangent line to a curve
. Indeed, this equation is
telling us that the slope is numerically equal to the value of the function!
For example, we might make a table that links values of the function
with values of its slope
Value of
| 0 | 1 | 2 |
Value of
| 0 | 1 | 2 |
This tells us that
if we were to look at a solution that passes through the
point
at any time
, then the slope of the
solution at that point would have to be
,
(and similarly for the other values).
We notice in particular that this is independent of the time at which
we look at the solution.
The differential equation is actually giving us information about a
collection of tangent lines ! The slope of the tangent lines is
connected to their height in the
plane, and does not
depend on the value of the independent variable
.
But what does all this mean? And how can all these tangent lines help
us to understand the behaviour of a solution that we do not know in
advance?
The direction field
Suppose we draw a collection of tangent lines as shown in the
picture below. This collection is often called a direction
field since it seems to give us a sense of direction in the
plane.
Remember that for every starting value (initial value)
, there is a specific exponential function
. We have shown just one of these specific
curves in blue below.
Notice that the curve has an overall
shape and direction "guided by" the direction field.
Indeed, we could say that
A solution to the differential equation
has a graph whose
tangent line at any point is one of the directions on its direction field.
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For your consideration:
- (1) By changing the initial value of the solution shown above,
experiment with the curve and show that no matter where it starts,
it will always follow the direction prescribed by the red lines.
- (2) What is the initial slope of the solution that has initial value
?
- (3) What would be the initial slope of the curve if the value of
was negative?
A second Example
To make the idea of the direction field clearer still, we
will look at a second example. Consider the equation
We actually know that the solutions of this differential equation are of the
form
But let us "pretend" momentarily that we forgot or never knew this fact.
Again, we could let the differential equation guide our qualitative
understanding of how the solution behaves.
We can make a similar table relating the values of the function
to its slope
. In this case, we would obtain
Value of
| 0 | 1 | 2 | 3 |
Value of
| 0 | -1/2 | -1 |
-3/2 |
Now, at each of the
values above, (and at some others,
not shown in the table) we might again draw a little representation of a
line with corresponding slope. The result, when we collect these together in
the
plane might look something like this:
You might notice that now, all the slopes are negative in the first
quadrant, so that any solution starting out with a positive
value will be "guided" towards the t axis, i.e. towards the value
.
For your consideration:
- (1) Experiment with various initial values of the solution shown above
in blue. Is the blue curve always tangent to the red lines?
- (2) What is the initial slope of the solution that has initial value
?
- (3) What would be the initial slope of the curve if the value of
was negative?
The ideas we have discussed here form the beginnings of an approach called
the qualitative analysis of differential equations. Even if
we had no idea what exponential functions looked like, or that they were the
solutions of the types of differential equations discussed here, the simple
ideas connecting differential equation with tangent lines and with a
direction field would have certainly conveyed to us the prediction of fast
growth or of decay of solutions to such equations.
We will see in the next few pages that these ideas are enormously useful as
they can lead us to understand the behaviour of more complicated cases
which are not so simple to understand from studying patterns of derivatives.
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