In this section we need to take a look at the equation of a line in R 3 R 3 . As we saw in the previous section the equation y = m x + b y = m x + b does not describe a line in R 3 R 3 , instead it describes a plane. This doesn’t mean however that we can’t write down an equation for a line in 3-D space. We’re just going to need a new way of writing down the equation of a curve. So, before we get into the equations of lines we first need to briefly look at vector functions. We’re going to take a more in depth look at vector functions later. At this point all that we need to worry about is notational issues and how they can be used to give the equation of a curve. The best way to get an idea of what a vector function is and what its graph looks like is to look at an example. So, consider the following vector function. → r ( t ) = ⟨ t , 1 ⟩ r → ( t ) = ⟨ t , 1 ⟩ A vector function is a function that takes one or more variables, one in this case, and returns a...
Example 2 Find a series solution around for the following differential equation.
As with the first example and so again for this differential equation every point is an ordinary point. Now we’ll start this one out just as we did the first example. Let’s write down the form of the solution and get its derivatives.
Plugging into the differential equation gives,
Unlike the first example we first need to get all the coefficients moved into the series.
Now we will need to shift the first series down by 2 and the second series up by 1 to get both of the series in terms of .
Next, we need to get the two series starting at the same value of . The only way to do that for this problem is to strip out the term.
We now need to set all the coefficients equal to zero. We will need to be careful with this however. The coefficient is in front of the series and the are all in the series. So, setting coefficient equal to zero gives,
Solving the first as well as the recurrence relation gives,
Now we need to start plugging in values of .
There are a couple of things to note about these coefficients. First, every third coefficient is zero. Next, the formulas here are somewhat unpleasant and not all that easy to see the first time around. Finally, these formulas will not work for unlike the first example.
Now, get the solution,
Again, collect up the terms that contain the same coefficient, factor the coefficient out and write the results as a new series,
We couldn’t start our series at this time since the general term doesn’t hold for .
Plugging into the differential equation gives,
Unlike the first example we first need to get all the coefficients moved into the series.
Now we will need to shift the first series down by 2 and the second series up by 1 to get both of the series in terms of .
Next, we need to get the two series starting at the same value of . The only way to do that for this problem is to strip out the term.
We now need to set all the coefficients equal to zero. We will need to be careful with this however. The coefficient is in front of the series and the are all in the series. So, setting coefficient equal to zero gives,
Solving the first as well as the recurrence relation gives,
Now we need to start plugging in values of .
Now, get the solution,
Again, collect up the terms that contain the same coefficient, factor the coefficient out and write the results as a new series,
We couldn’t start our series at this time since the general term doesn’t hold for .
Now, we need to work an example in which we use a point other that . In fact, let’s just take the previous example and rework it for a different value of . We’re also going to need to change up the instructions a little for this example.
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