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Others then messed up the algebra.
How many of you checked your answers? You know that the derivative of $x^{-2}$ is $-2x^{-3}$....
or
You can't slip that $x$ into the argument of $\cos(x)$. By the way, all trig functions need arguments: $\sin$ is a sin, not a sine. $\sin$ is a hungry operator, and needs something to eat: e.g. $\sin(x)$. We say "Sine of $x$" -- the "of" is the hunger: sine of what?
One more issue (two people, at least):
We might call this "over-simplification"....
We have a serious algebra problem here....
Use the quadratic formula. It always works.
Your sketch should be of a cubic. If you know what cubics look like, you're way ahead; if you don't, you're behind.
The Extreme Value Theorem guarantees that there will be global max and min on this interval.
So now we know how to handle closed, bounded intervals; now let's talk about what happens when we let $x$ become unbounded. How will a function behave as $x$ races off to $\infty$ or $-\infty$?
Another example with a horizontal asymptote is knowledge as a function of time -- #51, p. 222. We might guess that accumulated knowledge in studying for an exam looks something like this:
We might imagine that this physical process becomes less productive from hour to hour as the evening wears on (the law of diminishing returns).
Other Examples:
More generally, If $r>0$ is a rational number, then
then if the degree of q exceeds that of p, there is a horizontal asymptote, and the value of the asymptote is given by examining the approximating function given by the ratio of leading terms alone.
This is called a "slant asymptote" (not a horizontal asymptote, for obvious reasons! If you get far from the origin, then the difference between the two functions falls away.
We can then replace the more complicated with the simpler.
We use this idea in physics all the time: we assume that gravity is constant at the surface of the Earth. In fact, it varies as distance to the center of the Earth, but we're so far away that we can take this as a constant (its value at about 4000 miles -- our distance to the center of the Earth). We're far enough from the origin (the center of the Earth) that we treat acceleration due to gravity as locally constant.
We can say, however, that $\infty*\infty=\infty$, that $\infty*1=\infty$, that $\infty/1=\infty$, etc. So some of the usual rules apply (and hopefully make sense!).
This is just one type of asymptotic behavior that is sometimes useful. In fact, as mentioned in the previous section, every rational function approaches a polynomial in its end behavior, so that we're interested here in those rational functions (and some others) which approach linear functions as x gets large.
E.g.,
Or even non-rational functions, such as
These help to reduce the amount of work we have to do.
Use anything that you know about the form of the function to help inform your graph (e.g. if you know it's cubic, then you already have a good idea what it's going to look like).
If your function is periodic, then you only need to sketch it on one period.