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The appropriate way to solve this problem is by using the alternating
series error bound. We did this in class, and it was fairly quick and
straightforward.
However, we encountered difficulty when a few students asked (innocently)
what would be involved in using the Lagrange form of the remainder. I said,
“Believe me, it’s a lot more work,” and then instead of moving on, I unwisely
plunged right in and entered a festering swamp.
The problem can be solved using the
Lagrange form, but you need to consider the situation more carefully than I
did in class.
Let f (x) = sin 2x. Clearly Mn =
2n is an upper bound for
the magnitude of the nth
derivative, regardless of the value of the argument.
It may help, when visualizing the problem, to write out several terms of the Maclaurin series for f
(x), namely
f (x) = f (0) + f ˘(0) · (x – 0) + f ˘˘(0)/2!
· (x – 0)2 + f ˘˘˘(0)/3! · (x – 0)3 + . . .
Because of the way the derivatives of sin 2x work out, every even-degree term of this series is actually 0,
and because x < 0 (given), the
odd-degree terms are all nonzero.
Since we are to use 5 nonzero terms (given), the Maclaurin
term involving x9 is the
last nonzero one that we are using. Since the Maclaurin
term involving x10 is 0,
we have a choice for our Lagrange error bound of using either or
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We prefer the latter, since by inspection, the Lagrange
error bound using M11
will be smaller.
But just for fun, let’s go ahead and compute both error bounds. Using the
hints provided on the board (310 < 60,000 and 10! > 3.6
million) and no calculator, we have

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