Math 110.107, Calculus II (Biological and Social Sciences)
Fall 2010 Course Lecture Synopses
Week 11: November 8 through November 12
http://www.mathematics.jhu.edu/brown/courses/f10/107.htm
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MWF 10:00am - 10:50am Krieger 205 |
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403 Krieger Hall |
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410-516-8179 |
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Office Hours:
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1:00-2:00 pm |
by appt. other times |
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W |
1:00-2:00 pm |
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Below is some basic information pertaining to the lectures of this course. I will update this page after each lecture or two to benefit both the students in their attempts to organize the material for the course, and the TAs so that they know what material I covered and how it was covered. Please direct any comments about this page to me at the above contact information. |
· Monday, November 8:
· Wednesday,
November 10: Today, I talked about
another type of equilibrium solution at the origin for the system
. Suppose
has complex
eigenvalues (remember this means that the quadratic formula used to solve the
characteristic equation has negative discriminant. In this case, like in the case we did on
Monday, the two eigenvalues are distinct, but are not real (they are complex
conjugates
). This presents a problem because the
eigenvectors (the vector solutions to
) will also not
be real. It turns out, though that the
eigenvectors can be solved for in the usual way, and they are also complex
conjugates of each other
. This is a
problem because the solutions to a system of real differential equations must
also be real. They are, but must be
constructed in a different way. The book
does not construct the solutions.
Instead, they simply go back into the slope field to “see” the solutions.
Then they discuss the oscillatory nature of the solutions by graphing each
solution separately. I do not like this,
so I constructed the solutions explicitly.
Using the data above, I wrote out the solutions as
. I then
analyzed this solution for clues as to what is going on in the slope field
where the solutions live. First, only
the
-value really
determines whether solution collapse into the origin, or move away from
it. Second, the
-value ensures
that the sines and cosines make the solutions oscillate. They also make sure that there is NO straight
line motion along eigendirections like in the case we developed in the last
class. Using many examples in JODE on
the projector, we studied the cases for
(the stable
spiral or the spiral sink),
(the unstable
spiral or the spiral source), and
(the center,
also stable but solutions do not collapse to the origin. Then for the last part of the class, I
introduced Chapter 12 with a little bit of lighthearted probability, counting,
and why one would need calculus to do probability.
· Friday,
November 12: Today, we learned how to
count, with three counting principles of counting from Section 12.1. The first was the idea that for an experiment
consisting of many tasks performed in order, the total number of possible
outcomes is the product of the total number of outcomes for each task. With examples like, flipping coins, tossing
dice, playing cards and arranging pictures on a wall, we went through many
examples. The second is the idea of a
permutation, a choice and arrangement of a subset of objects from another
set. The key to a permutation is that it
is an ordered subset of objects out of
total
objects. When the arrangement or order
of the choosing matters, the counting is called a permutation, and the total
number of permutations of the
objects out of
is given by
. We also went
over the definition of the factorial used here.
The last principle we talk about was how to choose
objects out of
when the order
of the choosing does not matter. One can
count by again using the total number of permutations, but one must then
discount the total by the number of ways one can arrange the subset of
objects. There are exactly
ways to arrange
objects. These
are called combinations and the total number of ways one can choose
objects out of
when order does
not matter is
. Again, we
went through many examples.