News from MAST
Hello from MAST! I have gotten
some good responses to my request for email! Thanks for the suggestions,
keep them coming. I am always on the lookout for good material for
future columns.
This week I will discuss
a rather remarkable development in mathematics and physics. Without
this development it is not really possible to discuss physics in any
substantial way.
Frames of Reference
Last week we developed
an intuition about time. We even managed to define time as a clock
reading assigned to something that happens (in our case, an object
moved). What good does that do us? Without some way to combine time
and distance into a single entity, it is not very easy to use these
concepts. When we do combine these ideas (he said, encapsulating something
like two thousand years worth of fascinating research into a sentence)
we come up with a truly remarkable concept.
When an object moves its
path is called a trajectory. Each point on the trajectory represents
the position of the object corresponding to a position on a time line.
Recall that in a previous column, I wrote about functions. In this
case we can view position as a function of time! This realization
paves the way for rapid advance in the study of motion. First of all
this realization allows us to represent the position of an object
with a formula. Secondly, it allows us to represent this formula graphically
as a graph (or plot) with the independent variable (in this case time)
as the horizontal axis (or abscissa) and the dependent variable
(in this case position) as the vertical axis (or ordinate).
So long as the origin (or reference point) of both the position line
and the time line are chosen to intersect we have developed what is
called a frame of reference. In a future column I will discuss
how we can view the world from different frames of reference at the
same time (in fact we have no choice in this!)
Let's look at a specific
example of this. Say that we measure the position
of an object with respect to time
. Let
us also say that we are observing the motion of a ball hanging from
a perfect spring (that is we can neglect both friction and gravity).
After analyzing the data we determine that a formula describes the
motion,
![[Graphics:art/index_gr_3.gif]](art/index_gr_3.gif)
We can then make a plot
of this motion.
![[Graphics:art/index_gr_4.gif]](art/index_gr_4.gif)
The ability to treat the
position of an object as a function only of time is a truly awesome
conept and is very subtle in its implications. The development of
this concept in history is both fascinating and completely eclipsed
by the apparent simplicity of the concept. We look at this statement
and say, "Of course, how could it be otherwise?" But we
see in the history of this concept that it is anything but obvious.
It opens to us all of the tools of calculus to attack the problem
of describing the motion of an object. That is what we will do next.
Theory Challenge Answer
for Last Week's Column
The subject of this column
is, in effect, the answer to last week's Theory Challenge. Here I
will simply put it in a more formal language.
If we assign a set to describe
the position line of a moving object we note that the domain is the
entire set of real numbers. Perhaps I will explore the properties
of the set of real numbers in another column (a thing I should do,
since there is no reason for you to believe that this is a reasonable
statement otherwise). For now, you will just have to trust me. The
set of real numbers is denoted
.
If we assign another set
to describe the time line, then we find an interesting thing; the
domain is also the set of real numbers
.
Recall from the column
on functions that a function relates the independent variable to the
dependent variable (in this case time to position). This creates a
set of ordered pairs
where for every
there exists a unique value for
.
This gives us a Cartesian Product,
![[Graphics:art/index_gr_10.gif]](art/index_gr_10.gif)
Using functional notation
we see that
,
where
describes a rule assigning a unique value of
for the position to every value of
corresponding to time:
![[Graphics:art/index_gr_15.gif]](art/index_gr_15.gif)
The result is the trajectory.
Theory Challenge
Can you justify why position
and time can be considered to be described by the set of real numbers?
Books That I Like
There are two good sources
on this subject:
Josef Honerkamp, Hartmann
Römer (1993), Theoretical Physics A Classical Approach,
Springer-Verlag. Section 2.1 covers the theory challenge in all of
its gory detail, but at a level that assumes mastery of vector analysis
and the linear algebra of vector spaces.
George Hrabovsky (1997),
Kinematics, Lesson 1, Unpublished. Notes for the development
of a MAST course in physics that is in development for publication
on the MAST website. 
Converted by Mathematica
November 7, 2001