26 October 2001
How Far Have We Gone?
by George E. Hrabovsky, President
of MAST
News from MAST
This week I have begun
the microbiology experiment. The goal is to isolate some harnless
bacteria from soil to do additional research. I will be making stock
cultures of the bacteria I identify.
Continuing from last
week I will continue to develop the principles of motion from
first principles. I will also be answering last week's Theory Challenge.
What is the Distance
an Object Travels?
Last week we discussed
position. We determined that to discover the position of an object
we need to begin by identifying a reference point and then measure
the distance and direction to the object.
I will now expand that
idea to cover the most basic quantity of motion: the distance an object
travels. This quantity is called displacement. Recall our definition
of motion, "The change of position in time." So, all motion
starts with an initial position. We will call this position
.
The motion will end at the final position, we will call this
.
For now we will only think of motion in a straight line. This motion
will give us the line segment
.
This segment is called the displacement. Look at the diagram below,
![[Graphics:art/index_gr_4.gif]](art/index_gr_4.gif)
O is the origin of the
coordinate system we are using to locate
and
.
We can see that this forms a triangle. We can apply the Law of Cosines
to find the length of
:
![[Graphics:art/index_gr_5.gif]](art/index_gr_5.gif)
Assuming we know
and
we can manipulate the equation to get
![[Graphics:art/index_gr_8.gif]](art/index_gr_8.gif)
Thus, by knowing the position
vectors for the initial and final points of motion and the angle between
the two vectors we can find the displacement.
Theory Challenge Answer
for Last Week's Column
This is going to be somewhat
long, I am afraid. Get a pen and paper and follow along. First, I
will introduce some notions from geometry:
- We will understand that
everything is happening in a place. We will call this place a space.
We will make no attempt at this stage to characterize this space.
- This space can have regions
within it that we will call subspaces.
- One such subspace has
no size or shape. This is called a point.
How does the notion of
a point correspond to that of a particle (see the last two columns)?
How does this change the problem of locating the particle? Now that
we have changed the problem of finding the location of a particle
to finding the location of a point within a space, how do we do this?
What is our frame of reference?
This last notion has the seeds for the idea of assigning a reference
point
.
We now recall Euclid's First Postulate:
For every point
and every point
not equal to
there exists a unique line l that passes through
and
.
This line is denoted
.
We now state the formal
definition of a line segment. Definition 1: Any two points,
and
,
and the collection of all points between them, that lie on the line
combine to form a line segment. A segment is denoted
.
![[Graphics:art/index_gr_20.gif]](art/index_gr_20.gif)
We now state the formal
definition of distance. Definition 2: The segment
is called the distance between
and
.
We can measure this distance, which we denote
.
We now state the formal
definition of absolute value. Definition 3: Given a number
x the absolute value of x is x itself
so long as x is greater than or equal to 0; if x is
less than 0 then its absolute value is -x. Symbolically we
write it this way:
![[Graphics:art/index_gr_25.gif]](art/index_gr_25.gif)
We can now state the so-called
Ruler Axiom: For every line there exists a one-to-one correspondence
between the points lying on the line
and the set of real numbers (denoted
)
such that the distance between any two points on
is the absolute value of the difference between the numbers corresponding
to the two points.
From this we can construct
another derive an expression for distance by applying Definition 3
to the Ruler Axiom and then to Definition 2.
![[Graphics:art/index_gr_29.gif]](art/index_gr_29.gif)
To measure this we have
to establish a unit of length, some uniform segment that can be applied
successively. Let us say that this segment is bounded by the points
and
(the segment is thus
).
![[Graphics:art/index_gr_33.gif]](art/index_gr_33.gif)
We next have to find a
point
on
such that
,
![[Graphics:art/index_gr_37.gif]](art/index_gr_37.gif)
We apply the same technique
a second time, finding a second point
such that
.
![[Graphics:art/index_gr_40.gif]](art/index_gr_40.gif)
We continue this process
until we have a set of
equal segments
.=20
![[Graphics:art/index_gr_43.gif]](art/index_gr_43.gif)
And thus the distance
for the segment is then,
![[Graphics:art/index_gr_44.gif]](art/index_gr_44.gif)
Theory Challenge
How did I get the formula,
![[Graphics:art/index_gr_45.gif]](art/index_gr_45.gif)
From the Law of Sines?
Books That I Like
The best book on this
subject is not a physics book:
John Roe (1993), Elementary
Geometry, Oxford University Press. This is particularly a
good book for developing a geometric intuition about physics topics.

Converted by Mathematica
October 24, 2001