This set is due Friday, March 26.
- The taxicab norm on
is defined by setting
where
Show that this is indeed a norm. As usual, we can define a distance function by setting
Find 2 non-congruent, non-degenerate triangles with sides of length 1, 1, and 2.
- This exercise is related to an 80-year old open problem of Paul Erdös. Consider a unit square
. Inscribe in
exactly
squares with no common interior point. (The squares do not need to cover all of
.) Denote by
the side lengths of these squares, and define
Show that
, and that equality holds iff
is a perfect square.
(Erdös problem is to find all
for which
. Currently, it is only known that
for all
,
,
, and that if
, then
is a perfect square.)
- (This exercise comes from Jerry Shurman, Geometry of the quintic, Wiley-Interscience, 1997.)A rigid motion of
is a function
such that
for all vectors
(Here,
is the usual inner product on
.) The goal of this exercise is to show that these maps are precisely the functions of the form
where
is an orthogonal matrix and
.
- By definition, a
matrix
with real entries is orthogonal iff
where
is the transpose of
. Show that this is equivalent to stating that
preserves inner products, in the sense that
for all
.
- Show that if
where
is orthogonal, then
is indeed a rigid motion.
- To prove the converse, assume now that
is rigid.
- Show first that
is a bijection.
- Let
and set
Eventually, we want to show that
is a linear transformation. Begin by checking that
and that
for all
.
- Show that
for all
, and conclude that
preserves addition.
- Argue similarly that
preserves scalar multiplication, and is therefore linear.
- It follows that
for some matrix
. Conclude the proof by checking that
is indeed orthogonal.
- Show first that
- By definition, a
- Solve exercises 2-7, 10-14 from Chapter 6 of the textbook.
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Dr. Caicedo,
On question #1, v_1 and v_1 are vectors right? The sum of their magnitudes gives another vector’s length… bold v. I’m just verifying that they’re not scalars…
Also, #2: the max of a sum… does that mean that you take the largest value for the possible sums?
I apologize, I meant v_1 and v_2 on my first question.
Thanks,
Amy
Hi Amy,
1. What I meant was
is a vector in
It therefore has two coordinates (with respect to the standard basis), and I am calling the first
and the second
(So, yes,
are scalars.)
2. Yes, that is what I meant, the maximum (or sup, perhaps) is taken over all possible sums.
Hey Dr. Caicedo,
.
I think you meant to say in your last comment that
Nick
[*Sigh* Yes, thanks. Corrected. -A]
We have not defined “non-congruent” yet. Are we talking about using the standard distance measure and using trig to show they have different angle measures?
Let’s be as generous as it is reasonable, and take congruent to mean same lengths, angles, areas. What I mean is, we want two “obviously different” triangles whose sides have the same lengths nonetheless. (And non-degenerate is intended to eliminate the example of a segment with a point in the middle.)
Dr. Caicedo,
In the assigned problem 3 #5, To show A is orthogonal, do we prove A^T(A)=I? If so, these two matrices can get very messy with 3X3 real entries… is there another way?
On Assigned problem 3 #1, what is required to show 1 to 1 and onto here?
Thanks,
Amy
Hi Amy,
For 3.5, do you have another characterization of orthogonality? (Perhaps one proved earlier somewhere in problem 3?)
I am not sure I understand your question about 3.1. Can you tell me what you mean?
Hi, I am not sure how to show R is a bijection. I suppose I am still unclear what a rigid motion is. I keep going through the motions of showing one thing after another, but am not sure what the big picture is for R.
Thanks,
Amy
The definition of being rigid is the equation at the beginning,
for all 
What do you get if
? This says that
preserves distances. It implies (very easily) that
is 1-1 and that it is continuous.
You may remember from vector calculus that
where
is the angle between the vectors
and
. Since
preserves distances, the equation defining rigid motions then says that the angle between
and
is the same as the angle between
and 
In other words: Rigid motions preserve distances and angles. That is what a rigid motion is: A continuous transformation of
with those two properties.
I’ll write about surjectivity a bit later.
The most direct argument for surjectivity that I have thought of is as follows; there are several claims I make along the way that need to be justified, of course, but this is the skeleton:
Let
we want to find some
such that
Pick points
in the range of
say 
Consider the tetrahedron
There are only two tetrahedrons in
that are congruent to
and have
corresponding to
Say,
and
Then
must be the image of either
or 
A better layout of the exercise would have been to show first that
preserves inner products and then show that
bijects. To show that
surjects one could also work in coordinates:
Let
be the standard orthonormal basis in
Since
for all
with
and
then
is an orthonormal basis.
Next,
for any vector
and 
So to make
hit any point, express the point as 


Then let
Then
Maybe this immediately shows that
is linear, further shortening the exercise?
HTML ate my inner product symbols.
[Edited: I fixed it. Thanks! -A.]
Hi Jerry,
Thanks a lot!
Very neat solution. The solution I suggested above and the one below depend a bit too much on geometric ideas that don’t seem relevant to the problem, so I like your approach much better.
There are a few statements that probably need more details (if this were to be turned in as homework), but this is really an effective proof.
Thanks for sharing.
Here is another way of proving surjectivity. It was suggested by my friend and colleague Ramiro de la Vega. I think that Dr. Shurman‘s solution above is the best one, but all the solutions we have exhibit different ideas which may prove useful in different contexts.
For this approach, first prove that the image under
of a straight line is a straight line. This is the key observation.
Surjectivity is now easy: Show now that the image under
of a plane is a plane. For this, consider three noncollinear points in a plane
and note that
is the union of the lines that go through one of these three points and the opposite side in the triangle they determine.
Finally, consider a tetrahedron, and note that any point in space is in one of the lines going through a vertex and the opposite face.