Understanding the Fibre Bundle Structure of Mobius Band

In summary, the Mobius band has a base space, a fibre, and a bundle, but there is no natural unique homeomorphism of Yx with Y. There are two ways to map Yx to Y and one of them is the "wrong way up". The group G is the cyclic group of order 2 generated by g.
  • #1
rbwang1225
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I don't understand the fibre bundle structure of the Mobius band, described by my textbook.
"The base space ##X## is a circle obtained from a line segment L as indicated in Fig. by identifying its ends. The fibre ##Y## is a line segment. The bundle ##B## is obtained from the product ##L \times Y## by matching the two ends with a twist.
[The projection ##L \times Y \rightarrow L## carries over under this matching into a projection ##p: B \rightarrow X##. Any curve as indicated with end points that match provides a cross-section. Any two cross-sections must agree on at least one point. There is no natural unique homeomorphism of ##Y_x## with ##Y##. There are two such which differ by the map ##g## of ##Y## on itself obtained by reflecting in its midpoint. The group ##G## is the cyclic group of order 2 generated by ##g##.]"
What I don't understand are in brackets.
Could someone help me to clarify more clearly?
Regards.
 
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  • #2
hi rbwang1225! :smile:
rbwang1225 said:
[The projection ##L \times Y \rightarrow L## carries over under this matching into a projection ##p: B \rightarrow X##.

L is the flat unjoined-up base-line, X is the circle base-line.

p is the projection that just "drops" any curve in B (not necessarily stretching all the way round) onto the circle, X
There is no natural unique homeomorphism of ##Y_x## with ##Y##. There are two such which differ by the map ##g## of ##Y## on itself obtained by reflecting in its midpoint.

Yx is the vertical line above the point x on the circle X

mapping Yx onto the "original" Y (or onto any Yx') can be done in only two topologically different ways … the "right way up", and the "wrong way up" :wink:

g is the map which turns Y the wrong way up (so g2 is the identity)
The group ##G## is the cyclic group of order 2 generated by ##g##.]

G is the group {I,g} with g2 = I :smile:
 
  • #3
tiny-tim said:
hi rbwang1225! :smile:


L is the flat unjoined-up base-line, X is the circle base-line.

p is the projection that just "drops" any curve in B (not necessarily stretching all the way round) onto the circle, X


Yx is the vertical line above the point x on the circle X

mapping Yx onto the "original" Y (or onto any Yx') can be done in only two topologically different ways … the "right way up", and the "wrong way up" :wink:

i don't understand this. as i see it, we have no way of telling which way is "up", we just have two ways to map Yx to Y. "g" isn't one of them, it transforms one homemorphism into the other.

g is the map which turns Y the wrong way up (so g2 is the identity)


G is the group {I,g} with g2 = I :smile:

does G = Aut(Y)?
 
  • #4
Hi Deveno! :smile:
Deveno said:
i don't understand this. as i see it, we have no way of telling which way is "up", we just have two ways to map Yx to Y.

"up" is whatever we choose to call it o:)
"g" isn't one of them, it transforms one homemorphism into the other.

i didn't say g was from Yx to Y, I said it was from Y to Y,

which is the way it is defined in the textbook …
"There are two such which differ by the map g of Y on itself obtained by reflecting in its midpoint."​

does G = Aut(Y)?

pass :redface:
 
  • #5
tiny-tim said:
Hi Deveno! :smile:


"up" is whatever we choose to call it o:)


i didn't say g was from Yx to Y, I said it was from Y to Y,

which is the way it is defined in the textbook …
"There are two such which differ by the map g of Y on itself obtained by reflecting in its midpoint."​



pass :redface:

gotcha, g reflects Y.

my point about "up" is, there is no such thing on a mobius band. we can't orient it. there's just one way and another way, and we can't even decide on "choosing a convention". i mean if U is a neighborhood of x in X, then p-1(U) has "2 sides" but B only has 1
(locally flat, but globally twisted).

if I'm thinking about this right, it's like we have a cylinder antipodally identified like the sphere is with the projective plane. each fiber is "both versions" of the line Y, one is reflected about the circle X, but we honestly can't say "which is which".

by Aut(Y), i mean of course, the group of homeomorphisms Y→Y. strictly speaking, there ought to be more than just 2 (we could "stretch Y in the middle, and shrink it by half the amount we stretched at each end"), so maybe they ought to be isometries, i dunno.
 
  • #6
Deveno said:
my point about "up" is, there is no such thing on a mobius band …

ah, but my "up" was on Y :wink:
 
  • #7
One can think of the Moebius band as the quotient of the cylinder by the action of Z2 which sends a point (x,t) to the point (x + pi, -t) where the cylinder is viewed as the Cartesian product of a circle with the interval, (-1,1).

This action shows that the Moebius band is a flat Z2 bundle over the circle.
As such, it is defined with two coordinate charts and the transition function, t-> -t.

This action of Z2 is an isometry of the flat cylinder, (the cylinder that is made from a sheet of paper by taping opposite edges together), so the Moebius band is a flat Riemannian surface. Parallel translation of a vector that points along the fiber interval around the central circle returns the vector to its negative. Equivalently, parallel translation of an othonormal frame around the circle returns it to an orthonormal frame with the opposite orientation. This shows that the holonomy group of the flat Moebius band is Z2.

When one makes a real Moebius band out of paper, it becomes a flat Riemannian manifold that is realized in space. Since it is still flat i.e. it still has a flat geometry when realized in space, parallel translation of that same orthonormal frame around the central circle still reverses orientation. Now add one more vector perpendicular to the Moebius band to create a 3 vector orthonormal frame. Do the parallel translation again. In space, parallel translation of a 3 vector frame around any curve preserves its orientation. But one of the vectors along the Moebius band is reflected, so the normal vector must also be reflected. Thus there is no idea of up and down normal to the Moebius band in space.

The Klein bottle is similar to the Moebius band. It is the quotient of a flat torus by the action of Z2 that rotates the first coordinate circle by 180 degrees and reflects the second coordinate circle along an axis.

So the Klein bottle is a flat circle bundle over the circle with structure group Z2. The same parallel translation argument holds and the holonomy group of the flat Klein bottle is Z2.

If instead of reflecting about an axis, you multiply the second coordinate circle by -1, you get another flat Z2 bundle over the circle. So here is a question. Is this a trivial Z2-bundle?
 
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  • #8
Deveno said:
does G = Aut(Y)?
Actually, I don't understand this notation "Aut(Y)"
 
  • #9
Sorry for forgetting to put the figure.
mobius torus.jpg
 
  • #10
BTW: The intermediate value theorem tells you that any two cross sections of the Mobius band have to meet at least one point.
 
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  • #11
Aut(Y) denotes the group of automorphisms on Y. That means that it's the set of all isomorphisms from Y into Y.
 
  • #12
rbwang1225 said:
Actually, I don't understand this notation "Aut(Y)"

This answers your own post:

"There is no natural unique homeomorphism of Yx with Y. There are two such which differ by the map g of Y on itself obtained by reflecting in its midpoint. The group G is the cyclic group of order 2 generated by g.]"


This is what Aut(Y) is in this case.
 

FAQ: Understanding the Fibre Bundle Structure of Mobius Band

What is a Mobius band?

A Mobius band, also known as a Mobius strip, is a non-orientable surface with only one side and one edge. This means that it has no distinct top or bottom and the surface curves back onto itself seamlessly.

What is the fibre bundle structure of a Mobius band?

The fibre bundle structure of a Mobius band is a mathematical concept that describes the way in which the band is constructed. It consists of a circle (the base space) and a line (the fibre) that is wrapped around the circle in a twisted manner.

How is the fibre bundle structure of a Mobius band different from other surfaces?

The fibre bundle structure of a Mobius band is unique because it has a non-trivial fibre bundle structure. This means that the fibre does not simply run parallel to the base space, but rather twists and turns in a complex manner, creating a non-orientable surface.

How does understanding the fibre bundle structure of a Mobius band benefit science?

Understanding the fibre bundle structure of a Mobius band has many practical applications in various fields of science, such as physics, chemistry, and mathematics. It can be used to model and understand complex phenomena, and has been applied in fields such as fluid dynamics, electromagnetism, and quantum mechanics.

Can the fibre bundle structure of a Mobius band be generalized to other surfaces?

Yes, the concept of a fibre bundle structure can be applied to many other surfaces, not just the Mobius band. In fact, understanding the fibre bundle structure of different surfaces has been a topic of interest and research in mathematics and physics for many years.

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