Infinite cylinder covered by a single chart

In summary: No, because the map has to be a smooth map. It can't just be a function that takes a single point and outputs a single point.In summary, the author is trying to figure out how to construct a mapping from an open subset of a manifold to an open set in a different coordinate space so that the chart covers the entire manifold.
  • #1
Figaro
103
7

Homework Statement


This is a problem from Spacetime and Geometry by Carroll,

Just because a manifold is topologically nontrivial doesn't necessarily mean it can't be covered with a single chart. In contrast to the circle ##S^1##, show that the infinite cylinder ##RxS^1## can be covered with just one chart, by explicitly constructing the map.

Homework Equations

The Attempt at a Solution


Based on my understanding, a chart is a mapping from an open subset ##U## of a set ##M## to ##R^n## such that the image of ##U## is an open set in ##R^n##.

From my searches, I've came across that I can use the annulus as the open subset because it is homeomorphic to the infinite cylinder, but how do I define/construct the mapping? I think there are a lot of ways?
 
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  • #2
Map each line on the cylinder that runs parallel to the cylinder's axis of rotation, to a radial line in the annulus. Then set units along that radial line by parameterizing it in such a way that one approaches but never reaches the outer (inner) circumference of the annulus as ##t\to\infty## (##t\to-\infty##). The parameter ##t## can represent signed distance along the line on the cylinder from an arbitratily chosen starting point.
 
  • #3
andrewkirk said:
Map each line on the cylinder that runs parallel to the cylinder's axis of rotation, to a radial line in the annulus. Then set units along that radial line by parameterizing it in such a way that one approaches but never reaches the outer (inner) circumference of the annulus as ##t\to\infty## (##t\to-\infty##). The parameter ##t## can represent signed distance along the line on the cylinder from an arbitratily chosen starting point.
Thanks for that but I just want to know, since the cylinder is made out of infinite circles stacked together, why is that the ##S^1## (circle) can at least be covered by two charts while the cylinder can be covered by one chart? Aren't they similar? For the circle, one round trip [0, 2π] certainly will be a closed set, so some people use two charts with domain (-π, π) and (0, 2π). Shouldn't the annulus method be valid also for the circle? So is there a general way of identifying how to construct a mapping such that, say one chart (as in this case) can cover the manifold (aside from the annulus method)?
 
  • #4
Figaro said:
why is that the ##S^1## (circle) [requires] at least ... two charts while the cylinder can be covered by one chart?
Because ##S^1## is one-dimensional whereas the cylinder is two-dimensional. The chart has to map to a subset of Euclidean space of the same number of dimensions, and Euclidean 2-space contains circular subsets whereas Euclidean 1-space does not.
Shouldn't the annulus method be valid also for the circle?
No, because the annulus method maps the (cylindrical) manifold to a subset of ##\mathbb R^2## and a chart of ##S^1## must map into ##\mathbb R^1## instead.
So is there a general way of identifying how to construct a mapping such that, say one chart (as in this case) can cover the manifold (aside from the annulus method)?
No. Classifying manifolds is hard. There is no simple, general rule.
 
  • #5
andrewkirk said:
Because ##S^1## is one-dimensional whereas the cylinder is two-dimensional. The chart has to map to a subset of Euclidean space of the same number of dimensions, and Euclidean 2-space contains circular subsets whereas Euclidean 1-space does not.
No, because the annulus method maps the (cylindrical) manifold to a subset of ##\mathbb R^2## and a chart of ##S^1## must map into ##\mathbb R^1## instead.
No. Classifying manifolds is hard. There is no simple, general rule.
Can I set the inner radius to 0 such that I have the map ##φ: U(θ, z) → R^2~~~## where ##φ(U) = (θ, e^z), ~~~ -∞ < z < ∞, ~0≤θ<2π##

But I know ##0≤θ<2π## is not open, what do you think?
 
  • #6
That works. The image of that chart is a pierced plane not an annulus, but that's OK because Carroll's question doesn't specifically ask for an annulus. If you really wanted an annulus you'd need to use a function that is bounded above. One that works nicely is arctan (the logistic function is another).
It doesn't matter that ##[0,2\pi)## is not open. What has to be open is the domain of the chart, not necessarily all coordinate slices thereof.
 
  • #7
andrewkirk said:
That works. The image of that chart is a pierced plane not an annulus, but that's OK because Carroll's question doesn't specifically ask for an annulus. If you really wanted an annulus you'd need to use a function that is bounded above. One that works nicely is arctan (the logistic function is another).
It doesn't matter that ##[0,2\pi)## is not open. What has to be open is the domain of the chart, not necessarily all coordinate slices thereof.
So you mean the map ##φ: U(θ, z) → R^2~~~## where ##~φ(U) = (θ, arctan(z)), ~~~ -∞ < z < ∞, ~0≤θ<2π##
But doesn't that mean any function would work as long as it is bounded above and below?

So the cartesian product of a half open and open set is open? Hmmm...
 
  • #8
Figaro said:
So the cartesian product of a half open and open set is open?
No.
The Cartesian product specifies only the sets, not the topology, so that statement has no meaning. One can put either a topology on the Cartesian product that makes the set open, or one that makes it half open. The product topology would make it half open, but the product topology is different from the subspace topology that the image inherits from ##\mathbb R^2## in this case.
 
  • #9
andrewkirk said:
That works. The image of that chart is a pierced plane not an annulus, but that's OK because Carroll's question doesn't specifically ask for an annulus. If you really wanted an annulus you'd need to use a function that is bounded above. One that works nicely is arctan (the logistic function is another).
It doesn't matter that ##[0,2\pi)## is not open. What has to be open is the domain of the chart, not necessarily all coordinate slices thereof.
##[0, 2π )~## doesn't cover a whole circle, so if the given problem is a ##S^1## (circle), this would pose a problem since it doesn't cover the whole so we need to add another chart just to cover the "hole". But in this case, it is an infinite cylinder, so ##[0, 2π )~## being not open doesn't matter because ##-∞<z<∞## is open, so the domain will be open? Is this what you are pointing out?
 
  • #10
Figaro said:
[0, 2π ) doesn't cover a whole circle
It doesn't?
 
  • #11
haruspex said:
It doesn't?
Yes, it doesn't, 2π is not included.
 
  • #12
Figaro said:
Yes, it doesn't, 2π is not included.
The circle is covered by the following map ##f##, whose domain is ##[0,2\pi)##. Here the circle ##S^1## is considered embedded in ##\mathbb R^2## as the circle of unit radius centred on the origin.

##f## is the map from ##[0,2\pi)## to ## S^1## such that ##f(\theta)## is the point in ##\mathbb R^2## whose polar coordinates are ##(1,\theta)##. This map is surjective onto ##S^1## and in that sense 'covers' it. The point that would be ##f(2\pi)## if ##2\pi## were included in the domain is already covered by ##f(0)##.

The reason why ##S^1## is not homeomorphic to ##[0,2\pi)## is not that there is no 'covering' map but rather that the inverse of ##f## is not continuous.
 
  • #13
Figaro said:
Yes, it doesn't, 2π is not included.
How is the 0 point on the circle different from the 2π point?
 
  • #14
haruspex said:
How is the 0 point on the circle different from the 2π point?
Sorry, what I mean to say, it is not going to return to the original point, it just keeps getting closer but not exactly so in a sense it doesn't cover all? It is like running in an Olympic circle starting from the START but when you almost ran a full circle, you don't reach the START but just keep getting closer.
 
  • #15
Figaro said:
Sorry, what I mean to say, it is not going to return to the original point, it just keeps getting closer but not exactly so in a sense it doesn't cover all? It is like running in an Olympic circle starting from the START but when you almost ran a full circle, you don't reach the START but just keep getting closer.
In that analogy, the runner does not need to reach the start line since the runner has already been there.
All that is required is that for any given point on the circle there is a point in [0, 2π) that maps to it.
 
  • #16
haruspex said:
In that analogy, the runner does not need to reach the start line since the runner has already been there.
All that is required is that for any given point on the circle there is a point in [0, 2π) that maps to it.
Oh, fair enough, thanks for the clarification.
 
  • #17
I believe a simple chart is the following: (xe^z, ye^z)
 
  • #18
keithdow said:
I believe a simple chart is the following: (xe^z, ye^z)
Which is a specific example of the general method laid out in post #2.
By the way, the thread is two years old.
 

1. What is an infinite cylinder covered by a single chart?

An infinite cylinder covered by a single chart is a mathematical concept used in differential geometry to represent a cylindrical surface that extends infinitely in both directions. It is called a "single chart" because it can be described using only one coordinate system.

2. How is an infinite cylinder covered by a single chart different from a regular cylinder?

An infinite cylinder covered by a single chart is different from a regular cylinder because it extends infinitely in both directions, whereas a regular cylinder has a finite length. Additionally, a single chart can be used to describe the entire surface of the infinite cylinder, while a regular cylinder may require multiple charts to fully describe its curved surface.

3. What is the purpose of using a single chart to represent an infinite cylinder?

The purpose of using a single chart to represent an infinite cylinder is to simplify the mathematical calculations and equations involved in studying the cylindrical surface. By using a single coordinate system, it becomes easier to analyze and understand the geometric properties of the infinite cylinder.

4. Can an infinite cylinder covered by a single chart exist in the physical world?

No, an infinite cylinder covered by a single chart is a mathematical concept and does not exist in the physical world. It is a useful tool for theoretical and mathematical analysis, but it cannot be physically constructed.

5. What other mathematical concepts are related to an infinite cylinder covered by a single chart?

An infinite cylinder covered by a single chart is related to other mathematical concepts such as differential geometry, coordinate systems, and curvature. It is also connected to other geometric shapes, such as a cone or a sphere, which can also be represented using a single chart.

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