Diam A = diam Cl(A) in metric space

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Discussion Overview

The discussion revolves around proving that in a metric space (X, d), the diameter of a subset A equals the diameter of its closure Cl(A). Participants explore various approaches to this proof, considering different properties of open and closed sets, and the implications of the definitions of diameter.

Discussion Character

  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • One participant suggests that if A is closed, the equality is trivial, but if A is open, they express uncertainty about how to proceed.
  • Another participant argues that A may not be open or closed, and introduces the idea of using a sequence of points to represent the diameter of Cl(A) to establish a lower bound for the diameter of A.
  • A participant proposes that if A is a nonempty bounded subset, they can use the properties of open and closed balls to show that diam A = diam Cl(A) by establishing bounds.
  • Another participant emphasizes the importance of the supremum definition of diameter and questions the assumption that A is open, providing a counterexample.
  • Some participants suggest using the triangle inequality with points from the closure and their corresponding points in A to derive upper bounds on distances.
  • A later reply summarizes a successful approach using open balls around points in Cl(A) to show that the diameter of Cl(A) is bounded by diam A, leading to the conclusion that diam A = diam Cl(A).

Areas of Agreement / Disagreement

Participants express differing views on the assumptions regarding the openness or closedness of A, and there is no consensus on a single approach to the proof. Multiple competing ideas and methods are presented throughout the discussion.

Contextual Notes

Some participants note the limitations of assuming A is open or closed without justification, and the discussion reflects varying interpretations of the properties of metric spaces and their subsets.

radou
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As the title suggests, I have to prove, if (X, d) is a metric space, that for any subset A of X, diam A = diam Cl(A), i.e. the diameter of A equals the diameter of its closure.

So, if A is closed, it is trivial, since Cl(A) = A. Assume A is open. Now I'm a bit lost.

If A is open in (X, d), then it is a union of open balls in X. By the way, I know that for every open ball K(x, r) in X, diam K = diam Cl(K). Also, I have shown that Cl(A) can be written as a union of closed sets in X (since the closure of a union equals the union of closures).

Also, I know that, since A is a subset of Cl(A), diam A <= diam Cl(A) must hold.

And also, I know that for subsets A, B of X, diam (A U B) <= diam A + diam B + d(A, B), which can be generalized for any finite number of subsets.

The definitions of diameters didn't get me anywhere, too.

For some reason, I can't make any use of these facts to prove it. Any suggestion?
 
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You can't just assume A is open. More likely it is neither open nor closed.

The diameter of Cl(A) can be represented by a sequence (xn,yn) of points such that d(xn,yn) converges monotonically to the diameter. See if you can hijack this sequence to find a lower bound on the diameter of A
 
Could you tell me some more about this sequence? I'm not exactly sure how to construct it.

By the way, here's another idea. Let A be a nonempty bounded subset of X, so diam A = r. Then there exists some point x from A such that A is contained in the open ball K(x, r/2) of diameter r. But then the closed ball K[x, r/2] has a diameter r, too. Clearly Cl(A) is contained in K[x, r/2] (since if y were from X\K[x, r/2], which is open, there would exist a neighborhood of y which does not intersect A), so diam Cl(A) <= diam K[x, r/2] = r = diam A, which, when combined with diam A <= diam Cl(A), gives diam A = diam Cl(A).
 
radou said:
Could you tell me some more about this sequence? I'm not exactly sure how to construct it.

If B is a subset of a metric space:

diam(B)=sup\{d(x,y)|x,y\in B \}.

For a number to be a supremum of a set, it means that it is the least upper bound. So there has to be a sequence of distances in B that converge to the supremum.. those distances are based on pairs (x,y)

Let A be a nonempty bounded subset of X, so diam A = r. Then there exists some point x from A such that A is contained in the open ball K(x, r/2)

First, it should be the closed ball you're looking at. You seem to be under the impression that A is open, and it isn't,. As an example, look at the set A=[0,1].

Also, the middle of this set does not have to exist. If your metric space is just the points {0,1/4,3/4,1} and A={0,1} you can't even find a center for A inside of the metric space, let alone inside of A
 
Another option: Let x,y be arbitrary points in the closure and consider two small open balls around them. They contain points x',y' in A. Use those points and the triangle inequality to get an upper bound on d(x,y).
 
Fredrik said:
Another option: Let x,y be arbitrary points in the closure and consider two small open balls around them. They contain points x',y' in A. Use those points and the triangle inequality to get an upper bound on d(x,y).

Thanks, I think I got it now.

Let x, y be from Cl(A). Then, for any ε > 0, there exist open balls K(x, ε) and K(y, ε) which intersect A. Let x' and y' be points from these intersections, respectively. d(x, y) <= d(x, x') + d(x', y') + d(y', y) < 2ε + d(x', y') <= 2ε + diam A. So, for every x, y from Cl(A), d(x, y) <= diam A. Since diam Cl(A) is the least upper bound for the set {d(x, y) : x, y from Cl(A)}, and diam A <= diam Cl(A), we conclude that diam A = diam Cl(A).
 
Perfect. That's exactly what I had in mind.
 

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