How can a funnel be both paintable and unpaintable at the same time?

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The discussion revolves around a mathematical paradox involving a funnel-like surface generated by rotating the curve y = 1/x around the x-axis. Participants explore the implications of the finite volume of the funnel versus its infinite surface area, questioning how it can be both paintable and unpaintable simultaneously.

Discussion Character

  • Conceptual clarification, Assumption checking, Exploratory

Approaches and Questions Raised

  • Participants examine the mathematical properties of the funnel's volume and surface area, noting the paradox that arises from the finite volume and infinite surface area. Some question the implications of using paint with a diminishing thickness, while others reflect on the nature of infinite surfaces in mathematical contexts.

Discussion Status

The discussion is active, with various perspectives being shared. Some participants suggest that the paradox can be reconciled through the concept of diminishing thickness of paint, while others introduce related mathematical concepts, such as Gabriel's Horn, to further explore the implications of painting infinite surfaces.

Contextual Notes

Participants note the constraints of physical paint properties and the implications of atomic size, which may limit the ability to paint an infinite surface area despite having a finite volume of paint. There is an ongoing exploration of definitions and assumptions related to the problem.

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NB. first time using Latex so apologies if something came out wrong, I've done my best to double check it.

Consider the curve [itex]y = \frac{1}{x}[/itex] from [itex]x=1[/itex] to [itex]x=\infty[/itex]. Rotate this curve around the x-axis to create a funnel-like surface of revolution. By slicing up the funnel into disks with [itex]r=\frac {1}{x}[/itex] and thickness [itex]dx[/itex] (and hence volume ([itex]\pi r^2 dx[/itex])) stacked side by side, the volume of the funnel is
[itex]V = \int_1^\infty \frac{\pi}{x^2} dx=- \frac{\pi}{x}\mid\int_1^\infty = \pi,[/itex]

which is finite. The surface area however involves the circumferential of the disks, which is [itex](2\pi r)dx[/itex] multiplied by a [itex]\sqrt{1+y'2}[/itex] factor accountng for the tilt of the area. The surface of the funnel is therefore

[itex]A = \int_1^\infty \frac{2\pi\sqrt{1+y'2}}{x} dx > \int_1^\infty \frac{2\pi}{x}dx[/itex]
which is infinite. As the volume is finite but the area is infinite, the funnel can be filled with paint but you can't paint it. Which appears to be a paradox since one should be painting the inside surface when filling up the funnel. But the inside surface=outside surface given the funnel has no thickness.So the question asks me to basically make sense of this paradox, I've done a lot of headscratching over it but thinking logically I simply can't find find our what's going on here, since , having checked over the equations theoretically the statements posed by the question are logical and I see no disconnect, so seems possible but impossible in reality given the paint should be at a constant (visible) thickness which I assume.
 
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Dynamic Change said:
NB. first time using Latex so apologies if something came out wrong, I've done my best to double check it.

Consider the curve [itex]y = \frac{1}{x}[/itex] from [itex]x=1[/itex] to [itex]x=\infty[/itex]. Rotate this curve around the x-axis to create a funnel-like surface of revolution. By slicing up the funnel into disks with [itex]r=\frac {1}{x}[/itex] and thickness [itex]dx[/itex] (and hence volume ([itex]\pi r^2 dx[/itex])) stacked side by side, the volume of the funnel is
[itex]V = \int_1^\infty \frac{\pi}{x^2} dx=- \frac{\pi}{x}\mid\int_1^\infty = \pi,[/itex]

which is finite. The surface area however involves the circumferential of the disks, which is [itex](2\pi r)dx[/itex] multiplied by a [itex]\sqrt{1+y'2}[/itex] factor accountng for the tilt of the area. The surface of the funnel is therefore

[itex]A = \int_1^\infty \frac{2\pi\sqrt{1+y'2}}{x} dx > \int_1^\infty \frac{2\pi}{x}dx[/itex]
which is infinite. As the volume is finite but the area is infinite, the funnel can be filled with paint but you can't paint it. Which appears to be a paradox since one should be painting the inside surface when filling up the funnel. But the inside surface=outside surface given the funnel has no thickness.So the question asks me to basically make sense of this paradox, I've done a lot of headscratching over it but thinking logically I simply can't find find our what's going on here, since , having checked over the equations theoretically the statements posed by the question are logical and I see no disconnect, so seems possible but impossible in reality given the paint should be at a constant (visible) thickness which I assume.

First, you can't fill something mathematically infinite with paint nor paint it.

But, thinking mathematically, you can paint it: you just need a diminishing thickness of paint. Essentialy that is what is happening with the volume. You start with the equivalent of thick paint (filling the funnel) but as you go further from the origin the thickness of the funnel reduces without limit.

You could paint it on the outside - with a finite volume of paint - by copying what you do on the inside.
 
Intriguing. But they have made it seem unfamiliar by taking a 3-dimensional case. If you think of it, in all the integrals
y dx that you have ever done that were finite, the curve in the x, y plane had infinite length.
So it's not a special case and the fact is actually familiar, though still needing some explaining perhaps.

( the ∫ from Σ does not always come out very well I see!)
 
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It's interesting that given paint is made up of atomic particles, it hence has a certain size and so at some point, no paint would be able to fit further down the funnel. Whatever depth this is at, you would have only painted a finite surface area, and so you still have an infinite area that you physically can't paint.
 
If you want to google this, it's called Gabriel's Horn.
 
Here's my take. Let's talk about painting the xy plane. I will suppose we have an infinitely non viscous paint, by which I mean, if a coat of it has any positive thickness, it could be spread over a greater area.

Definition: The plane is painted if given any ##r>0## the disk centered at the origin of radius ##r## is painted.

Theorem: If you have ##m>0## cubic units of paint (the good stuff defined above), that is sufficient to paint the plane.

Proof. Suppose ##r>0##. Apply your ##m## units of paint to the disk of radius ##r## centered at the origin. This can be done since the thickness of the coat is ##\frac m {\pi r^2}>0##. So there is no contradiction, in principle, about painting an infinite surface with a finite volume of paint.

So you could just pour your paint on the origin and let it spread.
 
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