Does gravity affect the measurement of pi in non-euclidean geometries?

AI Thread Summary
The discussion centers on the claim that gravity affects the measurement of pi in non-Euclidean geometries, with participants expressing skepticism about this theory. It is clarified that pi is a mathematical constant defined as the ratio of a circle's circumference to its diameter, which remains unchanged regardless of gravitational effects. However, in curved spaces, such as those influenced by gravity, the ratio can deviate from pi due to the geometry of the space. Participants suggest that while pi can be measured accurately in Euclidean space, complications arise in non-Euclidean contexts, but this does not imply that pi itself changes. Overall, the conversation highlights misunderstandings about the nature of pi and the impact of curvature on geometric measurements.
Teresa
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I have heard that while pi is known to many millions, even billions of decimal places, gravity makes it both fundamentally and practically impossible to measure pi to more than 10 significant figures.

I find this to be a very strage theory, and have never heard of it before. I am also finding it difficult to find any information on the area.

Does anyone know of any good websites or books that could help answer this mystery? Or if you know anything on the matter yourself? The question is currently haunting me lol
 
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I think there is a common misunderstanding here. \pi is the ratio of the circumference of a circle to the diameter. \pi is a constant, it does not change.

Now it is true that on a deformed surface this ratio is no longer \pi but that does not mean that \pi is changed.

It is easy to see that the ratio changes if you deform a flat surface. Take a circular piece of clay and stick it on the top of a football, make sure there is no space between the clay and the football. The ratio between the diameter and the circumference is no longer \pi.

Only curvature that deforms changes the ratio. For instance just wrapping the clay around a cylinder does not deform the clay so it does not change the ratio. But sticking it onto a Vietnamese hat deforms it very much, so that means that the ratio changes.

Gravitation curves spacetime, which is like deforming a surface, but then in four dimensions.
 
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Pi isn't pi because we measure it, it is calculated from theoretically perfect geometric shapes.
 
Teresa said:
I have heard that while pi is known to many millions, even billions of decimal places, gravity makes it both fundamentally and practically impossible to measure pi to more than 10 significant figures.

I find this to be a very strage theory, and have never heard of it before. I am also finding it difficult to find any information on the area.

I'm also finding this very strange, I think something important has gotten lost or misrepresented somewhere.

As far as general curvature goes, the ratio of the circumference of a "circle" (a set of points a constant distance away from a central point to it's radius depends on the value of the radius. The error is quadratic in the radius, see for instance

http://en.wikipedia.org/wiki/Curvature

or Misner, Thorne, Wheeler, "Gravitation", pg 336.

This is also discussed somewhat in http://www.eftaylor.com/pub/chapter2.pdf

this is a chapter from one of the coauthors of "Gravitation" that has some of the same material, parts of which are online, and which is much closer to a popular level.The significance of this is not major though - even on the Earth, one can get 10 digits of accuracy for the ratio of circumference /diameter as long as the radius of the circle is less than about 10^-5 of the radius of the Earth - that's about 60 meters.

The extrinsic curvature of [correction]space due to gravity is much less than the extrinsic curvature of the surface of Earth. It depends on how you "slice" space-time into space+time, i.e. what defintion of simultaneity one adopts, as well as one's distance away from a large mass.

It's not quite what you are looking for, but http://www.pitt.edu/~jdnorton/teaching/HPS_0410_2007/Assignments/09_Non_Euc_GR/index.html

may also be helpful about the concept of "curvature" in general relativity,
 
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Teresa said:
I have heard that while pi is known to many millions, even billions of decimal places, gravity makes it both fundamentally and practically impossible to measure pi to more than 10 significant figures.

I find this to be a very strage theory, and have never heard of it before. I am also finding it difficult to find any information on the area.

Does anyone know of any good websites or books that could help answer this mystery? Or if you know anything on the matter yourself? The question is currently haunting me lol
As has been pointed out, \pi, at least the \pi that is "known to many millions, even billions of decimal places" is a specifically defined mathematical constant. It is true that, according to general relativity, in the geometry around a massive object, the "ratio of the circumference of a circle to its diameter" is not even a constant, much less "equal to \pi".


I'm not at all clear what you mean by "makes it both fundamentally and practically impossible to measure pi to more than 10 significant figures." I'm sure there are difficulties with that that have nothing to do with gravity!
 
One does not measure pi, it is a defined value: the ratio of a circle's circumference to it's diameter in *Euclidean space*.
 
Teresa said:
I have heard that while pi is known to many millions, even billions of decimal places, gravity makes it both fundamentally and practically impossible to measure pi to more than 10 significant figures.

I find this to be a very strage theory, and have never heard of it before. I am also finding it difficult to find any information on the area.

I've seen this nonsense claim at some math crank sites. (Others have already explained why it is nonsense.) I hope you didn't hear it in school or anyplace like that.
 
\pi , \alpha , it's all the same.

maybe at higher temperatures or energies, \pi changes to a different number.
 
Chris Hillman said:
I hope you didn't hear it in school or anyplace like that.

haha, actually I heard it from my university lecturer...

that online link that pervect gave for the gravitation book gave me an idea as 2 what my lecturer was on about... there's a bit in it that has to do with space being warped by gravity, and it uses an example of a black hole to make the point really obvious... section 4, titled the r-coordinate: reduced circumference, the 7th page down...

basically, coz the black hole warps spacetime, if u have a circle/sphere around the black hole, the actual radius is not going 2 b the ratio we'r used to, the radius will b greater... but yeh, that site explains it beta than i do haha
 
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Chris Hillman said:
I hope you didn't hear it in school or anyplace like that.

Last week I met my niece's boyfriend, who just finished his first year of university, and he said that his physics prof told the class that dark energy is responsible for the slowing down of the expansion of the universe.
 
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rbj said:
\pi , \alpha , it's all the same.

maybe at higher temperatures or energies, \pi changes to a different number.
No, no, no, no, no, no. (one for each post where someone corrected this misconception already...)
 
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Trying again to explain the point

rbj said:
\pi , \alpha , it's all the same.

maybe at higher temperatures or energies, \pi changes to a different number.

Robert, I really hope you were joking. If not, please move this to "Skepticism and debunking".

Teresa said:
haha, actually I heard it from my university lecturer...

Teresa: I think you are missing the point. Pi is defined to be the circumference of a euclidean circle of unit diameter. What the book you read (and probably what our lecturer) actually said--- or if not, what they should have said--- is that while the notion of "circles" still makes sense in noneuclidean geometries, the relation to circumference and area to diameter of these circles is not given by the euclidean formulae
<br /> C=\pi \, d, \; A= \pi \, d^2/2<br />
but rather by more complicated relations C=C(d), \, A=A(d). In some cases, e.g. hyperbolic or spherical geometry, it is possible to write down these relations precisely. In general, all one can say is that for very small circles, the euclidean relations hold almost exactly in any curved manifold. That is one reason by euclidean geometry holds a special place in Riemannian geometry (the study of curved manifolds).
 
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