Why does a Moebius strip twist unevenly along its length?

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Harlan
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A recent article in Smithsonian magazine about knitting geometric forms stimulated the following question:
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In the above, knitted Moebius strip, there are areas where the material is twisted (seen in front) and areas where the material is flatter/less twisted (seen in back). So far as I can tell, the same is always true for Moebius strips made from twisted paper. (The knitted form shown also has a kink in it, which a paper form will normally not have.)

This localization of the twist has also been found to occur in (both real and theoretically constructed) Moebius strips made of benzine or other chained molecules, which took the researchers investigating this phenomenon by surprise.

This raises for me the following questions:

1) Why, in all these physical situations, is the twist not evenly distributed along the strip?
2) Is a regular twist possible to achieve in any non-rigid material? (I specify non-rigid because it seems that one could cast such a thing in bronze or concrete, 3-D print such a form, or even construct one of superconducting materials...although even most such forms seem to have regions of greater and regions of lesser twist)
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If you follow a letter around it twists about its path at a constant rate. Notice the distortion of the text is maximum on the right hand side. Paper does not like to distort like that.

The above from, https://mathematica.stackexchange.com/questions/5783/rotating-an-image-along-a-möbius-strip

Which is from, https://www.google.com/search?safe=......1c.1.64.img..1.0.0...0.ulBGYlNPQfM#imgrc=_

The image Harlan wanted to post?

file-20180625-19399-y5ti0b.jpg


Right click on image, copy, and paste here.

Image at, https://www.smithsonianmag.com/innovation/what-knitting-can-teach-you-about-math-180969637/
 

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Harlan said:
1) Why, in all these physical situations, is the twist not evenly distributed along the strip?
The shape will depend on how easy the initial straight strip bends one way (roll) vs. how easy it bends the other way (curve in plane with edges stretching).

See for example:
https://link.springer.com/article/10.1007/s10659-014-9495-0
 
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Using the knitted version as a model, consider this. The same situations apply to the others but it's easier to see with the knitted one.

  • Cut the knitted strip vertically, thru the Blue, Red and Gray stripes.
  • Lay the resulting strip flat on the table.
  • Now curl the ends around to meet; so it looks like a flattened donut.
You will find that the inner circumference will buckle into ripples, it will not lay flat. That's because the inner and outer edges are the same length but with the inner circumference being smaller that the outer circumference, the extra material has to go somewhere.

The same thing happens with the Mobius strip. It just turns out that the lowest energy configuration is for the 'extra material' on the edges to exchange places so that there is only one ripple. In fact, even the 'donut' may have only one ripple in it (you could flatten it though so there are many small ripples).

Cheers,
Tom

EDIT: Looks like @A.T. found the complete version while I got interrupted during the short version. :frown:
 
Regading your second question:
Harlan said:
2) Is a regular twist possible to achieve in any non-rigid material?
I assume you mean sarting with a staight strip, then bending it to connect the ends with twist? If you vary the stiffness parameters for the different bending directions along the strip, then it should be possible to get constant twist rate and a circular center-line, like in the animation text animation above.

But whether achieving this with a constant combination of stiffness parameters is also possible, that's harder to say. Intuitively, when you make the loop from a rod with a circular cross section, then there should be a combination of bending stiffness (same in all directions) and torsional stiffness, that results in that shape. Maybe you just need high torsional stiffness.