Potential in caternary problem

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SUMMARY

The discussion focuses on the catenary problem, specifically the equilibrium shape of a flexible but inextensible chain suspended between two points. The potential energy of a segment of the chain is expressed as delta p = y(1+y'^2)^(1/2) delta x, where y' represents the slope. The participants clarify the derivation of this potential energy and its components, including the relationship between the slope and the length of the chain segment. The conversation references the Wikipedia page on catenaries for further derivations and insights.

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thehoten
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a flexible but inextensible chain having uniform mass density is suspended between two points (of course not vertically aligned). Find the shape of the equilibrium of the chain.

The chain will settle down to a position of minimal potential energy. Let the suspending points be (a,y(a)) and (b,y(b)) where (without loss of generality) b>a and y(b)>y(a). The potential energy delta p (relative to y(a)) of a portion of chain corresponding to small delta x is gievn by delta p = y(1+y'^2)^(1/2) delta x.

I don't understand where this potential comes from
 
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I don't recognise it either apart from the square root but its often difficult to work backwards from part of an answer- several good derivations can be found at

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

Regards

Sam
 
y' is the slope, tan(θ). Squaring, adding 1 and sqrting gives sec(θ).
Multiplying that by dx gives ds, the length of the section of chain (hypotenuse). Taking the density to be 1, that's also its mass.
The final factor, y, seems intended to be its height above the reference point, y(a), but that seems a very confusing notation.
 

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