# Hanging Cables Consider a portion of cable At lowest point of cable, a horizontal force H acts to stop the cable moving to the right H W(x) At centre of.

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Hanging Cables Consider a portion of cable At lowest point of cable, a horizontal force H acts to stop the cable moving to the right H W(x) At centre of mass of cable a weight force W acts At point (x,y) there is a tension force T tangential to the cable T (x,y)(x,y) Take origin at lowest point. x y

T Since system is in horizontal and vertical equilibrium As the gradient at (x,y) is given by H W(x) (x,y)(x,y)

But W varies as x changes, so differentiating Fundamental Equation H W(x) (x,y)(x,y)

The catenary A flexible rope of constant density hangs between two points. Determine its shape. Let w be the mass per unit length of the rope where s is the length of rope The fundamental equation is The fundamental equation becomes

Short section of cable ds dx dy Consider a short section of cable, so short that it is effectively a straight line

Fundamental equation Taking the origin at the lowest point what are the initial conditions?

Separate variables

Solve Separate variables and integrate

What is the length of the cable?

If we measure arc length from the origin Separate variables and integrate

Total length L D

L D If we want a cable to span a distance L Knowing the two properties of the cable, weight density and the tension that it can withstand We can work out the length of cable required and the droop of the cable.

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