Why is the tension in a massive cable always tangent to its portion?

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The tension in a massive cable is always tangent to its portion because, in equilibrium, the forces acting on a small elemental section of the cable must balance without creating a net torque. When examining the cable, the gravitational force is small compared to the larger tensions, which must be nearly equal and opposite to maintain stability. This tangential behavior is a result of the cable's ideal properties, as real ropes cannot exert internal shear forces. Unlike a copper rod, which can apply torques due to its bending stiffness, a rope behaves as a spring, only transmitting stretching forces. Therefore, the tension remains tangential in the limit of an infinitesimally small segment of the cable.
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Homework Statement


Why is the tension always tangent to the portion of the cable?
Snap1.jpg

The correct situation is on points A and B.
Why can't be like on C and D?

Homework Equations


Newton's force-mass: ##F=ma##

The Attempt at a Solution


If i move the portion of the cable and examine, for equilibrium, portion CD, then what about portion AC, does it pull up now, while in position A the portion of the cable on the left of A, if the tension wouldn't be only along the cable, would have pulled down since it was part of the examined cable.
So the tension is only along the cable from symmetry only. is it true? i sense it's not the single reasoning.
 
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Forces in other directions are only possible if your cable is stiff. Which can happen, but that is not the typical rope problem.
 
Consider a very short elemental section of the cable. It is almost straight. The forces on it are a small gravitational force and the two much larger tensions. The tensions won't be quite tangential, but most be close to it. They must be almost equal and opposite, and if not almost tangential they would apply a net torque. In the limit, as the length and mass of the element tend to zero, the tensions are tangential.
 
haruspex said:
Consider a very short elemental section of the cable. It is almost straight. The forces on it are a small gravitational force and the two much larger tensions. The tensions won't be quite tangential, but most be close to it. They must be almost equal and opposite, and if not almost tangential they would apply a net torque. In the limit, as the length and mass of the element tend to zero, the tensions are tangential.
But won't this same argument work for a copper rod bent into a catenary shape?

I thought it's related to material properties, that ideal ropes cannot exert an internal shear, so the only forces to consider are stretching forces (tangential to this tiny segment) (think a spring)
 
yucheng said:
But won't this same argument work for a copper rod bent into a catenary shape?
No, because the neighbouring parts of the rod can apply torques to the element. The tensions will still be nearly equal and opposite as vectors, but can be at an angle to the tangent, resulting in an opposing torque.
 
Copper tubing has substantial bending stiffness, which is not present in a thin rope or wire.
 
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