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Ch 07: Newton's Third Law
Chapter 7, Problem 7

A rope of length L and mass m is suspended from the ceiling. Find an expression for the tension in the rope at position y, measured upward from the free end of the rope.

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1
Consider a small segment of the rope at position y from the free end, with a thickness dy. This segment has a mass dm.
The mass dm can be expressed as dm = (m/L) dy, where m is the total mass of the rope and L is the total length of the rope.
The tension at the bottom of this segment (at position y) must support the weight of the rope hanging below this segment. The weight of the rope below this point is the gravitational force acting on the mass of the rope from y to L, which is g \times \int_y^L dm.
Substitute dm from step 2 into the integral to find the total weight supported by the tension at y. This gives the expression for the weight as g(m/L) \int_y^L dy.
The tension T(y) at position y in the rope is then equal to the weight calculated in step 4, which simplifies to T(y) = g(m/L)(L - y).

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Key Concepts

Here are the essential concepts you must grasp in order to answer the question correctly.

Tension in a Rope

Tension is the force exerted along the length of a rope or string when it is pulled tight by forces acting from opposite ends. In a hanging rope, the tension varies along its length due to the weight of the rope itself. The tension at any point in the rope must balance the weight of the rope below that point.
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Weight of the Rope

The weight of the rope is the force due to gravity acting on its mass, calculated as W = mg, where m is the mass of the rope and g is the acceleration due to gravity. This weight contributes to the tension in the rope, especially at points above the free end, as the tension must support the weight of the rope below the point of interest.
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Static Equilibrium

Static equilibrium refers to a state where an object is at rest and the sum of forces acting on it is zero. In the context of the rope, this means that at any point along the rope, the upward tension must equal the downward gravitational force acting on the segment of the rope below that point, allowing us to derive expressions for tension based on the position y.
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