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Question: A rope of length $l$ placed straight on a frictionless horizontal floor is pulled longitudinally by ...

A rope of length ll placed straight on a frictionless horizontal floor is pulled longitudinally by a force FF from one of its ends. Tensile force TT developed in the rope at a distance xx from the rear end varies with xx as shown in the graph. What can you certainly conclude about density of the rope?

A

It is uniform.

B

It decreases with distance xx from the rear end.

C

It increases with distance xx from the rear end.

D

It is maximum in the middle and decreases towards the ends.

Answer

(b)

Explanation

Solution

To determine the variation of the rope's density, we analyze the tensile force TT in the rope.

  1. Define the system and variables:

    • Length of the rope: ll
    • Applied force: FF at one end (let's assume the front end, x=lx=l).
    • Distance xx is measured from the rear end (x=0x=0).
    • Mass per unit length (linear density) of the rope: λ(x)\lambda(x).
    • The rope is on a frictionless horizontal floor.
    • Since the rope is pulled by a force FF, it will accelerate. Let the acceleration of the entire rope be aa. Since it's a rigid body (or in this context, an inextensible rope), all parts of the rope move with the same acceleration aa.
  2. Interpret the graph and tensile force:

    • The graph shows T(0)=0T(0) = 0 and T(l)=FT(l) = F.
    • T(x)T(x) is the tensile force at a distance xx from the rear end. This force is responsible for accelerating the segment of the rope from 00 to xx.
    • Let m(x)m(x) be the mass of the rope segment from 00 to xx.
    • m(x)=0xλ(x)dxm(x) = \int_0^x \lambda(x') dx'.
  3. Apply Newton's Second Law:

    • The net force on the segment of the rope from 00 to xx is T(x)T(x).
    • According to Newton's second law, T(x)=m(x)aT(x) = m(x) \cdot a.
    • Substituting m(x)m(x): T(x)=a0xλ(x)dxT(x) = a \int_0^x \lambda(x') dx'
  4. Relate tensile force to density:

    • To find λ(x)\lambda(x), we differentiate T(x)T(x) with respect to xx. Using the Fundamental Theorem of Calculus: dTdx=addx(0xλ(x)dx)=aλ(x)\frac{dT}{dx} = a \frac{d}{dx} \left(\int_0^x \lambda(x') dx'\right) = a \lambda(x)
    • So, the slope of the TT vs xx graph, dTdx\frac{dT}{dx}, is directly proportional to the linear density λ(x)\lambda(x), with the constant of proportionality being the acceleration aa.
  5. Analyze the graph's slope:

    • Observe the shape of the given TT vs xx graph. The curve is concave down.
    • This means that the slope dTdx\frac{dT}{dx} is decreasing as xx increases. Visually, the tangent to the curve is steepest near x=0x=0 and becomes flatter as xx approaches ll.
  6. Conclude about density:

    • Since dTdx=aλ(x)\frac{dT}{dx} = a \lambda(x) and aa is a positive constant (the rope is accelerating), if dTdx\frac{dT}{dx} decreases as xx increases, then λ(x)\lambda(x) must also decrease as xx increases.

Therefore, the density of the rope decreases with distance xx from the rear end.