GSO003 Problem 8
Problem Statement
Movable Pulley on a Hyperbolic Trajectory and Nonlinear Tension
Problem Statement
Set up an x–y coordinate plane. The positive y-direction is vertically upward; the positive x-direction is horizontally to the right. The magnitude of gravitational acceleration is g.
A light, inextensible string has one end fixed to point A(0,H) on the ceiling. A smooth fixed pulley of negligible size and mass is attached to point B(L,0) on a wall.
A smooth movable pulley of mass M (negligible size) is threaded onto the string, which then runs over the fixed pulley at B. The free end of the string is pulled slowly with force F.
The movable pulley maintains quasi-static force balance as it moves in the x–y plane. (As the string is pulled, the movable pulley traces a smooth curve moving upward and to the right toward pulley B.)
Find the magnitude of force F at the instant when the x-coordinate of the movable pulley is x=43L.
Pulley friction and string mass are negligible. The geometry is ideal (no interference between string sections).
Constraints
- H=2.0m
- L=3.0m
- M=16kg
- g=9.8m/s2
Input Format
Find the magnitude of force F in N and give the answer as a positive integer.
Solution
1. Force Balance on the Movable Pulley
Let the movable pulley be at P(x,y).
Since the movable pulley is smooth, the tension throughout the string equals F. The pulley is acted upon by three forces:
- Tension F directed toward A
- Tension F directed toward B
- Gravity Mg downward
Let θA and θB be the angles each string segment makes with the vertical.
Horizontal equilibrium:
−FsinθA+FsinθB=0⟹θA=θB=θThe two string segments always make equal angles with the vertical.
Vertical equilibrium:
2Fcosθ=Mg⋯(1)2. Deriving the Trajectory of the Movable Pulley
Expressing θA=θB=θ in coordinates (with y<0 since P is below B):
From A(0,H) to P(x,y): tanθA=H−yx
From B(L,0) to P(x,y): tanθB=−yL−x
Setting these equal:
H−yx=−yL−xRearranging:
−xy=(H−y)(L−x) 2xy−Ly−Hx+HL=0 y=2x−LH(x−L)⋯(2)This is a rectangular hyperbola. The domain is 2L<x<L.
3. Position and Angle at x=43L
Substituting into equation (2):
y=2⋅43L−LH(43L−L)=21LH⋅(−41L)=−2HThe movable pulley is at P(43L, −2H).
Computing tanθ:
tanθ=H−yx=H+2H43L=23H43L=2HL4. Computing Force F
Substituting H=2.0 and L=3.0:
tanθ=2×2.03.0=43From the right triangle with tanθ=3/4: hypotenuse =32+42=5, so cosθ=54.
From equation (1):
2F⋅54=Mg⟹F=85Mg F=85×16×9.8=98NAnswer: 98