Tension in two ropes holding a board

  • Thread starter Thread starter Mark Taylor
  • Start date Start date
  • Tags Tags
    Board Tension
Join the discussion
Registration is free. Ask a follow-up in this thread, or start your own.
2 replies · 4K views
Mark Taylor
Messages
1
Reaction score
0

Homework Statement


A 12m long board weighing 4kg is suspended by ropes on each end. 3m from the left side a painter is standing, closer to the first rope.

Find the tension in both ropes.

If the painter were to get off of the board, and the second rope snapped immediately after, find the instantaneous acceleration of the board.

Homework Equations

The Attempt at a Solution


I'm pretty lost as to where to even start, or if this is solvable without the mass of the painter, but here's my line of thinking:

If the system is in a state of equilibrium, then Ftension is equal to Fgravity at both ends of the board.

T1+T2 = Fgravity

If I want to solve for T1 or T2, I'm assuming that the center of mass is located where the painter is standing, which would mean that:

T1 = Fg1(the force of gravity on the left side of the board and Fg2 on the right.)

T1 = Fg1 = (3m/12m) * (4kg) * (9.8m/s) = 9.8N

If I carry this out for T2:

T2 = 29.4N

But this seems too easy/simple to be right, and I'm sure that the correct answer would lead to the answer of the third question where the rope snaps.
 
Last edited by a moderator:
Physics news on Phys.org
It is not solvable without the mass of the painter. Without any calcs, we can see that if the the painter were a hippopotamus the tensions would be much greater than if the painter were a flea. The second part doesn't need the painter's mass though, because she has stepped off the board.

In the first part, the centre of mass is not where the painter is standing. It will be a little bit towards the centre of the board from where she is.

To solve the first part, assign some variables names, say P for the painter's mass, TL for the total tension in the left ropes and TR for the total tension in the right ropes. We assume that the ropes are vertical. If not, the tensions would be greater and we'd need to know the rope angles.

We have three unknowns. We can get two equations: one by equating the net force on the board, from the four forces on it (own weight, painter's weight, TL and TR) to zero, and the other by equating the net torque on the board around a suitable point - say the middle of the board - to zero. Those equations allow us to eliminate two unknowns, say TL and TR. P will remain unknown, but we can rearrange to express TL and TR in terms of P.