I was trying to figure out how much force a rock climber would experience when they fall, at first I thought the rock climber would have some potential energy ($E_p$) given they are a certain distance up ($h$), have mass ($m$) and are under the force from gravity ($g$). $E_p = mgh$. I then thought that potential energy would be converted to kinetic energy, then to work done. Assuming that the transfer of energy is 100% efficient then I can just skip the kinetic energy part and convert right from potential energy to work done ($E_w$). So $E_w = E_p$, work done is the force ($F$) applied over a certain distance. I’m guessing in this situation the distance would be how much the rope stretches when the faller falls, lets call that ($d$).
$$Fd = mgh$$
or
$$F = \frac{mgh}{d} \tag{1}$$
(1) Feels right as it meets my sanity checks :-
- The more stretching ($d$), the less force ($F$)
- The more mass ($m$) the more force ($F$)
- The higher the fall ($h$) the more force ($F$)
There is just one problem. When I go online to find dummy values to check for ($d$) I find out that the stretch of the rope is always given as a percentage... Which implies the longer the rope is the more it stretches. If we are falling from a larger distance ($h$) we would need more rope, we can conclude $h \propto d$. If we add in the constant of proportionality we end up with $$d = kh \tag{2}$$ subbing (2) into (1) we get
$$F = \frac{mgh}{kh}$$ Which simplifies down to $$F = \frac{mg}{k}\tag{3}$$
If I then do a sanity check on that…
More stretching probably means higher ($k$), so lower ($F$) which is fine
More mass ($m$) is more force ($F$), fine
Uhm, yeah… Turns out falling from higher ($h$) doesn’t make a difference here...
So this implies that someone falling from say $1\cdot10^{-3}$ m is experiencing the same force as someone falling $100m$. Where have I gone wrong in my thinking? Thanks
To a first approximation the rope acts as a spring. The force is linearly proportional to the amount of stretch. It starts at $0$ when the rope just goes taut. We usually write $F=kx$ where $k$ is the spring constant and $x$ is the current stretch. The energy absorbed is then $\frac 12kx^2$, which you can set equal to the potential energy loss from the fall. Then $E=mgh=\frac 12kx^2=\frac {F^2}{2k}$. The maximum force rises as the square root of the height of the fall and is smaller when the $k$ factor is reduced because the energy is dissipated over a longer distance.
The stretch is given as a percentage because the rope stretches a given percentage when subjected to a given force. At a given force a longer rope will stretch more.