Guys, I don't mean to slight anyone or show disrespect to any experienced climbers, I'm really a nobody compared to you guys. I'd never attempt to tell anyone here how to do their job, rig a tree or anything of the sort.
But, we're not talking about that. We're talking about how much force a trunk-tie exerts on the TIP. How many of us have actually measured that in all of our years of experience? Only a few. So the question would be, with all those years of tree work experience, how does an expert arborist quantify forces in ropes and TIPs? The accurate answer is, they don't, and there's nothing at all wrong with that. So I'm not challenging anybody's experience, not at all, but this is not about how to remove a tree, etc. it's about quantifying forces involved in ropes and TIPs; that is kinda my field. So if we've never actually measured the forces, what do we base our numbers on? Well one way is by the physics involved, and I can talk about physics, especially static physics such as being discussed here.
So please don't think I'm disrespecting anyone over arborist issues, I'm not, this thread is about forces in ropes and on TIPs.
When the question is asked about how much force is produced by something, how do we arrive at an answer? Do the laws of physics give us the theoretical results? Yes, and quite accurately IF all the variables are included. For example, we could make two simple measurements with a dyno and determine how much friction is produced by the rope over the TIP and what force is exerted on the TIP. If we can't do that, then I concede that physics is completely useless and a worthless waste of time to study.
But the whole purpose of physics, statics, dynamics, and even statistics is to help us quantify things we could not otherwise know.
From a theoretical perspective, it is impossible for a trunk tie to triple the weight of the climber at the TIP. I'll be specific: the climber is tied to one end of the rope, the rope is passed over a single TIP, or over a block for a frictionless TIP, brought back down and tied to the tree trunk. The dyno is connected between the limb (TIP) and the rope or block if a block is used. I'm saying, in a static condition, i.e. with the climber hanging motionless, it is impossible for this configuration to produce three times the climber's weight on the TIP. The absolute max will be 2x.
It would seem that there is a need to establish the loading on the TIP in a static condition first, then look at dynamic forces. If we can't figure out the static conditions, we sure won't be able to figure out the dynamic effects.
Mahk,
I was thinking along the same lines you mentioned, I would be extremely interested to see what the dyno measures Tod's weight at. I.e. attach the dyno to the saddle TIP, connect the other end of the dyno to a rope attached to a TIP in the tree and 'sit' on it. I know it doesn't take much of a 'sit' to produce high dynamic forces, but once the dynamic forces settle out, and they will if the climber doesn't move, all that will be left is the static force, which should be the climber's weight plus the weight of his gear. If the dyno reads peak, it should display a weight much higher than Tod's 165 lbs which would of course be the peak loading due to dynamic loading. If it's simply reading average, or real-time, it should read very close to Tod's weight, plus the weight of his gear. If it doesn't, something is very wrong somewhere.