Paul Hedderly
New member
It depends on the angle of the rope going through the tree as to whether the load is doubled. Also friction at the anchor point can effect the load as well. This article has been posted here before but it is so good I'll post it again. towards the end is where it talks about rope angles.
http://vtio.org.au/Content/wp-content/uploads/2010/07/Single-Rope-Technique-i.pdf
Cheers TreezyBuzzy! I'm aware I posting a simplified summary of the basic loading principles - but that was because I perceived some confusion from previous posts.
I'm also aware that I was talking about the Total Climber Load (mass) as a static variable, which it is, but that by introducing movement we are really needing to consider the dynamic load.
The angle thing is interesting, but I ignored it for two reasons, first, we are generally here talking aboutthe initial access to a high tip (ie no redirects, and that here is not the TIP, but the tip of the climb, Top Of System = TOS) and so typically the load and anchor lines being close to parallel and second, 200% is the worse case (at least for the TOS!) so is a worthy consideration. (The caveat is situations where you can get the anchor line going above and beyond the TOS crotch in the direction of the supporting branch thereby bring the load vector closer to the branch itself, in which case a base anchor will put a much safer compression load on the TOS - but how difficult is that to achieve from the ground? which explains my point above.)
Friction makes life so much more complicated, but at the end of the day, in terms of TOS loading I suspect it is dwarfed by the shock loads of a climber ascending the rope, especially since no rope is anywhere near completely static, and again - the worst case scenario is that the anchor side holds the same load as the climbing/load side and so the effect on the TOS is doubled - and we always need to be considering the WCS.
I have no proof but I think there is a further effect that makes _certain points_ of a climb more risky than others. A shock (generated by movement - ie each climbing thrust or descent brake) travels along the line in waves. The transmission, duration and frequency will vary by the line construction, climber mass, movement aggression and timing, oh and by friction. Waves have a tendency to reflect off static points (ie the anchor and the TOS. At certain points the freqeency, wavelength and line length may collude to align fresh shock waves with reflections... either in the load or anchor side, amplifying their strength and the momentary loads on the TOS and harness and anchor.
But how to prove and/or quantify the effect... beyond me
Its certainly demonstrably very destructive to power lines, bridges and buildings with wind loading or earth movements... you dont have to trawl google very far for the evidence there.
EDIT:: I've replaced references to TIP above to TOS - meaning Top Of System. In DdRT and SRT with a top anchor the TOS will be the TIP also, unlike the base anchor system. SOrry for the confusion!
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