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SHARP-EDGE ROPE TESTING. STATUS
AND PROSPECTS
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Carlo Zanantoni
Commission
for Materials and Techniques, Italian Alpine Club
Motivation and short history
There is no report of accidents occurring in mountaineering
due to ropes breaking on the point of contact with a carabiner:
the ropes usually break on sharp edges (sometimes by friction
on rough rocks). The standard DODERO test, where the rope passes
through an orifice over an edge with 5 mm radius, simulating
a carabiner, doesn’t tell much about the resistance of
a rope on a sharp edge. The firm EDELWEISS repeatedly proposed,
since the early 1980s, to test ropes on a straight sharp edge;
the proposal was supported by Pit Schubert, but was repeatedly
refused by the UIAA Safety Commission on the basis of a number
of appreciable arguments, which may be reviewed during the
discussion. Recently (1999) the Board of the UIAA asked its
Safety Commission to further investigate the problem. As a
consequence of this request, the Commission for Materials
and Techniques (CMT) of the Italian Alpine Club carried out
a number of tests on sharp edge failure of ropes on their
DODERO at the University of Padova.
At the same time, the CMT was improving its equipment, as
described in a companion paper in this Conference, in order
to investigate the significance of the energy absorption at
rupture on a single drop, at least for the sharp edge case.
For a number of reasons the modifications of the equipment
were delayed until now, so we can only speak about our programmes
concerning the energy absorption method. We hope this helps
stimulating discussions and suggestions.
Multi-drop sharp edge tests
on the DODERO The edge - The specimens.
The tests were performed on a straight sharp edge according
to Fig.1, as proposed for an additional test in the UIAA standard.
Most of the tests were made (winter 1999-2000) with a 0.75
mm radius of the edge, some of them (spring 2001) with 0.5
and 0.25 mm radius. Four types of single rope were used, standard
length (2.5 m beyond the edge).
The tests with edge radius 0.5 and 0.25 mm are not reported
here, since they would not significantly contribute to the
conclusions of this paper.
Why multi-drop
The tests were repeated with variable fall heights, smaller
than or equal to the standard DODERO height of 4.8 m, in order
to achieve resistance to a number of falls considerably higher
than 1. The idea behind this is rooted in the history of the
UIAA Safety Commission: a reasonably high number of falls
must be achieved, in order to be able to differentiate between
two ropes (or between two different stages of wear in a given
rope), in other words to provide a result that may approach
a decent measurement of the rope’s performance. Indeed
if, say, the resistance to a single fall at full height (4.8
m) were required as standard, it wouldn’t be possible
to appreciate the difference between a rope which is just
able to hold one fall (result : 1) and a rope which is just
a little weaker (result : 0).
The same principle lies behind the classical DODERO test,
in particular in the case of half-ropes: in the Plenary Session
of the UIAA SAFCOMM held in Venice, 1979, Mr Lacoste of the
Laboratoire de l’Armée, Toulouse, and the writer
of this note proposed a test for half-ropes based on 5 falls
of a 55 kg mass: a long set of experiments had been carried
out to find a multi-drop test which could, roughly, be considered
as equivalent to 1 fall of an 80 kg mass. Resistance to this
fall was indeed considered as the minimum requirement for
a rope that could have been loaded by the fall of the leader
on a single strand.

Figure 2
The tests – a critical view
The ropes had been conditioned for a long time in the same
environment (the humidity varied between 60 and 75 %) in the
University underground, but not conditioned according to the
UIAA standard; this was considered to be sufficient for a
preliminary investigation. For the same reason each test was
limited to one specimen. The easy interpolation in plotting
the results seemed to justify this approximation.
The results of the tests over a 0.75 mm radius straight edge
are reported in Fig.2. It’s a pity that not enough specimens
were available to cover the complete range of fall heights
for all ropes: in spite of this, Fig.2 is eloquent enough
to justify a number of conclusions:
1. Rope S, typically built for resistance on sharp edges,
is the best in high falls, but not so much better than rope
J, although J has poor performance on the standard test (5-6
falls instead of 10 for rope S).
2. When the fall height is reduced, some ropes tend to become
even better than rope S. This seems to depend on the ability
of the core yarns to spread over the edge; it occurs when
the sheath is soft, particularly so (rope J) when the sheath
breaks soon after the first fall, thus allowing all threads
to spread freely over the edge. This had been discovered many
years before (1980s) by Pit Schubert , but unfortunately not
much attention had been given to it.
3. So, whilst going to lower fall heights is necessary to
give us something similar to a decent measurement of the rope
performance, it leads us far away from the physical phenomena
that really occur during failure on a sharp edge. This remark
is similar to the reproach that is usually made to the conventional
DODERO test, when its ability to simulate the real occurrences
during a breakage of the rope in a single drop over a carabiner
is questioned; however, whereas in that case that breakage
is not probable, in our case (sharp edge) we are trying to
simulate a very probable occurrence.
4. We must look for other means of measuring the rope performance
over a sharp edge. The prospects of the energy absorption
at rupture as a significant parameter must be investigated.
In addition, measurements of the breaking load over a sharp
edge at low speed may provide useful information. This matches
with the intentions that prompted our CMT to increasing its
experimental equipment (as described in a companion paper)
in order to perform a real measurement of the rope performance;
this decision was taken many years ago, but unfortunately
our equipment is just ready now, thus it was not possible
for us to use it to support the feasibility of this approach.
Measurement of the energy
absorption at rupture
Short history
The multi-drop classical DODERO test was subjected to criticisms
since it was born, just after the second world war; it was
considered to have three main weaknesses:
1) testing occurs over a rounded edge like a carabiner,
2) it is not a real measurement of rope performance [particularly
so at those times, when the number of falls to be held was
just 2] due to the large error caused by a 1- fall difference
between two tests. Therefore it is not accurate enough to
accurately compare two ropes,
3) there is an obvious difference between the physical phenomena
occurring on occasion of a number of falls and those occurring
during a single fall leading to rupture of the rope.
For obvious reasons related to the rope technology available
at that time, objection 1 didn’t lead to any practical
initiative, except the one of EDELWEISS mentioned above; objections
2 and 3 led Leonard McTernan, of the National Engineering
Laboratory, Glasgow, to develop a DODERO for energy measurement
at rupture even for tests over a conventional edge (5 mm radius).
To the writer’s knowledge, he was first to propose this
kind of test. He used a 190 kg mass to bring the rope to failure
on a single fall, and an electromagnetic transducer to measure
the variation of the speed of the falling mass, thus the energy
absorption. That was about the middle 1970s. McTernan’s
proposal didn’t have much success at that time, probably
because it didn’t provide an answer to objection 1,
whilst the improvements in rope quality rendered the objection
2 less stringent as time went by, due to the increase of the
number of falls. Objection 3, however, was becoming even more
valid with better ropes.
Objection 1 prompted the sharp edge proposal of EDELWEISS,
that we are now trying to develop. For sharp-edge tests, objection
2 would play in favour of the multi-drop tests described above;
however, the disappointing results of our tests and objection
3 speak in favour of a single drop with energy absorption
measurement. So, energy absorption seems to be the best we
can propose at the moment. Let us now discuss the prospects
- as well as the objections against - this proposal.
Measurement of energy absorption at rupture- Comments and
prospects.
Several ways of measuring the energy absorption with sufficient
accuracy are now available. The ones available at our laboratory
at Padova University are described in a companion paper. Forces
and position of the mass are recorded as a function of time,
thus enabling us to calculate the energy absorption. The position
is measured by means of a laser beam, impinging on a “mirror”
attached to the mass.
Several objections can be raised against this method:
- there are no clear reasons for choosing a given curvature
radius for the edge
- the edge of a rock may be sharper
- the edge of the rock may not be at a square angle to
the rope line, thus its knife-like cutting action may be
qualitatively different from the one proposed.
the energy is absorbed by the whole specimen, therefore it has
no direct relationship with the phenomena that occur in the
short piece of rope touching the edge.
I am trying to respond to these objections in the following
way:
- objection a): no rope can stand over a knife blade, we just
want to have an indication of the ability of a rope to withstand
the action of edges better than other ropes. Moreover, the tests
carried out on many occasions by Pit Schubert, comparing different
ropes on various edges, down to 0.2 mm radius, have shown that
the comparison between ropes is very little affected by the
sharpness of the edge. Finally: what else can we do?
- objection b): see previous answer
- objection c): this is a problem. An inclined edge could be
used: sensible? I am afraid we must be satisfied with the present
proposal; however, we could investigate this alternative with
low-speed tests, using the machine described in the companion
paper.
- objection d): this objection can also be raised against the
conventional DODERO test, and it is more justified there than
here: in a single-drop test, a “better” rope will
more clearly show its ability to absorb more energy before it
is cut by the edge. It will, e.g., be able to stand a fall with
a higher fall factor or with a less effective dynamic belay.
The CMT programme
We shall of course use a mass heavier than 80 kg and carry
out a large number of tests to investigate to what extent
the energy absorption at rupture can tell the difference between
two ropes. I am taking the risk here of anticipating what
else we could do.
On the DODERO:
with r = 5 mm, M = 80 kg:
• measure the usual N = number of falls sustained
with r = 5 mm, M* > 80 kg
• Fm = maximum force (arrest, Fangstoss)
with sharp edge, mass M* > 80 kg:
- Er, energy absorbed at rupture
- compare Er for many ropes, to verify the significance
of this test
- Fr, breaking force
On the slow-speed machine, using doubled specimens:
- check the independence of force/elongation curve from
speed
- Frs = “static” breaking load on r = 5 mm
- Frsh = “static” breaking load on sharp edge
- compare various types of sharp edge
- study the breaking process with a TV camera
Possible investigations:
- try to find a correlation between Er and the classical
N, as an attempt to justify the standard procedures
- try to find a correlation between Fr / Fm and Er
- try to find a correlation between Frsh / Frs and Er
CONCLUSIONS
We believe that we must do our best to develop a sharp edge
test; the efforts that we have made in improving our experimental
equipment were to a great extent justified by this aim. We
are unfortunately confined to speaking about equipment and
programmes; we do so because of our desire to take advantage
of the opportunity offered by this conference to stimulate
discussions and suggestions on the part of a wide and competent
audience, such as we would rarely have the opportunity to
encounter.
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