Tensile Shock Waves in Tethers

Years of flying small kites in hurricane-force winds on the US NW Coast had many exciting lessons for what Jet Stream wind is like. A particular incident involved a 1m2 parafoil lifter on ~200kg rated (~400kg breaking strength) UHMWPE line in ~30msec wind. A sudden wind burst sent an apparent shock wave down the line that smashed into the anchor-point, where the line failed instantly. A loose end was to come with the right search term- “Tensile Shock Wave”, to find relevant science. This 1969 paper does the job, just keep in mind any polymer supports elastic waves, not just natural rubber. The sonic-relativity physics is cool, that if Mach ramps up suddenly along a kite line, a shock wave forms, and this sonic boom can destroy tethers. Such a shock wave may easily form on a suddenly snubbed tether by a massive high-velocity kiteplane.

Production of Tensile Shock Waves in Stretched Natural Rubber

Nature volume 224 , page1301(1969)

Abstract

IT may be shown theoretically that when plane mechanical pulses of finite amplitude travel in non-dispersive media, the velocity of propagation in space is given by c + V where c = ( S / ρ )1/2, S being the tangent modulus of the material and ρ its density, and V is the particle velocity associated with the pulse. If S increases with increasing amplitude of deformation, the head of the pulse will become steeper as it travels through the medium and it will eventually become a shock front, the gradient of which is limited by dissipative processes, such as internal friction and thermal conductivity. Such compressive shock waves are well known in fluids and in recent years similar shock waves have been produced and studied in blocks of solids1.

https://www.nature.com/articles/2241301a0

==== original Old Forum message =====

"dave santos santos137@yahoo.com
To:AirborneWindEnergy@yahoogroups.com

Feb 7, 2013 at 1:42 PM

Our advanced low-stretch tethers seem to have a unique vulnerability to shock-wave formation. The conjecture is- if the line is tensioned near its max working load, and there are high-energy harmonics on the line, rogue shock waves can form to crash into kite and anchor-nodes, and cause a line to fail well below its measurable static load. An elastic line absorbs shock peaks before they do damage.

I lost a small (1m2) single-line parafoil last year in a US NW Coast gale to a shock wave on the line (its still a hundred feet high in a tree). The kite was going nuts and the 400lb rated UHMWPE line, in good condition, was “jangling” wildly, but a padded belt around my waist made the 50lb estimated gust surge pulls quite manageable. A specially powerful gust hit the kite, and the jumpy line suddenly parted right at the hand winder knot on the belt.

Its well known that an ordinary knot weakens a line greatly, but there was more going on here, since this line was so over specified. There was no excessive tug before the line parted. It was rather clear the line had not parted by “static force” alone, but a sudden shock effect focused at the anchor-node seemed to be to blame. UHMWPE has a low melting temp, so the failure mode may have been a sudden local heating resulting in the break (rather than a break in progress releasing heat). The knot was a stress-concentrator node itself, and knot failures by shockwaves may be common. A corollary prediction here is that knots in stretchy line have a lesser weakening effect.

Rogue shockwave line failure is predicted to follow a certain classic pattern. The at-risk line is low-stretch, tension is high, and the harmonics on the line are energetic and chaotic enough to combine by chance into rogue peaks exceeding the breaking strength. The longer the line, the more energy it can store harmonically to focus on a node. If the line is being rapidly pumped, complex phase-shifts arise favorable to random shock wave formation. Wind turbulence on the line also destabilizes normal dynamics. Risky nodes are stiff and sharply discontinuous.

There is a luck factor to rogue waves, which can occur even in moderate “improbable” conditions. Shock waves can also hammer at a node, for accumulated damage. The node itself, say a composite airframe, might be directly damaged. Good shock absorption design is possibly essential to future AWES. Fishing poles are a good reference model for harmless shockwave absorption, but high efficiency line pumping is the competing trade.

This is another poorly understood topic in AWES design suitable for careful study…"

Below, just after the quote, is a text from Dave Santos. Although its content differs significantly from the subject of this topic, I think that it can find its place there because we remain in the field of tethers, and according to a common point which is the energy storage with tethers:

Future AWE Potential of Twisted Carbon Nanotube Threads, now shown superior for Kinetic Energy Storage Media

AWE depends on polymer tethers and fabrics whose elastic energetic properties apply to many concepts, to transiently store energy in oscillating spring-mass dynamic cycles, and transfer and store energy of harvesting. Elastomer bungee is already useful.

Recently, I did an extended AI session where it was found that current engineering polymer elastic storage could already be technoeconomic in hard-rock mine shafts filled with parallel ropes tensioned by AWE, perhaps as a Grid load-leveling resource.

Now comes this work validating remarkable specific energy (energy-to-mass) storage of Carbon Nanotube based threads twisted and cross-bonded from many tubes. All that really has to happen now is for cost to continue coming down.

“Notably, the gravimetric energy density of these twisted ropes reaches up to 2.1 MJ kg−1, exceeding the energy storage capacity of mechanical steel springs by over four orders of magnitude and surpassing advanced lithium-ion batteries by a factor of three.”

Giant nanomechanical energy storage capacity in twisted single-walled carbon nanotube ropes | Nature Nanotechnology

AWE is just one of countless potential applications. The ultimate combination of Graphene fabric and Carbon Nanotubes promises kites that do not tear and are so light they seem to float in place during lulls, and now they may store kinetic energy in useful ways.

Elastic Polymer Energy Storage is an ancient technology, as Torsion Bundles in Catapults, and later in Rubber-band Motors in Model Aircraft. New versions wih advanced materials simply promise to be orders-of-magnitude more effective.

The PDF is available at the link in the text above.

From the link above:

Twisted y-rope (TPU) efficient energy output and conversion

Furthermore, we investigated the direct energy output from twisted y-ropes (TPU) by the rotation of a load (eye-hook + paddle) attached to it, which is more than 4 × 104 times higher in weight than the weight of the rope sample. The rope sample was first twisted through 10, 20 and 30 rotations using a motor at 110 rpm, after which it was allowed to untwist with the load. We have defined ‘recovery’ Rr as the ability of the twisted (forward rotation) SWCNT rope to return (reverse rotation) to its original, untwisted state after undergoing a specified number of twist cycles. In particular, after ten twisting rotations, the rope untwisted back to approximately 90% of its initial untwisted configuration. This implies that a residual twist remains in the rope after the untwisting process. The presence of a residual twist suggests that there might be some energy dissipation due to internal friction and air resistance, leading to the decay and eventual cessation of the periodic motion in the system, resulting in a slight deviation from complete recovery. The actual stored energy influences the extent to which Rr surpasses 100% and the duration of the periodic motion. Indeed, we observed Rr values exceeding 100% during reverse rotation of y-rope (TPU) samples twisted through 20 and 30 rotations in the forward direction (Supplementary Video 2).

This could also be a way to transfer torque via the central tether of the SuperTurbine ™ or the ropes of Daisy (?) over long distances, and to reach very high altitudes using lifter (rotating?) kites, not only in the upper part, but also in the middle sections in order to share the overall lift across the entire multi-rotor device.

In this case the storage is not used as such, but only to start the torque transfer operation, like a propeller or a wind multi-rotor turning a rubber (not the reverse!), or several rubbers for Daisy (?), before acting the torque at the other end in order to turn the generator.