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I always (well, now I should say normally) get a lot out of your post, but I have to say that is the most meaningless post I have ever read from you.
No, seriously what you have said does make since and I have thought as well about the fact that both canopies have the same number of lines and atachment points, therefor sharing the same force per line no matter the size. But I still don't know????????????????
QuoteI don't understand what happens there very well
Quotethe most meaningful part of your post
Quote>This is where the inverse square law comes in to play. Basicly
>stated: As the surface area insreases the energy of load is
>distributed over a greater area effectivly decreasing the overall
>load on any given point. Make sense?
Hmm, not to me.
The inverse-square law says that strength is inversely proportional to the square of the distance from the source of some radiation/force. It's more applicable to things like radiation than materials strength.
There's also the squared-cubed law, which states that strength goes up as a function of cross-sectional area (i.e. it's size squared) but weight goes up as a function of volume (i.e. it's size cubed.) Which is why ants can't be the size of elephants; their legs wouldn't hold them. But that doesn't seem to apply here either; the weight of a parachute is pretty negligible when compared to the overall system during opening.
So let's consider two 7-cell reserves, one 100 square feet and the other 200 square feet. Assume design is similar, exit weight is similar and opening speeds are similar. Each line sees a similar load; the collection of 40 lines going to the canopy still carries 100% of the load no matter what the canopy size, so each attachement point sees a similar loading. Since the construction of the line attach points, and the configuration nearest the line attachement point is the same in both canopy sizes, they would seem to resist failure near the attachement points equally well. (Unless I'm missing something, which is entirely possible.)
There's one caveat to the above. The final (post deployment) vertical speed of the larger reserve will be slower than the final vertical speed of the smaller reserve - so if opening _times_ are the same, I'd assume forces would be higher on the larger canopy (more deceleration required.) But there's nothing that says opening _times_ have to be the same, and indeed the amount of reefing would have a big effect on maximum loads seen.
However, all the above doesn't speak to what happens between the attachement points; I don't understand what happens there very well. I've seen about a similar number of mains fail near line attachement points as fail from blowouts in the center of a cell; I don't know if reserves are similar in that manner.
OK, the inverse square law is maybe a bad analogy but it is the only one I could think of at the time. But looking at diagrams of the inverse sq it does shed some lighton how a force is distribited over a larger area for the same load/ speed/ weight.
If more fabric is involved between the load attachment points (as in a bigger canopy) then a greater volume of material will available to absorb/ attenuate more of the shock loading than with a much smaller canopy. In addition to longer lines (more material), the larger cells (or more of them) and their accompaning load tapes will be scaled up accordingly, giving still more material to help absorb the load. This coupled with a longer fill time due to the larger cells, will further degrade the inital forces on the entire platform.
Take, for example a 20 lb load applied to a very very small canopy that causes it to fail during opening, that same 20 lb load applied to a much larger canopy will have little effect due to the attenuation charicteristics of the increased volume of material it has to overcome and its increased size which will increase the fill time dramaticly. It should be pointed out that a parachute doesn't just stop once it has been deployed, it undergoes a series of "slow down intervals". These are most often witnessed by the inflation (spreading) of the bottom skin which slows the load and brings it to a near vertical position, followed by the cell inflation which causes the wing to pressurize and start to take flight in a close to horizontal fashion. However the closer the intervals are together the quicker the opening will be.
When ram air canopies are scaled up it is not a linier process, there are many dynamics that are changed due to the scale up process. Cell size, performance, material considerations and angles all have to be re-calculated in order to produce similar results. All of this has a direct bearing on the loads felt and how they are distributed.
I'm not a canopy engineer (I'm a H/C engineer) but I've been around a few like Gary Douris and Ernie Villaneuva of Free Flight (Amigo reserves, Preserve reserves, BRS etc) and this what I personaly gleaned from them. Jerry B, you're a mechanical engineer, if you're listening (looking?) what is your take on it? Am I right or have I completly missed the mark?
The way I see it is; The more material and distance between the load points, the greater the attenuation properties of the article in question. Am I thinking correctly?
Bill, Jerry, your thoughts on the matter would be greatly appreciated.
Good discussion!!
Mick.
>stated: As the surface area insreases the energy of load is
>distributed over a greater area effectivly decreasing the overall
>load on any given point. Make sense?
Hmm, not to me.
The inverse-square law says that strength is inversely proportional to the square of the distance from the source of some radiation/force. It's more applicable to things like radiation than materials strength.
There's also the squared-cubed law, which states that strength goes up as a function of cross-sectional area (i.e. it's size squared) but weight goes up as a function of volume (i.e. it's size cubed.) Which is why ants can't be the size of elephants; their legs wouldn't hold them. But that doesn't seem to apply here either; the weight of a parachute is pretty negligible when compared to the overall system during opening.
So let's consider two 7-cell reserves, one 100 square feet and the other 200 square feet. Assume design is similar, exit weight is similar and opening speeds are similar. Each line sees a similar load; the collection of 40 lines going to the canopy still carries 100% of the load no matter what the canopy size, so each attachement point sees a similar loading. Since the construction of the line attach points, and the configuration nearest the line attachement point is the same in both canopy sizes, they would seem to resist failure near the attachement points equally well. (Unless I'm missing something, which is entirely possible.)
There's one caveat to the above. The final (post deployment) vertical speed of the larger reserve will be slower than the final vertical speed of the smaller reserve - so if opening _times_ are the same, I'd assume forces would be higher on the larger canopy (more deceleration required.) But there's nothing that says opening _times_ have to be the same, and indeed the amount of reefing would have a big effect on maximum loads seen.
However, all the above doesn't speak to what happens between the attachement points; I don't understand what happens there very well. I've seen about a similar number of mains fail near line attachement points as fail from blowouts in the center of a cell; I don't know if reserves are similar in that manner.
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