Last week we looked at something which initially seems straightforward but quickly becomes very difficult: sourcing the lightest possible springs suitable for a Human Powered Vehicle with a wheel suspension travel of about 100mm. As described in that story, I bench-tested torsion bars made from plastics, rubber and steel; I tested rubber in compression and shear; I tested a cantilever spring made from a carbon fibre snow ski and I even tested things like carbon fibre golf clubs. As a result of all this testing I decided I needed a spring with at least 75mm deflection (ie the motion ratio would be kept fairly low) and the lightest possible mass. But what sort of spring satisfied those criteria? What about air bags? Air Springs
So when I started to consider airbags for the new suspension trike, I went firstly to www.airbagman.com.au. That quickly led me to the Firestone site www.firestoneindustrial.com and from there I went to the data sheet for the 4001 Firestone Airstroke / Airmount – see www.firestoneindustrial.com/pdfs The Firestone 4001 air spring has a maximum diameter of 3.1 inches, a minimum length of 3.6 inches and a maximum length of 7.2 inches, giving a travel of 3.6 inches (91mm). The minimum air pressure that can be used is 10 psi; the maximum is 100 psi. Mass is quoted as 1 pound (450 grams) but is actually 350g. Unlike air shocks used in some mountain bikes - and air cylinders used in pneumatic machinery – these airbags don’t use a piston sliding in a precision cylinder, complete with precision seals everywhere. Instead, the construction is almost ridiculously simple. In the designs of airbag truck and bus suspension – and of the unit described here – the airbag rubber rolls back on itself rather like the way your mother bundled your socks together in your bedside drawer. A non-precision (but specially shaped) piston moves within the airbag rubber and as the piston extends, the rubber unrolls itself. Sufficient air pressure is needed to separate the rolling rubber walls (so explaining the minimum 10 psi) and the maximum travel is dictated at the different extremes of travel by (a) when the rubber nearly fully unrolls, and (b) when the piston and the opposite end mount nearly come in contact. With increasing air pressure, the diameter of the airbag expands slightly and, of course, applies more extension force. So, compared with steel coil springs, there are already three very important differences.
But I lot of that I found out subsequently – at this stage I was just wondering about the availability and cost of the Firestone 4001. Ouch!I rang The Airbag Man to find out both good and bad news. The good news was that the airbag was in stock and available. The bad news was that it had a retail price of AUD$300. That was about twice what I’d hoped for but it’s still much cheaper than local prices for esoteric mountain bike air shocks. (To give another comparison: the steel coil springs that I’d had custom made for my first trike had cost me AUD$77 each.) I ducked into Brisbane and picked up a Firestone airbag. My first reaction was that no way this looked like it should be worth AUD$300. But then when I got it home and started playing with it, I slowly changed my mind.
All Firestone’s literature suggests you shouldn’t inflate the airbag without it being constrained between stops. But that didn’t stop me connecting a high pressure bike pump and pumping a few strokes, only to find to my amazement and consternation that the airbag suddenly unrolled itself, popping fully open. Fortunately, with the right internal pressure applied, it’s easy enough to roll the airbag back over itself... Spring CharacteristicsA normal, constant rate spring compresses by the same increment when the same weight is placed on top. So a 1kg per millimetre spring will compress by 1mm when 1kg is placed on it, 2mm when 2kg is placed on top and so on. On the other hand, rubber (eg in compression) has a spring rate that rapidly rises – in fact, as you reach maximum compression, the rate is many tens of times higher than initially. Air springs are different again. As with rubber, the rate rises with compression. But the increase is much more progressive through the travel, which can also be quite long. This slowly rising rate characteristic of air springs makes aspects such as designing the ride height (and so setting the amount of bump and rebound travel available) much more complex than for linear rate springs. In fact, I found that despite having available pretty detailed specs sheets on the Firestone spring, by far the best data were gained by testing the spring’s characteristics in a mock-up suspension on the bench. Bench Testing
I initially tested the Firestone 4001 air spring with a simple bench-mounted set-up. A piece of timber was drilled horizontally at one end to take a long, snug-fitting (but not tight) bolt. The bolt was inserted through the timber and then its exposed end clamped in a large vice. At various points along the timber I drilled holes in which the top mount of the air spring could sit. Further along the timber I marked the spot where in the finished design the wheel will go. This set-up allowed the spring to be placed at various positions along the arm, so changing the motion ratio. By placing heavy steel weights on the top of the arm at the spot marked ‘wheel’ I could realistically create different loads, including static deflection, 1g vertical acceleration in bump (ie weight doubling) and other loads. In addition, by bouncing the arm on the spring, I could directly measure natural frequency and see how much damping was present. The first step was support the timber so that the air bag couldn’t be fully closed up (ie put in place a full bump stop) and then the second step was to place 30kg at the ‘wheel’. I then inflated the airbag until the airbag was about half way through its travel. (Incidentally, seeing the airbag inflate and then the load gently rise off the stop is a very interesting experience.) With the 30kg design load (ie the sprung weight of the trike and rider) applied through the appropriate length and ratio lever arm, I could then bounce the ‘wheel’ up and down and watch the system’s behaviour. However, it soon became clear that it wasn’t the normal ride weight which was the critical design factor, but instead the problem was coping with the 1g vertical bump, one which doubles the weight acting through the wheel. To simulate this, I loaded 60kg on the timber at the wheel position and then inflated the spring until the spring just lifted the weight off the bottom suspension stop. Then, without adding or subtracting air, I removed 30kg to return the load back to normal. With the load halved, the airbag extended to what would be the normal ride height position. Maximum bump and droop travel could then be measured from that position. Doing this showed that with the 4001 air spring, the closer that the motion ratio could be to 1:1 (ie wheel and spring movement the same), the better the system worked. However, the nearer that the motion ratio is 1:1, the closer the wheel travel matches the spring travel – so limiting wheel travel to being in this case the maximum travel of the air spring - 3.6 inches. A motion ratio of 1.3:1 was then used, which gave a maximum wheel travel of about 4.75 inches, distributed a little more in bump than droop.
Spring RatesAs indicated, the spring rate of an airbag changes with both static internal pressure and spring deflection. And, making things rather complex, the air pressures rises with deflection! Let’s take a look at that. With the spring supporting 30kg at a motion ratio of 1.3:1, about 30 psi gave a ride height roughly halfway through full travel. Pump the spring up harder and the ride height also increased – the spring was stiffer. But even with no air added or subtracted from the spring, the measured air pressure within the spring could double. How? When the spring was compressed! Adding more weight (the equivalent of experiencing a bump) compressed the air within the spring into a smaller space and so its pressure rose, so increasing the spring rate. This is what makes it so hard to work out what spring rate will be present at what deflection, and from what starting pressure. Firestone’s tech sheets do not show these figures. This varying rate is another reason why I suggest the spring pressure and motion ratio firstly be optimised for maximum bump.
Natural FrequenciesBecause of their internal air pressure change characteristics (and that’s purposely kept vague because I don’t fully understand the mechanism by which it occurs!), air bags have a very low resonant frequency. Depending on the motion ratio (and so the required air pressure), bench testing showed that frequencies in the range of 1.4 – 1.6Hz were quite possible. Translated, that means far better ride comfort without requiring a tall spring package.
ConclusionAir bags have some major advantages and disadvantages over alternative springs. (And I think that applies for cars as well as HPVs!) The advantages are:
The disadvantages are:
But there’s one other killer advantage that I discovered on the test bench, an advantage that I think makes the disadvantages pale into insignificance. That advantage is that the behaviour of airbags can be dramatically changed with simple valving... Next week: interconnected suspension systems Share this Article:
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