Hello all, seems I opened a can of worms here!
Just to update you, I have run a two types of experiments, none of which is going to be conclusive as I could only afford 4 wheels on my budget. I trued two wheels (to the best of my ability - I have trued wheels for repair and built one wheel before but would not say that they were up to a high quality) to a tension of 1638.27 Newtons, and two to 568.98 Newtons.
I then hung weights on them and with the weights available couldn't get the wheels to collapse (had 130KG) Unfortunately I couldn't afford strain gauges and the Park Tensiometer I had borrowed from the local bike shop was awkward to use on 20 inch 48 spoke wheels so couldn't get accurate readings of what was actually going on with the spokes. I then loaded two wheels in an Instron machine and loaded as a point load at the rim. The wheels showed a similar curve, but the failure modes were different. The spokes with the higher tension deformed more with a lower pressure applied than the lower tensioned wheel!
I then went back to hanging weights, this time measuring deflection. The results were similar for both (high and low tensioned wheels) for low loads (up to about 58N) the deflection of the wheel was similar. The lower tension wheel continues to deflect at a steady rate up to about 345N, whereas the rate of deflection of the higher tension wheel is reduced. The lower tension wheel continues to deform at a similar steady rate (slightly increased but not much), but the deformation rate of the higher tension wheel begins to accelerate at 4000N. At 5000N the deflection is the same and beyond this point the lower tension wheel continues to deform at a steady state but the higher tension wheel rapidly deforms. Saying that, we are talking 0.1's and less of a millimeter in difference between the high and low tensioned wheels, but these wheels were not loaded as it would be if somebody was sitting on them, so I think the deflections would be exagerated. The loads were also static loading, so again I think the deflections would be increased slightly, but not by much.
How I am understanding it (which I am not claiming to be right, I guess I'll wait and hear what the lecturers say about my findings) I think the tension in the spokes holds the shape of the wheel, but also brings the rim closer to the Euler's stress. I think this would explain why the tension in the spokes gives initial strength, but once the deflection goes beyond a certain point the wheel buckles due to Eulers buckling formula.
This would explain why the angle of the spokes makes a wheel laterally stronger, as it is being tied down like a tent (think of trying to hold a stick up right using guy ropes), so a wide flange hub would indeed increase the angle and make a stronger wheel.
I would have liked to try with more wheels and with different spoke gauges, but I cant really see why they would make much difference, other than greater ability to absorb energy, so I don't think in my static loading scenario it would make much difference.
Using Eulers buckling theory would also explain why deep rims are stiffer, having a greater second moment of area than a standard rim. So for laterally strong wheels a rim with a high second moment of area would be good.
I'm in the process of writing it up but thought I would share with you the raw results as soon as I had them
Cheers
Luke