That's a misconception. Tensile strength has nothing to do with stiffness against deflection, which is governed by Young's (or Hook's, for europeans) modulus. This modulus hardly changes for most alloyed steels.
-Knut
True but this goes to the crux of the assertions being made by JS on need for a middle cam bearing and cam deflection and I will get to that in a minute. I have gone over Jim Comstock's excellent spintron work and in my opinion, the case has not been made for significant valve bounce due to cam rebound. I can speculate on what is being observed but will not go there now.
True, Young's Modulus is one governing factor in simple beam deflection analysis but a fundamental guidance on beam flexure is to also "check extreme fiber stress". In a simple static beam, this is a point calculation as a simple pass/fail for failure and appropriate safety factor and is dependent upon the ultimate strength of the material. With cam flexure, one needs to determine extreme fiber stress and put it into the context of a cyclic reversing load/stress which goes to the heart of this matter (based on my first hand experience in this particular application). As you may already know, below a certain threshold stress, steel exhibits an infinite durability; above that threshold, the steel exhibits a finite life. Above the threshold the greater the magnitude of the load reversals at the extreme fiber and/or number of load reversals, the shorter a steel components life.
Below is a cam we used for the 500 Norton USS phased for a 180 degree crank. The profiles were developed by Prof. Gordon Blair, the middle bearing was a Herb Becker concept implemented maybe 15 years ago (which may have been done before - e.g. Jim Comstock) from way back and the cam fabrication was by Megacycle.
Viewed from the timing side this cam rotates counterclockwise.
The cam breakage problems we were experiencing (pre middle bearing support) I now attribute to more or less two cam lobes (more or less mid beam) on the cam opening the RH EX and LH IN concurrently while coming off the LH exhaust. The double valve opening coupled with much greater spring rates and acceleration loads of the extremely high speed pushrod valve train resulted in a few caput cams. The middle bearing decisively resolved the cam breakage problem. We started the 500 USS with a 360 crank and did not experience cam breakage.
In contrast, rather than post a picture of a standard 360 cam, visualize the above cam picture looking from the timing chest, visualize the two RH cylinder lobes being rotated 90 degrees clockwise and you should be able to see that with the 360 phased (stock) cam, at no time is the cam lifting more than one valve at a time. So whatever high speed demands we were placing on the Commando camshaft, with the 180 degree cam we were more than doubling it. Again, the middle bearing fixed the breakage problem associated with the 180 degree phase and we did not experience this with the 360 phase crank.
With the 180 phase I am certain there were other goblins at work (snatch, vibration and harmonics) which were giving us fits. We kicked this can all the way to the point (e.g. gear driven cam) that the crankshaft timing pinon was the weakest link.
As best as I can tell, there's no direct nor indirect measurement of cam deflection (other than VR correlation) in Jim C's spintron work and from what I have seen it is open to interpretation as to exactly what role cam deflection plays in valve seat bounce as there's more than the cam in the valve train. It would be great if someone could reproduce/replicate the spintorn work with different valve head profiles and materials of construction. My hunch is it would be an eye opener. It would also be nice to be able to get the deflection data from 4StHead modeling software but my hunch is there are bigger fish to fry.