ipsys,
I was able to download the following article from the Delft web page:
Lavooij, C.S.W.;Koetzier, H.;Kruisbrink, A.C.H., Dynamic behaviour of large non-return valves., 5th International Conf. on Pressure Surges, Hanover, F.R. Germany, 22-24 September, 1986. (co-authors), 1986.
This paper provides "dynamic characterisric" curves which plot the maximum reverse fluid velocity against the average fluid deceleration during check valve closure. Once the maximum reverse velocity is known, the waterhammer pressure can be calcualted using the Joukowsky equation: dP = rho*u*a, where dP is the waterhammer pressure rise, rho is the fluid denisty, u is the fluid velocity, and a is the sonic velocity in the fluid.
I will compare results from the "fluid float" model I mentioned previously against the experimetntally determined dynamic characteristic curves presented in the Delft paper. I will provide another post with the results of this comparison.
Tremolo.