I apologize if anyone didn't like my tone. The regulars on this forum all know a lot more about pumps then I ever will.
A small attempt to summarize the conclusions:
For a centrifugal pump attached to a fixed fluid system, the "operating point characteristics" (*) will follow the complete pattern Q~N, DP~N^2, FHP~N^3 if and only if the fluid system satisfies DP~Q^2
I think most agree with the above. Some comments/objections were raised:
1 – It is not likely that many fluid systems are fixed – often there is some control valve.
2 – Perhaps there are not a lot of systems that obey DP~Q^2 to begin with. Very turbulent systems do on a first view, although Snorty had some more comments on that. In any case more in depth analysis is usually in order than trying to give a simple generalization as this.
3 – Who cares
![[shadeshappy] [shadeshappy] [shadeshappy]](/data/assets/smilies/shadeshappy.gif)
* "operating point characteristics" represents change in operating point of the fixed system as a functio of speed. It is not to be confused with pump laws. Pump laws depend on the pump only, nothing to do with the system.
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