QUOTE (Chucktown PE @ Aug 4 2009, 04:00 PM)

I think you know what I mean. Bottom line is that from one end of the pipe to the other the water loses 50 feet of energy.
I don't know what you mean... because it's only true that from one end of the pipe to the other, the water loses 50 feet of POTENTIAL energy. The point to all this discussion isn't to argue what's the right answer, but to explain what the right approach is. I suggest it's bad advice to discount the KINETIC energy out of hand, even if it doesn't make much of a difference here. I recommend always starting with the Energy Equation and then simplify to Bernoulli... canceling the terms that you want to discount given certain assumptions.
QUOTE (Chucktown PE @ Aug 4 2009, 04:00 PM)

Okay, leave the velocity head in, but then the problem becomes an iterative solution. Please provide a solution doing it your way.
Well, yeah... that's what I said in one of my first posts! Then I suggested using Darcy-Weisbach which gives the friction loss in terms of V
2 which can easily be combined algebraically with the velocity head. I don't think you really need me to work that out being as I already gave the answer. Using your approach, you could easily calculate the velocity and friction head for various velocities, including the one you get assuming the velocity head is negligible.
And yeah, I know the problem said to use Hazen-Williams, but you shouldn't get a radically difference answer seeing as they are both derived from de Chezy.
Again, the discussion is about helping the OP understand how to approach these problems. If you think something with my recommended approach is wrong, please speak up! I'm certainly not shy about speaking up where I think a part of your approach is wrong - EVEN if I agree with your answer (and the implicit assumption that velocity head is negligible compared to the friction head).