Art,
I am pleased you are back and active here again. I think the thread to which you are referring is thread798-135792 It was in the Chemical process engineering forum, which is probably why it did not result in much discussion.
My objection to the Crane 410 "K" values was that they are not applicable to laminar flow calculations, but Crane example 4-7 explicitly shows them being used for laminar flow. I recently got involved with some calculations for a liquid fertiliser plant where CMS (condensed molasses solids) was being pumped. The very high viscosities involved make this a definite laminar problem, and I found huge discrepancies between the various methods.
What really surprised me was that the "equivalent length" method, which tends to be looked down upon as an inferior short-cut method, was far better then using turbulent flow "K" values.
I put together a few examples to illustrate this, using a Sched 40 standard radius 90 degree welded elbow. The two fluids are water at 2 m/s (Reynolds = 205000) and molasses (visc = 4000 cP, Reynolds = 10.1).
For water I got:
Constant K = 0.3, press drop = 0.600 kPa
Equivalent length = 20, press drop = 0.749 kPa
Hooper 2-K method K = 0.316, press drop = 0.632 kPa
Darby 3-K method K = 0.335, press drop = 0.670 kPa
For molasses I got:
Constant K = 0.3, press drop = 0.019 kPa
Equivalent length = 20, press drop = 8.193 kPa
Hooper 2-K method K = 79.5, press drop = 5.136 kPa
Darby 3-K method K = 79.5, press drop = 5.136 kPa
In both cases the equivalent length method gives results that are a bit high, but in the ball-park. For laminar flow the Constant K method is out by a factor of 265. This is way beyond acceptable.
Back to the Cv to K conversion. I think the discrepancy you point out between the two Crane formulas is just rounding error. In my notes, where I worked to 4 significant digits I got a value of 29.83 in place of Crane's 29.9, and a value of 889.8 in place of their 891.0. In view of the other likely uncertainties I don't think it is too critical.
regards
Harvey