BigInch nailed the answer with his first post, but this question highlights what I consider to be one of the weaker points of the Crane 410 manual so please forgive me a little rant here. I have seen Crane's treatment of the K value for pipe fittings cause so much confusion - it really is a great pity they chose to do it this way.
The Crane engineers noted that the K values for fittings generally
decreased as the fitting size
increased. But it all went wrong when they noticed that this rate of decrease was close to the same as the rate at which the friction factor for fully developed turbulent flow in commercial steel pipe decreased as the pipe size increased. The fatal mistake was to link the two. See Crane Fig 2-14 and associated commentary.
For example, on page A-29 the K value for a 90 degree butt-weld pipe bend with an r/d of 1.5 is given as 14f
T. The values of f
T are given at the top of page A-26 as a function of pipe size. The values may have been calculated using the function referenced by vzeos, but for the purposes of calculating K values they are
constants for each pipe size.
This apparent link between the K value and the friction factor gives the impression that the K value is linked to the pipe roughness, but in fact it is not because f
T is
defined to be at a particular roughness. Even worse, it is possible to be mislead into believing the Crane K values compensate for changes in Reynolds number because everyone knows that the friction factor is influenced by the Reynolds number. But again, it is not because f
T is
defined to be in a particular Reynolds regime (fully turbulent).
To use the example of the 90 degree bend I gave above, it would have been better for Crane to give the K value as 14J, where J is simply a fudge-factor and would still be given by the values in the table on Page A-26
but without any reference to the friction factor. (Note that I have selected J as my symbol simply because it has no prior definition in the Crane Nomenclature table.)
The upshot of all of this is that in Crane's treatment, the K value of a fitting is a function
only of the pipe size (or geometry to use the terms used by wfn217 and BigInch). This was an improvement over previous work where the K value had been assumed to be constant for all sizes of fittings, and at the time that Crane first published this method it was rightly acclaimed as an important advance but IMHO it was badly worded and newer editions of 410 have unfortunately done nothing to remove the confusion.
I have awarded a star to BigInch for his comment that if you want to convert the Crane K value to an equivalent length, you must use the f
T value from Crane's table on page A-26 (which is based on a roughness of 0.0018") and
NOT the actual friction factor of the pipe you are using. The Crane description of this on pages 2-8 to 2-11 is extremely confusing, and the example 4-7 is just plain wrong because the K values given in the 410 manual apply only to fully developed turbulent flow and should never be used for laminar flow.
If you are working with laminar flow it is much better to work with equivalent lengths than with fixed or even Crane K values. Resistance values for fittings increase rapidly at low Reynolds numbers, but so does the friction factor. This means that if you use fixed L/D values, which get multiplied by the friction factor in the Darcy-Weisbach equation, the high resistance values are automatically compensated for. Or even better, use the 2-K or 3-K methods proposed by Hooper and Darby.
[Close rant mode - thanks for listening!]
Harvey
Katmar Software
Engineering & Risk Analysis Software