
8.54 CHAPTER EIGHT
indicated that minor losses vary approximately as the square of the velocity through
the fittings.
VALVES AND STANDARD FITTINGS
The resistance to flow through valves and fittings may be
found in References 4, 5, 17, and other sources. Losses are usually expressed in terms of
a resistance coefficient K and the average velocity head in a pipe having the same diam-
eter as the valve or fitting. The frictional resistance h in feet (meters) is found from the
equation
(20)
where K resistance coefficient, which depends on design and size of valve or fitting
V average velocity in pipe of corresponding internal diameter, ft/s (m/s)
g acceleration of gravity, 32.17 ft/s
2
(9.807 m/s
2
)
A comparison of the Darcy-Weisbach equation (Eq. 16) with Eq. 20 suggests that K
equals f(L/D), where L is the equivalent length of pipe in feet (meters) and D is the inside
pipe diameter in feet (meters), to produce the same head loss in a straight pipe as through
a valve or fitting. The friction in an “equivalent length of pipe” has been another method
used to estimate head loss through valves and fittings. Values of the ratio L/D have been
experimentally determined. This ratio multiplied by the inside diameter of a pipe of spec-
ified schedule for the valve or fitting being considered gives the equivalent length of pipe
to use to calculate the head lost.
Loss of head in straight pipe depends on the friction factor or Reynolds number. How-
ever, with valves and fittings, head is lost primarily because of change in direction of flow,
change in cross section, and obstructions in the flow path. For this reason, the resistance
coefficient is practically constant for a particular shape of valve or fitting for all flow con-
ditions, including laminar flow. The resistance coefficient would theoretically be constant
for all sizes of a particular design of valve or fitting except that all sizes are not geometri-
cally similar. The Crane Company has reported the results of tests that show that the
resistance coefficient for a number of lines of valves and fittings decreases with increas-
ing size at flow conditions of equal friction factor and that the equivalent length L/D tends
to be constant for the various sizes at the same flow conditions.
When available, the K factor furnished by the valve or fitting manufacturer should
always be used rather than the value from a general listing. The Hydraulic Institute lists
losses in terms of K through valves and fittings (Tables 5a to 5c); these losses vary with
size of the valve or fitting but are independent of friction factor. The Crane Company pro-
vides a similar listing of K values (Tables 6a to 6e). The latter listing of flow coefficients is
associated with the velocity head V
2
/2g that would occur through the internal diameter of
the schedule pipes for the various ANSI classes of valves and fittings shown in Table 6e.
If the connecting pipe is of a different size or schedule, either use the velocity for the pipe
shown in Table 6a or use the actual pipe velocity head and correct the resistance coeffi-
cient obtained from this table by the multiplier
Tables 6 are based on the use of an equivalent length constant for complete turbulent
flow for each valve or fitting shown.This constant is shown as the multiplier of the friction
factor f
T
for the corresponding clean commercial steel pipe with completely turbulent flow.
The product (L/D)(f
T
) is the coefficient K. The friction factors are given in Table 6a for dif-
ferent pipe sizes, or they can be obtained from Figure 31 or 32. If the valve or fitting has a
sudden or gradual contraction, enlargement, or change in direction of flow, appropriate for-
mulas for these conditions are given for the determination of K. If flow is laminar, valve
and fitting resistance coefficients are obtained from Table 6a based on completely turbu-
a
Actual pipe ID
Standard pipe ID
b
4
h K
V
2
2g