...Venturimeter... contd from previous slide
- If the pressure difference between Sections
1 and 2 is measured by a manometer as shown in Fig. 15.2,
we can write
where ρm is the density of the manometric liquid.
- Equation (15.7) shows that a manometer
always registers a direct reading of the difference in piezometric
pressures. Now, substitution of
from Eq. (15.7) in Eq. (15.6) gives
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(15.8) |
- If the pipe along with the venturimeter
is horizontal, then z1 = z2; and hence
becomes h1 − h2, where h1
and h2 are the static pressure heads
- The manometric equation Eq. (15.7) then
becomes
- Therefore, it is interesting to note
that the final expression of flow rate, given by Eq. (15.8),
in terms of manometer deflection ∆h, remains the same
irrespective of whether the pipe-line along with the venturimeter connection is horizontal or not.
- Measured values of ∆h, the difference
in piezometric pressures between Secs I and 2, for a real
fluid will always be greater than that assumed in case of
an ideal fluid because of frictional losses in addition
to the change in momentum.
- Therefore, Eq. (15.8) always overestimates
the actual flow rate. In order to take this into account,
a multiplying factor Cd, called the coefficient
of discharge, is incorporated in the Eq. (15.8) as
- The
coefficient of discharge
Cd is always less than unity and is defined as
where, the theoretical discharge
rate is predicted by the Eq. (15.8) with the measured value
of ∆h, and the actual rate of discharge is the discharge
rate measured in practice. Value of Cd
for a venturimeter usually lies between 0.95 to 0.98.
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