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The flow through a valve can be calculated thanks to the pressure drop through the valve and a coefficient Kv which represents the number of m³/h of water that goes through the valve at 15°C and with a pressure drop of 1 bar.
Manufacturers may specify the coefficient Cv instead of Kv for their valve. Cv is the number of US gallons that goes through the valve at 60°F and with a pressure drop of 1 psi. It is actually possible to convert Kv and Cv and have the expression in the right unit for the calculation of interest.
\( C_v = 1.156 \cdot K_v \quad \Longleftrightarrow \quad K_v = 0.865 \cdot C_v \)
In order to calculate the flow of liquid through a valve thanks to the Cv, the Engineer must 1st determine if the flow is subcritical or critical (cavitation / flashing). To do so, it is necessary to compare the pressure drop to some limit values.
With:
\(\Delta P\) = Pressure drop across the valve (bar abs)
\(F_L\) = liquid pressure recovery factor = \(\sqrt{\frac{P_1 -
P_2}{P_1 - P_{VC}}}\)
\(P_1\) = upstream pressure (bar abs)
\(P_2\) = downstream pressure (bar abs)
\(P_{VC}\) = pressure at the vena contracta of the valve (bar abs)
\(\Delta P_s\) = critical pressure drop = \(P_1 - \left(0.96 - 0.28
\cdot \sqrt{P_v / P_c}\right) \cdot P_v\)
\(P_v\) = vapor pressure of the liquid at the flow temperature (bar
abs)
\(P_c\) = pressure at thermodynamic critical point (bar abs)
The relations given below are valid only for a Newtonian liquid in turbulent flow.
The volumetric flow of liquid through a valve can be calculated by \(Q_v = K_v \cdot \sqrt{\Delta P / d}\) or \(Q_v = \frac{C_v}{1.156} \cdot \sqrt{\Delta P / d}\) for subcritical flow.
With:
\(Q_v\) = Flow rate (m³/h)
\(C_v\) = valve flow coefficient (GPM)
\(K_v\) = valve flow coefficient (m³/h)
\(\Delta P\) = Pressure drop across the valve (bar)
\(d_{15}^t\) = density of the liquid referred to water at 15°C (-) -
as density of water at this temperature is 999.13 kg/m³,
\(d_{15}^t\) can be approximated as \(\rho / 1000\)
\(\rho\) = density of the liquid at flow temperature (kg/m³)
The mass flow rate through the valve can be calculated thanks to the formula \(C_v = \frac{1.156 \cdot \dot{m}}{\sqrt{d_{15}^t \times \Delta P}} \implies \dot{m} = \frac{C_v}{1.156} \cdot \sqrt{d_{15}^t \times \Delta P}\):
With \(\dot{m}\) = Flow rate (t/h).
For critical flow, the following formula can be used to calculate the volumetric flow through a valve of coefficient Cv:
For calculating the mass flow in critical flow:
A control valve has a Cv of 5. The instrumentation on the line shows that the pressure drop through the valve is 0.5 bar. What is the flow through the valve? It is water at 50°C.
The density of water at 15°C is 999.13 kg/m³.
The density of water at 50°C is 988.07 kg/m³.
The specific gravity of water at 50°C compared to water at 15°C is: 988.07 / 999.13 = 0.9889.
The flowrate is \(Q_v = \frac{C_v}{1.156} \cdot \sqrt{\Delta P / d} = \frac{5}{1.156} \cdot \sqrt{0.5 / 0.9889} = 3.07 \text{ m}^3\text{/h}\).
The volumetric flow rate of gas through a valve can be calculated from the valve Cv thanks to the following formula:
With:
\(Q_v\) = Flow rate (m³/h) at 15°C and 101,325 Pa abs
\(F_L\) = critical flow factor
\(C_v\) = valve flow coefficient (GPM)
\(P_1\) = upstream pressure (bar abs)
\(d\) = gas specific gravity vs air (\(d_{\text{air}} = 1\)) = \(M /
28.96\)
\(M\) = molar mass of the gas (g/mol)
\(T\) = temperature (K)
\(Z\) = compressibility factor (-)
\(y = \frac{1.63}{F_L} \cdot \sqrt{\frac{\Delta P}{P_1}}\)
The mass flowrate through the valve can be calculated thanks to the following formula:
With \(\dot{m}\) = Flow rate (t/h).
The formulas given above are valid when the valve diameter is equal to the pipe diameter. However, it sometimes happens that the valve is mounted in between pipe reducers, which reduces the effective capacity of the valve. To account for this effect, a coefficient \(F_p\), the piping geometry factor, is calculated. The actual required Cv is then:
\( C_{v,\text{corrected}} = \frac{C_v}{F_p} \)
With:
\(C_{v,\text{corrected}}\) = actual Cv of the valve between pipe
reducers
\(C_v\) = calculated Cv without pipe reducers
\(F_p\) = pipe geometry factor
\(d\) = valve diameter (mm)
\(\sum K = K_1 + K_2 + K_{B1} - K_{B2}\)
\(K_1\) = loss coefficient at inlet = \(0.5 \cdot \left[1 - (d /
D_1)^2\right]^2\)
\(K_2\) = loss coefficient at outlet = \(\left[1 - (d /
D_2)^2\right]^2\)
\(K_{B1}\) = Bernoulli coefficient = \(1 - (d / D_1)^4\)
\(K_{B2}\) = Bernoulli coefficient = \(1 - (d / D_2)^4\)
\(D_1\) = inside diameter of upstream pipe (mm)
\(D_2\) = inside diameter of downstream pipe (mm)
According to [Baumann], the correction of the valve Cv due to viscosity is to be applied only if the fluid has a kinematic viscosity > 40 centistokes. The correction procedure requires the calculation of a correction factor \(F_R\) which will be used in a similar way as the coefficient \(F_p\) for pipe geometry.
The case of laminar flow is according to Baumann calculated the same way as a correction of viscosity, which appears logical as a higher viscosity will often lead to laminar flow.
The relations above, in US customary units, are expressed in the following ways to calculate valves of Cv in liquid and gas applications:
With \(P\) and \(\Delta P\) in psi abs / psi, \(Q_v\) in US GPM (liquids) or SCFH (gas), \(C_v\) in GPM, \(\dot{m}\) in lb/h, \(d\) is specific gravity (water = 1 at 60°F), \(T\) flowing temperature in °R.
Source:
Masoneilan Control Valve Sizing Handbook, 2000