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@wikipedia


A ratio between actual volumetric flowrate through the orifice and volumetric flowrate  estimate through the ideal orifice:

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C_d = \frac{q}{q_{\rm ideal}}

where

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q_{\rm ideal}= \epsilon \cdot \frac{\pi d^2}{4} \cdot \sqrt{\frac{2 \cdot \Delta p}{\rho \cdot (1-\beta^4)}}

and

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body\Delta p

pressure drop on the choke

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body\Delta p = p_{in} - p_{out}

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body\beta = \frac{d}{D}

choke narrowing ratio

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bodyd

orifice diameter

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bodyD

pipe diameter 

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body\epsilon

expansion factor


The deviation from ideal estimation 

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 arise from fluid friction with choke elements and possible flow turbulence.


The discharge coefficient 

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bodyC_d
 is a function of a choke narrowing ratio 
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body\beta
and Reynolds number 
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body{\rm Re}
:

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C_d = C_d(\beta, {\rm Re})

It can be estimated for popular choke types or tabulated in laboratory.


The most popular engineering correlation covering all ISO 5167 tapping arrangements is given by Discharge coefficient @ model:

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C_d = C_{d, \infty}(\beta) + b(\beta) \cdot {\rm Re}^{-n}


Device

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Nozzle, ISA 19320.9− 0.2262 · β4.11,70− 8,936 · β 19,779 · β4.71.15
Orifice, Corner Taps0.5950.0312 · β2.1​ − 0.184 · β691.71 · β2.50.75



See also


Physics / Fluid Dynamics / Pipe Flow Dynamics / Pipe Flow Simulation (PFS) / Pipeline Choke @model

Pipeline Engineering / Pipeline / Choke 


Reference


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Stolz
Stolz
Stolz,J.,"A Universal Equation for the Calculation of Discharge Coefficient  of Orifice Plates";, Proc. Flomeko 1978- Flow Measurement of Fluids,H. H. Dijstelbergenand E. A.Spencer(Eds), North-HollandPublishingCo.,Amsterdam(1978), pp 519-534


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https://neutrium.net/fluid_flow/discharge-coefficient-for-nozzles-and-orifices/


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C_d = \frac{d_D}{d} + 0.3167 \cdot \left( \frac{d}{d_D} \right)^{0.6} + 0.025 \cdot \big [ \log {\rm Re} - 4 \big ]