Difference between revisions of "Gray correlation"

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(→‎Workflow \varepsilon')
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:<math> H_g = \frac{1-e^A}{R+1}</math>
 
:<math> H_g = \frac{1-e^A}{R+1}</math>
  
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== Workflow <math>\varepsilon'</math> ==
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== Workflow &epsilon;<sup>'</sup> ==
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&epsilon;
 
  
 
== Nomenclature  ==
 
== Nomenclature  ==

Revision as of 18:33, 4 April 2017

Brief

  • The boundary between the bubble and slug flow[1]

Math & Physics

Following the law of conservation of energy the basic steady state flow equation is:

144 \frac{\Delta p}{\Delta h} = \bar \rho_m + \rho_m \frac{f v_m^2 }{2 g_c D} + \rho_m \frac{\Delta{(\frac{v_m^2}{2g_c}})}{\Delta h}[1]

where

\bar \rho_m = \rho_L (1-H_g) + \rho_g H_g, slip mixture density
\rho_m = \rho_L C_L + \rho_g (1-C_L) , no-slip mixture density

Colebrook–White [2] equation for the Darcy's friction factor:

\frac{1}{\sqrt{f}}= -2 \log \left( \frac { \varepsilon'} {3.7 D} + \frac {2.51} {\mathrm{Re} \sqrt{f}} \right)[3]

Reynolds two phase number:

Re = 2.2 \times 10^{-2} \frac {q_L M}{D \mu_L^{H_L} \mu_g^{(1-H_L)}}

Discussion

Workflow Hg

N_V = 453.592\ \frac{{\rho_m}^2 {v_m}^4}{g_c \sigma_L (\rho_L - \rho_g)} [1]
N_D = 453.592\ \frac{g_c (\rho_L - \rho_g) D^2}{\sigma_L }
R = \frac{v_{SL}}{v_{SG}}
B = 0.0814 \left ( 1 - 0.554\ \ln \left (1 + \frac{730 R}{R+1} \right ) \right )
A = -2.2314 \left ( N_V \left (1 + \frac{205}{N_D} \right ) \right )^B
H_g = \frac{1-e^A}{R+1}

Workflow ε'

Nomenclature

NV velocity number

References

  1. ↑ 1.0 1.1 1.2 Gray, H. E. (1974). "Vertical Flow Correlation in Gas Wells". User manual for API 14B, Subsurface controlled safety valve sizing computer program. API. 
  2. ↑ Colebrook, C. F. (1938–1939). "Turbulent Flow in Pipes, With Particular Reference to the Transition Region Between the Smooth and Rough Pipe Laws"Paid subscription required. Journal of the Institution of Civil Engineers. London, England. 11: 133–156. 
  3. ↑ Moody, L. F. (1944). "Friction factors for pipe flow"Paid subscription required. Transactions of the ASME. 66 (8): 671–684. 
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