Difference between revisions of "Gray correlation"
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== Workflow == | == Workflow == | ||
− | To find H<sub>g</sub> calculate: | + | To find H<sub>g</sub> calculate <ref name= Gray/>: |
− | :<math> N_V = 453.592\ \frac{{\rho_m}^2 {v_m}^4}{g_c \sigma_L (\rho_L - \rho_g)} </math | + | :<math> N_V = 453.592\ \frac{{\rho_m}^2 {v_m}^4}{g_c \sigma_L (\rho_L - \rho_g)} </math> |
− | :<math> N_D = 453.592\ \frac{q_c (\rho_L - \rho_g) D^2}{\sigma_L } </math | + | :<math> N_D = 453.592\ \frac{q_c (\rho_L - \rho_g) D^2}{\sigma_L } </math> |
== Nomenclature == | == Nomenclature == |
Revision as of 14:24, 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:
where
- = No-slip mixture density
Colebrook–White [2] equation for the Darcy's friction factor:
Reynolds two phase number:
Discussion
Workflow
To find Hg calculate [1]:
Nomenclature
References
- ↑ 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.
- ↑ Colebrook, C. F. (1938–1939). "Turbulent Flow in Pipes, With Particular Reference to the Transition Region Between the Smooth and Rough Pipe Laws". Journal of the Institution of Civil Engineers. London, England. 11: 133–156.
- ↑ Moody, L. F. (1944). "Friction factors for pipe flow". Transactions of the ASME. 66 (8): 671–684.