Difference between revisions of "Gray correlation"
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\frac{28.5}{453.592} \frac{\sigma_L}{\rho_m v_m^2}, &\mbox{if } R \geqslant 0.007 \\ | \frac{28.5}{453.592} \frac{\sigma_L}{\rho_m v_m^2}, &\mbox{if } R \geqslant 0.007 \\ | ||
\varepsilon + R \frac{\varepsilon'-\varepsilon}{0.0007}, & \mbox{if } R < 0.007 | \varepsilon + R \frac{\varepsilon'-\varepsilon}{0.0007}, & \mbox{if } R < 0.007 | ||
− | \end{cases} </math> with the limit <math> \varepsilon' \geqslant 2.77 \times 10^{-5}</math> <ref name= Gray/> | + | \end{cases} </math>, with the limit <math> \varepsilon' \geqslant 2.77 \times 10^{-5}</math> <ref name= Gray/> |
== Nomenclature == | == Nomenclature == |
Revision as of 18:48, 4 April 2017
Contents
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
- , slip mixture density
- , no-slip mixture density
Colebrook–White [2] equation for the Darcy's friction factor:
Reynolds two phase number:
Discussion
Workflow Hg
Workflow ε'
- , with the limit [1]
Nomenclature
NV velocity number
References
- ↑ 1.0 1.1 1.2 1.3 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.