Volumetric calculations
Following the definition of Solution GOR (Rs) and Vaporized Oil Ratio (Rv) :
so that:
q_O = q_{Oo} + R_v \, q_{Gg} |
| q_G = q_{Gg} + R_s \, q_{Oo} |
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Following the definition of Oil formation volume factor (Bo) , Gas formation volume factor (Bg) and Water formation volume factor (Bw):
so that:
q_O = \frac{q_o}{B_o} + R_v \,\frac{q_g}{B_g} |
| q_G = \frac{q_g}{B_g} + R_s \, \frac{q_o}{B_o} |
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and solving the above system of equations leads to:
q_o = \frac{B_o \cdot (q_O - R_v \, q_G)}{1- R_v \, R_s} |
| q_g = \frac{B_g \cdot (q_G - R_s \, q_O)}{1- R_v \, R_s} |
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Mass calculations
The oil phase includes oil component and gas component so that the oil phase mass flux is:
The gas phase includes gas component and oil component so that the gas phase mass flux is:
The water phase includes water component only so that the water phase mass flux is:
→
m_o = \rho_O \cdot q_{Oo} + \rho_G \cdot q_{Go} |
| m_g = \rho_G \cdot q_{Gg} + \rho_O \cdot q_{Og} |
| m_w = \rho_W \cdot q_{Ww} |
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→
m_o = \rho_O \cdot q_{Oo} + \rho_G \cdot R_s \, q_{Oo} |
| m_g = \rho_G \cdot q_{Gg} + \rho_O \cdot R_v \, q_{Gg} |
| m_w = \rho_W \cdot q_{Ww} |
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→
m_o = (\rho_O + \rho_G \cdot R_s) \cdot q_{Oo} |
| m_g = (\rho_G + \rho_O \cdot R_v) \cdot q_{Gg} |
| m_w = \rho_W \cdot q_{Ww} |
|
→
m_o = (\rho_O + \rho_G \cdot R_s) \cdot \frac{q_o}{B_o} |
| m_g = (\rho_G + \rho_O \cdot R_v) \cdot \frac{q_g}{B_g} |
| m_w = \rho_W \cdot \frac{q_w}{B_w} |
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→
\rho_o = \frac{\rho_O + \rho_G \cdot R_s}{B_o} |
| \rho_g = \frac{\rho_G + \rho_O \cdot R_v}{B_g} |
| \rho_w = \frac{\rho_W}{B_w} |
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The total mass flow of all phases:
\dot m = \dot m_o + \dot m_g + \dot m_w = (\rho_O + \rho_G \cdot R_s) \cdot \frac{q_o}{B_o} + (\rho_G + \rho_O \cdot R_v) \cdot \frac{q_g}{B_g} + \rho_W \cdot \frac{q_w}{B_w} |
→
\dot m = (\rho_O + \rho_G \cdot R_s) \cdot \frac{q_O - R_v \, q_G}{1-R_v \, R_s} + (\rho_G + \rho_O \cdot R_v) \cdot \frac{q_G - R_s \, q_O}{1- R_v \, R_s} + \rho_W \cdot q_W |
→
\dot m = \frac{ (\rho_O + \rho_G \cdot R_s)\cdot (q_O - R_v \, q_G) + (\rho_G + \rho_O \cdot R_v) \cdot (q_G - R_s \, q_O) }{1-R_v \, R_s} + \rho_W \cdot \frac{q_w}{B_w} |
→
\dot m = \frac{ \rho_O \, q_O \, (1- R_v \, R_s) + \rho_G \, q_G \, (1- R_v \, R_s) }{1-R_v \, R_s} + \rho_W \cdot q_W |
→
\dot m = \rho_O \cdot q_O + \rho_G \cdot q_G + \rho_W \cdot q_W = \dot m_O + \dot m_G + \dot m_W |
→
\dot m = \dot m_o + \dot m_g + \dot m_w = \dot m_O + \dot m_G + \dot m_W |
which means that total mass flux of all fluid phases is equal to the total mass flux of all fluid components.
As volatile oil model does not assume water-component exchange between phases the equality can be broken down into two equalities:
\dot m_{HC} = \dot m_o + \dot m_g = \dot m_O + \dot m_G |
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The total fluid density of Volatile Oil fluid @model is given by following equation (see Multiphase fluid for derivation):
\rho = s_o \, \rho_o + s_g \, \rho_g + s_w \, \rho_w |
The total fluid compressibility of multiphase fluid is given by following equation (see Multiphase fluid for derivation):
c = s_o \, c_o + s_g \, c_g + s_w \, c_w |
See Also
Petroleum Industry / Upstream / Subsurface E&P Disciplines / Fluid (PVT) Analysis / Fluid @model / Volatile Oil Fluid @model