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Motivation


The most accurate way to simulate gas expansion is conventional 3D full-field dynamic modelling where gas expansion is treated as one of the fluid phases and accounts of geological heterogeneities, gas fluid properties, relperm properties and heat exchange with surrounding rocks.

Inputs & Outputs


InputsOutputs

p_i

Initial formation pressure

Q^{\downarrow}_{GC}(t)

Cumulative flux of gas from Gas Cap
V_{GC}(0)


Initial Gas Cap volume

q^{\downarrow}_{GC}(t) = \frac{dQ^{\downarrow}_{GC}}{dt}

Volumetric gas flowrate from Gas Cap

c_g(p)

Gas compressibility


Assumptions


Isothermal expansionUniform pressure depletion in Gas Cap

T = \rm const

p_{GC}(t) = p(t)


which leads to the following equation for  Gas Cap volume:

(1) V_{GC}(t) = V_{GC}(0) \cdot \exp \left[ - \int_{p_i}^{p(t)} c_g(p) dp \right]


Equations



(2) Q^{\downarrow}_{GC}(t) = V_{GC}(0) - V_{GC}(t) = V_{GC}(0) \cdot \left( \exp \left[ - \int_{p_i}^{p(t)} c_g(p) dp \right] - 1 \right)
(3) q^{\downarrow}_{GC}(t) = \frac{dQ_{GC}}{dt} = - V_{GC}(0) \cdot c_g \cdot \frac{dp}{dt} \cdot \exp \left[ - \int_{p_i}^{p(t)} c_g(p) dp \right]


Approximations



In case when pressure depletion \displaystyle \frac{p(t)}{p_i} is not severe then compressibility factor maybe considered as relatively constant  Z = \rm const which leads to  \displaystyle c_g = \frac{1}{p} and:

(4) Q^{\downarrow}_{GC}(t) = V_{GC}(0) \cdot \left( \frac{p_i}{p(t)} -1 \right)
(5) q^{\downarrow}_{GC}(t) = \frac{dQ_{GC}}{dt} = V_{GC}(0) \frac{p_i}{p^2(t)} \frac{dp}{dt}

 

See Also


Petroleum Industry / Upstream / Subsurface E&P Disciplines / Field Study & Modelling / Gas Cap Drive

Depletion ] [ Saturated oil reservoir ] 


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