Abstract
The system of transfer equations in a two-phase medium reduces to a single effective equation which can be analyzed without significant difficulties (in comparison with the given system), with the accuracy of the problem formulation being practically preserved.
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Abbreviations
- Θ, t, x, u:
-
dimensionless temperature (pressure), time, coordinate, velocity
- Θ :
-
the value of x = 0
- a, ɛ, ν:
-
dimensionless parameters in (1)
- d:
-
parameter in (8)
- ξ:
-
self-similarity variable
- q:
-
debit (heat flux)
- χ:
-
piezoconductivity
- m°:
-
porosity at the initial pressure p°
- βp, βm :
-
compressibility factors of liquid and block pores
- σ:
-
critical pressure
- α:
-
dimensionless depression
- p:
-
parameter of the Laplace transform
- b(p):
-
function in (8)
- β(p), in (11), r0 :
-
dimensionless radius of a bore
- K:
-
operator in (5)
- L, L1 :
-
operators in (6)
- F(Θ 1):
-
function in (7)
- G(x, t):
-
function in (20)
- ▽:
-
gradient
- Δ:
-
the Laplace operator
- 1, 2:
-
refer to fissures and blocks
- a superscript bar:
-
the Laplace transform
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Translated from Inzhenerno-Fizicheskii Zhurnal, Vol. 54, No. 5, pp. 779–786, May, 1988.
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Nustrov, V.S., Saifullaev, B.N. A method of an equivalent equation in the theory of heat and mass transfer. Journal of Engineering Physics 54, 527–533 (1988). https://doi.org/10.1007/BF00872572
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DOI: https://doi.org/10.1007/BF00872572