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A method of an equivalent equation in the theory of heat and mass transfer

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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

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