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Dynamic evolution computing of leakage and diffusion from pipeline gas and risk analysis

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Abstract

Urban gas pipelines are typically distributed in crowded areas among several people and buildings. The leakage of gas from damaged pipelines may result in significant property loss or casualties. Therefore, it is necessary to study the dynamic evolution characteristics of gas leakage and diffusion to quantify the harmful consequences and influence ranges of urban gas leakage and diffusion. To this end, through the analysis of the dynamic leakage process and pressure state of gas pipelines, a dynamic model of gas leakage is established by considering the sudden closure of the pipeline valve. According to the dynamic characteristics of the leakage rate, the Gaussian puff integral model is set up to simulate the dynamic diffusion of gas leakage. Combined with an actual case, the leakage and diffusion laws of urban gas pipelines caused by third-party damage to pipelines and the hazardous zone risk are quantitatively analyzed and characterized. The results indicate that the leakage rate decreases with continuous dynamic leakage time and the leakage and diffusion of pipeline gas result in certain hazardous zones. The concentration of the diffusion gas generally reaches a maximum value at a certain point and lasts for a period that corresponds to the time of steady sonic leakage. Timely detection of gas leakage and timely closing of the valve play an essential role in effectively slowing down and preventing the occurrence of serious accidents.

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Abbreviations

P α :

Atmospheric pressure, Pa

P c :

Critical pressure of the pipeline, Pa

K :

Isentropic index of gas

CPR:

Critical pressure ratio value

t s :

Beginning time of unsteady sonic flow of gas leakage, s

t c :

Beginning time of unsteady subsonic flow of gas leakage, s

t p :

End time of gas leakage, s

Q :

Leakage rate of gas, kg/s

M :

Leakage mass, kg

V :

Volume of the pipeline gas, m3

Ρ :

Density of gas in pipeline, kg/m3

C 0 :

Coefficient of the hole flow

A h :

Area of the hole, m2

M :

Molar mass of gas, kg/mol

Z :

Compression factor of the gas

R :

Constant of ideal gas, J/(mol·K)

T :

Gas temperature of the pipeline, K

P :

Pressure of the pipeline, Pa.

Q 0 :

Initial leakage rate at the fixed leakage time ts, kg/s

m 0 :

Initial mass at the fixed leakage time ts, kg

T 0 :

Initial temperature at the fixed leakage time ts, K

ρ 0 :

Initial density at a fixed leakage time ts, kg/m3

P 0 :

Initial pressure at the fixed leakage time ts, Pa

Q 0, sub :

Initial leakage rate for subsonic flow at a fixed leakage time tc, kg/s

m 0, sub :

Initial mass for subsonic flow at a fixed leakage time tc, kg

T 0, sub :

Initial temperature for subsonic flow at fixed leakage time tc, K

P 0, sub :

Initial pressure for subsonic flow at the fixed leakage time tc, Pa

Ci :

Gas concentration from the i-th puff mass at point (x, y, z), kg/m3

C :

Gas concentration at point (x, y, z), kg/m3

m i :

i-th puff mass during the leakage accident, kg

t' :

Any time corresponding to appearance of puff mass, s

σ x :

Diffusion coefficients in the x directions, m

σ y :

Diffusion coefficients from the y directions, m

σ z :

Diffusion coefficients from z direction, m

u :

Wind speed, m/s

H :

Effective source height, m

D :

Equivalent diameter of the failure hole

D :

Internal diameter of the pipeline, m

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Acknowledgments

This study was supported by the Qinzhou Scientific Research and Technology Development Project of Guangxi, China (No.20198513) and Project of Scientific Research Basic Ability Enhancement of Young and Middle-aged Teachers in Colleges and Universities of Guangxi, China (No. 2019KY0472).

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Correspondence to X. Zhou.

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Editorial responsibility: Chenxi Li.

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Zhou, X., Yang, D., Chen, X. et al. Dynamic evolution computing of leakage and diffusion from pipeline gas and risk analysis. Int. J. Environ. Sci. Technol. 20, 6091–6102 (2023). https://doi.org/10.1007/s13762-022-04366-7

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  • DOI: https://doi.org/10.1007/s13762-022-04366-7

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