CN112214943B - Method for calculating nitrogen flow dynamic pressure loss of three-dimensional simulated coal mine goaf - Google Patents

Method for calculating nitrogen flow dynamic pressure loss of three-dimensional simulated coal mine goaf Download PDF

Info

Publication number
CN112214943B
CN112214943B CN202011146211.8A CN202011146211A CN112214943B CN 112214943 B CN112214943 B CN 112214943B CN 202011146211 A CN202011146211 A CN 202011146211A CN 112214943 B CN112214943 B CN 112214943B
Authority
CN
China
Prior art keywords
flow
pressure loss
goaf
dimensional
diameter
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Active
Application number
CN202011146211.8A
Other languages
Chinese (zh)
Other versions
CN112214943A (en
Inventor
陈世强
张连会
赵利群
王君
王海桥
鲁义
姜文
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Hunan University of Science and Technology
Original Assignee
Hunan University of Science and Technology
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Hunan University of Science and Technology filed Critical Hunan University of Science and Technology
Priority to CN202011146211.8A priority Critical patent/CN112214943B/en
Publication of CN112214943A publication Critical patent/CN112214943A/en
Application granted granted Critical
Publication of CN112214943B publication Critical patent/CN112214943B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Images

Classifications

    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F30/00Computer-aided design [CAD]
    • G06F30/20Design optimisation, verification or simulation
    • G06F30/28Design optimisation, verification or simulation using fluid dynamics, e.g. using Navier-Stokes equations or computational fluid dynamics [CFD]
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F2113/00Details relating to the application field
    • G06F2113/08Fluids
    • GPHYSICS
    • G06COMPUTING; CALCULATING OR COUNTING
    • G06FELECTRIC DIGITAL DATA PROCESSING
    • G06F2119/00Details relating to the type or aim of the analysis or the optimisation
    • G06F2119/14Force analysis or force optimisation, e.g. static or dynamic forces

Landscapes

  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Theoretical Computer Science (AREA)
  • Mathematical Physics (AREA)
  • Fluid Mechanics (AREA)
  • Mathematical Analysis (AREA)
  • Mathematical Optimization (AREA)
  • Computing Systems (AREA)
  • Pure & Applied Mathematics (AREA)
  • Computer Hardware Design (AREA)
  • Evolutionary Computation (AREA)
  • Geometry (AREA)
  • General Engineering & Computer Science (AREA)
  • Algebra (AREA)
  • Management, Administration, Business Operations System, And Electronic Commerce (AREA)

Abstract

The invention discloses a method for calculating nitrogen flow dynamic pressure loss of a simulated three-dimensional coal mine goaf. The method mainly comprises the following steps: establishing a goaf gas flow model, and dividing a single-period flow unit; taking the single-period flow unit as a research object, and dividing the single-period flow unit into four flow stages according to different expressions of the section area changing along with the flow distance; deducing a theoretical calculation formula of nitrogen flow pressure loss in the goaf; on the basis of a theoretical calculation formula, experimental optimization is carried out, the difference between one-dimensional simplification and three-dimensional flow is reduced, and a pseudo three-dimensional flow pressure loss calculation formula is obtained. The method can be used for calculating the nitrogen flow dynamic pressure loss in the goaf, realizes the quick and accurate calculation of the initial pressure and the filling range required by goaf nitrogen filling, and avoids the defects of more time consumption and large technical difficulty of a numerical simulation method.

Description

Method for calculating nitrogen flow dynamic pressure loss of three-dimensional simulated coal mine goaf
Technical Field
The invention belongs to the technical field of mine ventilation and goaf disaster prevention and reduction, and particularly relates to a pseudo-three-dimensional coal mine goaf nitrogen flow dynamic pressure loss calculation method.
Background
Over 70% of coal mine fire accidents occur in goafs adjacent to the mining area. The natural fire of the left coal in the goaf and the fire extinguishing and disaster relief thereof are always hot problems in the industry, and the most common and effective fire extinguishing measure is to adopt nitrogen injection to treat the natural fire. However, the existing calculation method and implementation rules cannot accurately calculate the flowing distance of the injected nitrogen for fire extinguishing in the goaf, so that the influence range of the injected nitrogen cannot be accurately predicted, and liquid nitrogen waste and fire extinguishing difficulty are caused.
In the aspect of research progress of determining a method and measures for nitrogen injection parameters of a goaf, Ledong et al provides a fire prevention and extinguishing method for full-section curtain nitrogen injection of a U-shaped ventilation working surface of the goaf, and nitrogen inerting efficiency is improved. The automatic control rotary traction type nitrogen injection fire prevention and extinguishing device is invented by vermilion green, continuity of nitrogen injection points in the goaf on the space is achieved, and the inerting effect of nitrogen injection in the goaf is improved. According to the method, leakage stoppage, wind control and rapid inerting cooling are integrated, and spontaneous combustion of the residual coal is efficiently prevented. Guojunliu discusses the observation of three zones in the goaf and the practical method of nitrogen injection fire prevention and extinguishing, and improves the safety and economic benefit of coal mining. And establishing a theoretical fluid mechanics model of the gas volume fraction change of the goaf by cinnabar according to mass, momentum and component conservation equations, and determining the optimal nitrogen injection position and nitrogen injection amount through numerical simulation by initialization, boundary value assignment and iterative calculation. The Lizong combined section Wang coal mine performs nitrogen injection fire prevention and extinguishing simulation in a 'two-in-one' complex stope goaf, and determines the optimal nitrogen injection amount and nitrogen injection position. And Hojunzhong determines the air leakage rate of the gob of the macrorock coal mine 4405 through SF6 tracer gas, determines the main air leakage direction, and optimizes the gob nitrogen injection process on the basis. Zhang Qi combines the actual situation of coal valley mine site of the DaTong coal mine group company, and proposes to adopt a bypass type nitrogen injection method to treat the fire hazard in the goaf of the fully mechanized caving face by researching the fire hazard treatment technology of the fully mechanized caving face. Aiming at a high-gas easily self-combustible coal seam, Roxinglong takes a certain fully-mechanized mining face as a prototype, and a computational fluid mechanics code with an extraction hole is developed secondarily. And the Liu Star Queen simulates the change condition of the spontaneous combustion zone range of the goaf before and after nitrogen injection by using Fluent software, analyzes the influence of the nitrogen injection position and the nitrogen injection amount on the position distribution of the oxidation zone of the goaf, and fits the optimal nitrogen injection parameter. The Dongjun establishes a mathematical physical model of a goaf seepage field according to a basic theory of computational fluid mechanics in order to determine the optimal technological parameters for continuous nitrogen injection fire prevention and extinguishing in a goaf of a 5-2S-2 fully mechanized caving face, and performs numerical simulation research on goaf oxygen concentration distribution and three-band division under different nitrogen injection conditions to obtain the optimal nitrogen injection parameters. The research is an important foundation for preventing and controlling spontaneous ignition of the goaf, but the method and the device have problems if applied to actual engineering. Firstly, as the physical property parameters and the production process parameters of different goafs of different coal mines are different, the method for determining the nitrogen injection parameters by numerical simulation consumes more time and has high technical difficulty and difficult popularization; secondly, the above studies cannot clarify the quantitative relationship between the pressure loss and the nitrogen injection parameters in the nitrogen flowing process, so that the specific parameters of nitrogen injection cannot be determined quickly. In order to overcome the defects, the invention provides a goaf nitrogen filling pressure loss calculation method based on a minimum flow unit. However, in this method, the three-dimensional flow is simplified to the one-dimensional flow to obtain a pressure loss calculation method, and the pressure loss calculated by this method has a certain error from the actual situation.
Disclosure of Invention
The invention aims to provide a method for calculating the nitrogen flow dynamic pressure loss of a simulated three-dimensional coal mine goaf after test optimization aiming at the defects in the prior art.
The invention discloses a method for calculating nitrogen flow dynamic pressure loss of a simulated three-dimensional coal mine goaf, which comprises the following steps of:
(1) establishing a goaf gas flow model, and dividing a single-period flow unit;
(2) taking the single-period flow unit as a research object, and dividing the single-period flow unit into four flow stages according to different expressions of the section area changing along with the flow distance;
(3) deducing a theoretical calculation formula of nitrogen flow pressure loss in the goaf;
according to a hydrodynamic Navier-Stocks equation, a one-dimensional flow pressure loss calculation formula is derived as shown in a formula (1):
Figure BDA0002739812890000031
in the formula, JT1Is the one-dimensional flow pressure loss of gas flowing through a gob with unit length, Pa/m; μ is the dynamic viscosity of the gas, pas; rho is gas density, kg/m3(ii) a d is the diameter of the pellet, m; u. of0Is the initial average velocity of the gas, m/s;
(4) on the basis of a theoretical calculation formula, carrying out experimental optimization, reducing the difference between one-dimensional simplification and three-dimensional flow, and obtaining a calculation formula of the pseudo-three-dimensional flow pressure loss as shown in a formula (2):
Figure BDA0002739812890000032
in the formula, JT3The pressure loss is the simulated three-dimensional flow pressure loss of gas flowing through a gob with unit length, and is Pa/m; k is a correction proportion coefficient, and is 0.52 without a dimensional number; alpha is a velocity distribution coefficient and is a dimensionless number.
Specifically, the step (1) comprises the following steps:
(a) establishing a goaf gas flow model;
the gas flow model was built up from 8 large spheres of diameter d, one with diameter
Figure BDA0002739812890000033
The loose core sphere and 6 diameters are
Figure BDA0002739812890000034
The semi-hollow sphere; the eight cubic vertexes with the side length of 2d are respectively provided with 8 large balls with the diameter d, and each large ball with the diameter d is tangent to the adjacent large ball with the diameter d; diameter of
Figure BDA0002739812890000035
The core-pulling ball body is positioned at the center of 8 large balls with the diameter d and is tangent with the 8 large balls with the diameter d respectively; 6 have a diameter of
Figure BDA0002739812890000036
The core-pulling hemispheroids are respectively positioned at the central positions of six surfaces of the cube, and the diameter of each core-pulling hemispheroid is
Figure BDA0002739812890000037
The core-pulling hemispheroid is tangent with the surrounding spherical surface;
(b) dividing the single-cycle flow units;
by the symmetry of the flow model, the goaf gas flow model can be divided into single-period flow units, specifically: and cutting the flow model into eight single-period flow units by taking the middle point of each edge of the cube with the side length of 2d as a cutting point.
Specifically, the step (2) comprises the following steps:
taking a single-period flow unit as a research object, wherein the flow direction is the positive direction of a z axis, and the flow starting point is the origin of the z axis; in the first flow stage, starting from the point where z is 0, the flow cross-sectional area expression is as shown in formula (3):
Figure BDA0002739812890000041
wherein A is0Is the cross-sectional area of flow, m2(ii) a d is the diameter of the pellet, m; l is a connecting line from the center of the cutting cylinder to the circumference of the bottom surface, and m is the length of the connecting line; theta is the included angle and radian between the dotted line L and the central axis of the cutting cylinder.
The flow cross-sectional areas of the four flow stages are respectively as follows:
when it is satisfied with
Figure BDA0002739812890000042
The method comprises the following steps:
Figure BDA0002739812890000043
when it is satisfied with
Figure BDA0002739812890000044
The method comprises the following steps:
Figure BDA0002739812890000045
when it is satisfied with
Figure BDA0002739812890000046
The method comprises the following steps:
Figure BDA0002739812890000047
when it is satisfied with
Figure BDA0002739812890000048
The method comprises the following steps:
Figure BDA0002739812890000049
specifically, the step (3) comprises the following steps:
(a) the pressure loss per unit length for each flow stage is calculated as follows:
a first flow stage:
Figure BDA0002739812890000051
a second flow stage:
Figure BDA0002739812890000052
a third flow phase:
Figure BDA0002739812890000053
a fourth flow phase:
Figure BDA0002739812890000054
wherein μ is the kinetic viscosity of the gas, pas; rho is gas density, kg/m3(ii) a d is the diameter of the pellet, m; u. of0Is the initial average velocity of the gas, m/s;
(b) determining a theoretical calculation formula of the loss of the nitrogen flow pressure of the goaf as follows:
integrating the formulas of the four flowing stages according to the length proportion of the model to obtain a pressure loss calculation formula of the last flowing period of the minimum flowing unit:
Figure BDA0002739812890000055
specifically, the step (4) comprises the following steps:
(a) based on a test bed, setting four different wind paths so as to obtain four different flow section areas, and setting the four conditions as four different working conditions;
(b) measuring actual measurement pressure loss under different wind speeds of each working condition and theoretical pressure loss calculated according to the formula (1);
(c) comparing the measured pressure loss with the theoretical pressure loss, and solving the difference between the one-dimensional simplification and the three-dimensional flow by using a speed distribution coefficient alpha;
(d) and dividing the theoretical pressure loss and the actual pressure loss to obtain a correction proportion coefficient K.
Compared with the prior art, the invention has the beneficial effects that:
the method can be used for calculating the nitrogen flow dynamic pressure loss in the goaf, realizes the quick and accurate calculation of the initial pressure and the filling range required by goaf nitrogen filling, and avoids the defects of more time consumption and large technical difficulty of a numerical simulation method.
Drawings
FIG. 1 is a front view of a goaf gas flow model in an embodiment of the present invention.
FIG. 2 is a left side view of a goaf gas flow model in an embodiment of the present invention.
Figure 3 is a top view of a goaf gas flow model in an embodiment of the present invention.
FIG. 4 is a schematic diagram of a cut pellet cylinder according to an embodiment of the present invention.
FIG. 5 is a block diagram of a single cycle flow cell in accordance with an embodiment of the present invention.
Fig. 6 is a flow phase profile for an embodiment of the present invention.
FIG. 7 is a block diagram of an experimental platform according to an embodiment of the present invention.
FIG. 8 is a graph of measured pressure loss versus theoretical pressure loss under the first operating condition of the embodiment of the present invention.
FIG. 9 is a graph of measured pressure loss versus theoretical pressure loss for a second operating condition in accordance with an embodiment of the present invention.
FIG. 10 is a graph of measured pressure loss versus theoretical pressure loss under a third condition in accordance with an embodiment of the present invention.
Fig. 11 is a graph of the measured pressure loss and the theoretical pressure loss in the fourth operation of the embodiment of the present invention.
FIG. 12 is a graph of the proportionality coefficient of the calculated pressure loss and the measured pressure loss under the first operating condition of the embodiment of the present invention.
FIG. 13 is a graph of the proportionality coefficient of the calculated pressure loss and the measured pressure loss under the second operating condition of the embodiment of the present invention.
FIG. 14 is a graph of the proportionality coefficient of the calculated pressure loss and the measured pressure loss under the third operating condition in accordance with the exemplary embodiment of the present invention.
Fig. 15 is a graph of a proportionality coefficient of the calculated pressure loss and the measured pressure loss in the fourth operating mode according to the embodiment of the present invention.
Detailed Description
The present invention will be described in further detail with reference to the accompanying drawings and examples.
The specific implementation steps of this embodiment are as follows:
(1) and establishing a goaf gas flow model and dividing the single-period flow units.
For a cube with a side length of 2d, it is exactly capable of accommodating 8 spheres with a diameter of d, the loosest arrangement is that the spheres are tangent to each other and to the sides of the cube, and the porosity of the cube containing 8 spheres is 1-pi/6, which is about 0.4764; then, 8 large-diameter spheres with the diameter d and 4 spheres with the diameter d
Figure BDA0002739812890000071
The porosity of the flow model formed by the small-diameter spheres is 0.3737; the two models are set as uniform porous media with equivalent porosity, and in order to better reflect the heterogeneity of the porous media in the goaf, the cylinder shown in the figure 4 is used in the inventionCutting the small-diameter ball of the second model to obtain the porosity:
Figure BDA0002739812890000072
in fig. 4, L is a line connecting the center of the cutting cylinder to the circumference of the bottom surface, m; r is the diameter of the bottom surface of the cutting cylinder, m; theta is the included angle and radian between the dotted line L and the central axis of the cutting cylinder.
Thus, a gas flow model was created as shown in FIGS. 1-3, consisting of 8 large spheres of diameter d, one with a diameter of
Figure BDA0002739812890000073
The loose core sphere and 6 diameters are
Figure BDA0002739812890000074
The core-pulling hemisphere. The eight cubic vertexes with the side length of 2d are respectively provided with 8 large balls with the diameter d, and each large ball with the diameter d is tangent with the adjacent large ball with the diameter d; diameter of
Figure BDA0002739812890000075
The core-pulling ball body is positioned at the center of 8 large balls with the diameter d and is tangent with the 8 large balls with the diameter d respectively; 6 have a diameter of
Figure BDA0002739812890000076
The core-pulling hemispheroids are respectively positioned at the central positions of six surfaces of the cube, and the diameter of each core-pulling hemispheroid is
Figure BDA0002739812890000077
The core-pulling hemispheroid is tangent with the surrounding spherical surface.
Due to the symmetry of the flow model, the goaf flow model can be divided into monocycle flow units in order to simplify theoretical derivation. The method specifically comprises the following steps: the middle point of each edge of the cube with the side length of 2d is taken as a cutting point, and the flow model is cut into eight single-period flow units, as shown in fig. 5.
(2) The single-period flow unit is taken as a research object, the flow direction is the positive direction of the z axis, and the flow starting point is the origin of the z axis. In the first flow phase, starting from the point where z is 0, the initial flow cross-sectional area a0The expression is as follows:
Figure BDA0002739812890000081
the flow cross-sectional areas of the four flow stages are respectively as follows:
when it is satisfied with
Figure BDA0002739812890000082
The method comprises the following steps:
Figure BDA0002739812890000083
when it is satisfied with
Figure BDA0002739812890000084
The method comprises the following steps:
Figure BDA0002739812890000085
when it is satisfied with
Figure BDA0002739812890000086
The method comprises the following steps:
Figure BDA0002739812890000087
when it is satisfied with
Figure BDA0002739812890000088
The method comprises the following steps:
Figure BDA0002739812890000089
according to different relations of the flow cross-section area along with z, different flow stages are divided, and when the flow cross-section relations of the formulas (4), (5), (6) or (7) are respectively met, the flow stages are called as a first flow stage, a second flow stage, a third flow stage or a fourth flow stage, as shown in fig. 6, so that a micro-flow process in the single-cycle flow unit is formed.
(3) According to a fluid dynamics Navier-Stocks equation, deriving a pressure loss calculation formula per unit length in the four flow stages; the single cycle flow cell porosity was set at 0.4317, then the pressure loss per unit length for each flow phase was:
a first flow stage:
Figure BDA00027398128900000810
a second flow stage:
Figure BDA0002739812890000091
a third flow phase:
Figure BDA0002739812890000092
a fourth flow phase:
Figure BDA0002739812890000093
the formula of the four stages is integrated according to the length proportion of the model to obtain a one-dimensional pressure loss calculation formula of the previous flow period of the single-period flow unit:
Figure BDA0002739812890000094
(4) the method for calculating the nitrogen flow dynamic pressure loss in the goaf is further optimized through experiments, and specifically comprises the following operations:
the experimental platform is shown in FIG. 7, wherein 1-6 are valves; a is a variable frequency fan; A-E is an air duct, wherein A, B, C, D is filled with ceramsite, E is not filled with ceramsite, A and B, E are separated by a non-porous partition plate, and B, C, D, E is separated by a porous partition plate; f is an air inlet pipeline, and G is an air outlet pipeline.
(a) And (4) detecting the porosity of the ceramsite system used in the experiment and checking whether air leaks or not by using an experiment platform. The porosity of the ceramsite system model is measured by a drainage method, which specifically comprises the following steps: placing the ceramsite sample into a large measuring cylinder, and recording the volume of the ceramsite sample as V1Pouring water with a certain volume into a large measuring cylinder by using a small measuring cylinder to ensure that the water is level with the ceramsite sample, and recording the volume as V2Then the porosity of the ceramsite sample is V2/V1The measurement result was 43.17%; the method for detecting air leakage by using the stage spraying agent and the spray tobacco tar specifically comprises the following steps: firstly, mixing spray tobacco tar and distilled water in a ratio of 1:4, then pouring the mixture into a stage sprayer, simultaneously placing the spray into an air inlet of a system, then opening a fan, after the fan stably runs for a period of time at a low wind speed, opening the stage sprayer to release smoke, enabling the smoke to slowly enter an air duct of the system, observing whether white smoke emerges from the joint of an experimental platform, and if so, ensuring that the air tightness is poor and further repairing is needed.
(b) Based on an experimental platform, setting four different wind paths and measuring four different flow section areas, as shown in fig. 7, wherein 2 and 5 valves are opened, and the rest are closed to be a first working condition; 1. 4, opening the valve, and closing the rest valves to be a second working condition; 2. opening the valve 6, and closing the rest valves to form a third working condition; 3. 5, opening the valve, and closing the rest valves to form a fourth working condition; meanwhile, a pitot tube connected with a micro-manometer is correctly arranged at the inlet and outlet positions of the goaf experiment table according to the specific conditions of each working condition for measuring pressure loss; and then installing the multifunctional ventilation meter at the air inlet for measuring the air speed at the inlet.
(c) After the experimental equipment is connected, the fan is started, the frequency conversion electric control cabinet is directly switched to frequency conversion operation, and the size of the inlet air speed is adjusted by manually adjusting the knob. After the wind speed is stable, reading the numerical value on the micro-manometer to obtain the pressure loss measured by the experiment; and simultaneously recording the size of the wind speed, measuring 26 section wind speeds under each working condition of the experiment, measuring three groups of experimental data aiming at each section wind speed, averaging the experimental data to ensure the correctness of the measurement result, and then substituting the average value into the formula (1) to calculate the theoretical pressure loss.
By analyzing the specific embodiments, the following summary is made: the actual measured pressure loss of each working condition is smaller than the calculated pressure loss, when the wind speed of the first working condition and the second working condition is reduced to one sixth of the actually measured wind speed, when the actual wind speed of the third working condition is reduced to one fifth of the actually measured wind speed, and when the actual wind speed of the third working condition is reduced to one third of the actually measured wind speed, the measured data is most consistent with the calculated data, and the result is shown in fig. 8 to 11, the calculated pressure loss value is divided by the actually measured pressure loss value, and the actually measured pressure loss is increased along with the increase of the wind speed of the working condition; the ratio of the measured pressure loss to the calculated pressure loss of the goaf is reduced firstly along with the increase of the section wind speed, and is slowly stabilized to be a stable value, the stable values under four working conditions are taken as the arithmetic mean value, which is called as a correction coefficient K, and the correction coefficient K is used for correcting the derived formula, so that the calculation result is closer to the real value. The results are shown in fig. 12 to 15.

Claims (3)

1. A method for calculating nitrogen flow dynamic pressure loss in a simulated three-dimensional coal mine goaf is characterized by comprising the following steps:
(1) establishing a goaf gas flow model, and dividing a single-period flow unit;
(2) taking the single-period flow unit as a research object, and dividing the single-period flow unit into four flow stages according to different expressions of the section area changing along with the flow distance;
(3) deducing a theoretical calculation formula of nitrogen flow pressure loss in the goaf;
according to a hydrodynamic Navier-Stocks equation, a one-dimensional flow pressure loss calculation formula is derived as shown in a formula (1):
Figure FDA0003553427790000011
in the formula, JT1Is the one-dimensional flow pressure loss of gas flowing through a gob with unit length, Pa/m; μ is the dynamic viscosity of the gas, pas; rho is gas density, kg/m3(ii) a d is the diameter of the pellet, m; u. of0Is the initial average velocity of the gas, m/s;
(4) on the basis of a theoretical calculation formula, carrying out experimental optimization, reducing the difference between one-dimensional simplification and three-dimensional flow, and obtaining a calculation formula of the pseudo-three-dimensional flow pressure loss as shown in a formula (2):
Figure FDA0003553427790000012
in the formula, JT3The pressure loss is the simulated three-dimensional flow pressure loss of gas flowing through a gob with unit length, and is Pa/m; k is a correction proportion coefficient, and is 0.52 without a dimensional number; alpha is a velocity distribution coefficient and is a dimensionless number;
the step (1) comprises the following steps:
(a) establishing a goaf gas flow model;
the gas flow model was built up from 8 large spheres of diameter d, one with diameter
Figure FDA0003553427790000013
The loose core sphere and 6 diameters are
Figure FDA0003553427790000014
The core-pulling hemisphere; the eight cubic vertexes with the side length of 2d are respectively provided with 8 large balls with the diameter d, and each large ball with the diameter d is tangent to the adjacent large ball with the diameter d; diameter of
Figure FDA0003553427790000021
The core-pulling ball body is positioned at the center of 8 large balls with the diameter d and is tangent with the 8 large balls with the diameter d respectively; 6 have a diameter of
Figure FDA0003553427790000022
The loose core hemispheres are respectively positioned at the central positions of six faces of the cube, and the diameters of the loose core hemispheres are
Figure FDA0003553427790000023
The core-pulling hemisphere is tangent to the surrounding spherical surface;
(b) dividing the single-cycle flow units;
by the symmetry of the flow model, the goaf gas flow model can be divided into single-period flow units, specifically: cutting the flow model into eight single-period flow units by taking the middle point of each edge of a cube with the side length of 2d as a cutting point;
the step (2) comprises the following steps:
taking a single-period flow unit as a research object, wherein the flow direction is the positive direction of a z axis, and the flow starting point is the origin of the z axis; in the first flow stage, starting from the point where z is 0, the flow cross-sectional area expression is as shown in formula (3):
Figure FDA0003553427790000024
wherein A is0Is the cross-sectional area of flow, m2(ii) a d is the diameter of the pellet, m; l is a connecting line from the center of the cutting cylinder to the circumference of the bottom surface, and m is the length of the connecting line; theta is an included angle and radian between the dotted line L and the central axis of the cutting cylinder;
the flow cross-sectional areas of the four flow stages are respectively as follows:
when it is satisfied with
Figure FDA0003553427790000025
The method comprises the following steps:
Figure FDA0003553427790000026
when it is satisfied with
Figure FDA0003553427790000027
The method comprises the following steps:
Figure FDA0003553427790000028
when it is satisfied with
Figure FDA0003553427790000029
The method comprises the following steps:
Figure FDA00035534277900000210
when it is satisfied with
Figure FDA00035534277900000211
The method comprises the following steps:
Figure FDA0003553427790000031
2. the method for calculating the nitrogen flow dynamic pressure loss of the quasi-three-dimensional coal mine goaf according to claim 1, characterized by comprising the following steps: the step (3) comprises the following steps:
(a) the pressure loss per unit length for each flow stage is calculated as follows:
a first flow stage:
Figure FDA0003553427790000032
a second flow stage:
Figure FDA0003553427790000033
a third flow phase:
Figure FDA0003553427790000034
a fourth flow phase:
Figure FDA0003553427790000035
wherein μ is the kinetic viscosity of the gas, pas; rho is gas density, kg/m3(ii) a d is the diameter of the pellet, m; u. of0Is the initial average velocity of the gas, m/s;
(b) determining a theoretical calculation formula of the loss of the nitrogen flow pressure of the goaf as follows:
integrating the formulas of the four flowing stages according to the length proportion of the model to obtain a pressure loss calculation formula of the last flowing period of the minimum flowing unit:
Figure FDA0003553427790000036
3. the method for calculating the nitrogen flow dynamic pressure loss of the quasi-three-dimensional coal mine goaf according to claim 1, characterized by comprising the following steps: the step (4) comprises the following steps:
(a) based on a test bed, setting four different wind paths so as to obtain four different flow section areas, and setting the four conditions as four different working conditions;
(b) measuring actual measurement pressure loss under different wind speeds of each working condition and theoretical pressure loss calculated according to the formula (1);
(c) comparing the measured pressure loss with the theoretical pressure loss, and solving the difference between the one-dimensional simplification and the three-dimensional flow by using a speed distribution coefficient alpha;
(d) and dividing the theoretical pressure loss and the actual pressure loss to obtain a correction proportion coefficient K.
CN202011146211.8A 2020-10-23 2020-10-23 Method for calculating nitrogen flow dynamic pressure loss of three-dimensional simulated coal mine goaf Active CN112214943B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN202011146211.8A CN112214943B (en) 2020-10-23 2020-10-23 Method for calculating nitrogen flow dynamic pressure loss of three-dimensional simulated coal mine goaf

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN202011146211.8A CN112214943B (en) 2020-10-23 2020-10-23 Method for calculating nitrogen flow dynamic pressure loss of three-dimensional simulated coal mine goaf

Publications (2)

Publication Number Publication Date
CN112214943A CN112214943A (en) 2021-01-12
CN112214943B true CN112214943B (en) 2022-04-22

Family

ID=74055011

Family Applications (1)

Application Number Title Priority Date Filing Date
CN202011146211.8A Active CN112214943B (en) 2020-10-23 2020-10-23 Method for calculating nitrogen flow dynamic pressure loss of three-dimensional simulated coal mine goaf

Country Status (1)

Country Link
CN (1) CN112214943B (en)

Family Cites Families (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US20160084083A1 (en) * 2014-09-23 2016-03-24 Gilbert Alan Hice Borehole Mining System and Methods Using Sonic-Pulsed Jetting Excavation and Eductor Slurry Recovery Apparatus
CA3099452A1 (en) * 2018-05-17 2019-11-21 Hydrostor Inc. A hydrostatically compressed gas energy storage system
CN108733923B (en) * 2018-05-21 2020-04-14 湖南科技大学 Goaf nitrogen filling pressure loss calculation method based on minimum flow unit

Also Published As

Publication number Publication date
CN112214943A (en) 2021-01-12

Similar Documents

Publication Publication Date Title
CN108038275A (en) A kind of numerical simulation of gas pipeline leakage sound field and characteristic analysis method
CN107816638A (en) A kind of experimental provision and method suitable for buried gas pipe leakage measurement
CN106000007B (en) A kind of simulation system and analogy method in wet desulphurization flow field
CN104318845B (en) A kind of apparatus and method simulating profundal zone oil spilling under water
CN102608290B (en) Large-scale piping testing apparatus capable of simulating overburden pressure of soil and testing method using large-scale piping testing apparatus
CN107167383A (en) Circulating HTHP gas-liquid two-phase erosive wear experimental provision and method
CN111611723B (en) Urban building group conveying pipeline leakage diffusion data generation method, device and medium
Bu et al. Leakage diffusion characteristics and harmful boundary analysis of buried natural gas pipeline under multiple working conditions
KR102307223B1 (en) Method of Calculating Nitrogen Gas Filling Pressure Loss in Mined Cavity Zones Based on Minimum Flow Units
Wang et al. Study and application of a new gas pressure inversion model in coal seam while drilling based on directional drilling technology
CN112214943B (en) Method for calculating nitrogen flow dynamic pressure loss of three-dimensional simulated coal mine goaf
CN111968479A (en) Tunnel fire simulation experiment device under multi-angle canyon wind effect
Tao et al. A new ventilation system for extra-long railway tunnel construction by using the air cabin relay: A case study on optimization of air cabin parameters length
CN109026154A (en) A kind of determination method and device of wind cave air leak rate of air curtain
DK2430626T3 (en) USING OPERATING GASES TO SIMULATE REAL FIRE SOURCES
CN109442226A (en) Simulate the device of liquid hydrocarbon pipe leakage and the method using device measuring and calculating leakage rate
CN211980003U (en) Coal mine gas extraction pipeline leakage simulation system
CN104376145A (en) Method for evaluating burning quality of turbulent burner based on CFD technology
CN207702136U (en) A kind of experimental provision suitable for buried gas pipe leakage measurement
CN108169419A (en) It is a kind of to test device and the experimental method that water seal cave depot reinjected water influences cave depot
CN113700472B (en) Method for determining air leakage direction and measuring air leakage amount of goaf
CN114239193B (en) Gas pipeline leakage simulation method and device
CN204204304U (en) A kind of device of simulating profundal zone oil spilling under water
CN114722742B (en) Method for measuring gas dispersion coefficient of porous medium in goaf
CN112147049A (en) Method for determining water film thickness of rock core

Legal Events

Date Code Title Description
PB01 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
SE01 Entry into force of request for substantive examination
GR01 Patent grant
GR01 Patent grant