Evaluation method for rapid burning of explosive
Technical Field
The invention belongs to the technical field of explosive safety evaluation, and particularly relates to an evaluation method for rapid roasting and burning of an explosive.
Background
The modern war has higher and higher requirements on the thermal safety of weapons and ammunitions, and the firearms and ammunitions must be absolutely safe in the processes of manufacturing, storing, transporting and using, cannot cause serious accidents such as ignition and explosion and cannot reduce the safety of the firearms and ammunitions in the service life cycle. Therefore, the research on the safety of the ammunition under thermal stimulation has very important significance.
The fire test is an important means for testing and evaluating the thermal safety of ammunition and is divided into fast fire and slow fire according to different heating environments. The rapid fire-burning mainly simulates the thermal response characteristic of ammunition in a fire environment, and tests and numerical simulation are important methods for researching the rapid fire-burning of ammunition. Because the burning test needs a large test field, the test result is greatly influenced by the environmental conditions, and the test device is mainly used for the test research of prototype bullets.
With the development of a numerical simulation technology, numerical simulation gradually becomes an important research method for rapid burning, more researches are carried out in China, wherein the dynamite burning test and the numerical simulation are carried out based on a mass _ flux method [ J ] weapon equipment engineering newspaper, 2020,41(8):1-6 ] based on RBOE explosives, and a calculation model comprising a projectile body, an air domain, a fuel inlet and a fuel outlet is established on the basis of a physical diagram of a burning test device, as shown in figure 1. And loading the programmed linear temperature-time historical curve and mass flow rate to a fuel inlet by adopting a mass flow inlet boundary condition, reacting in a charging area according to an autothermal reaction rule, and applying a reaction kinetic equation to the charging area through a subprogram. The projectile was then heated by high temperature gas radiation and thermal convection, the temperature history of the test and simulated flame environments is shown in fig. 2, and the mass flow rate was adjusted so that the calculated ignition time was substantially consistent with the test ignition time.
The existing method for calculating the fast burning value has the defects that:
(1) the mass flow rate and the linear temperature-time history are loaded to a fuel inlet, and the calculation is less consistent with the temperature history curve of the test environment in a temperature rise section, so that the flame temperature growth process cannot be well described.
(2) The air domain needs to be established in the fast-baking numerical calculation, and in order to simulate the flame combustion environment, the size of the air domain needs to be far larger than that of the projectile body, so that the calculation amount is multiplied, and the calculation efficiency is reduced.
(3) The existing numerical calculation of the quick air-containing domain combustion-baking value is not directly loaded with the temperature on the surface of an elastomer, but is heated through the radiation and convection action of high-temperature fuel gas, the calculation result is greatly influenced by factors such as grid size and air domain size, and the calculation precision is poor.
Disclosure of Invention
In view of this, the invention provides an evaluation method for explosive fast-burning, which can optimize the existing air-containing domain fast-burning calculation and realize the evaluation of explosive fast-burning without an air domain.
The invention is realized by the following technical scheme:
an evaluation method for fast burning of explosives comprises the following specific steps:
step one, building a rapid burning test system and carrying out a rapid burning test;
establishing a rapid combustion-supporting calculation model containing an air domain according to the rapid combustion-supporting test system for simulation; the fast-burning calculation model of the air-containing domain comprises the following steps: the test bomb comprises a test bomb model, an air domain, a fuel inlet and a fuel outlet;
calculating the charge models in the test bomb models in the fast combustion calculation model containing the air domain in different sizes, namely, calculating to obtain the ignition time A of the charge models under different charge model diameters by changing the diameters of the charge models;
establishing a rapid combustion-baking calculation model without an air domain, wherein the rapid combustion-baking calculation model without the air domain only comprises a test bomb model; the outer wall surface of the cartridge case model of the test cartridge model adopts a heat flux boundary as a heating boundary; according to the calculation model of the rapid combustion without the air domain, under the condition that the diameter of the calculation model of the charge is the same as that of the charge model in the third step, calculating the ignition time B of the charge model, and adjusting the size of a heat flux boundary to enable the ignition time A in the third step to be equal to the ignition time B; finally, obtaining the corresponding relation of the heat flux boundary and the corresponding diameter of the charging model, and fitting the scattering point into a curve;
and fifthly, loading the heat flux boundary to the outer wall surface of the test bomb model for calculation according to any diameter of the explosive charging model and the heat flux boundary obtained by calculation according to the curve obtained in the fourth step, obtaining the internal temperature change, the ignition time and the ignition temperature of the explosive charging model, and evaluating the fast burning characteristics of the explosive.
Further, in step one, the testing system comprises: the device comprises a fuel oil pool, a test bomb, a thermocouple, a bracket, a suspension rod, an ignition device and a temperature recorder; the test bomb comprises: the cartridge case and the explosive filled in the cartridge case; the test bomb is fixed on the support through the suspension rod, the fuel pool is positioned under the test bomb, the distance between the lowest part of the test bomb and the upper surface of fuel oil in the fuel pool is 300mm, and the fuel oil in the fuel pool is connected with the ignition device; the thermocouple is arranged outside the test bomb, the thermocouple is positioned on an axis extension line of the test bomb, the closest distance between the thermocouple and the outer end face of the test bomb is 50mm, and the temperature recorder is electrically connected with the thermocouple;
when a rapid burning test is carried out, the ignition device ignites the fuel oil, the fuel oil in the fuel oil pool is combusted to generate flame and high-temperature fuel gas, a flame field is formed around the test bomb, the charge of the test bomb is heated in the flame field, and when the temperature of the flame field is higher than the burning point of the charge of the test bomb, the charge is ignited when the highest temperature of the charge of the test bomb is higher than the burning point; the thermocouple measures the ambient temperature of the flame field where the test bomb is located when fuel oil in the fuel oil pool is combusted, and the temperature recorder records the change of the ambient temperature measured by the thermocouple along with time to obtain the change curve of the ambient temperature along with time.
Further, in step two, the test bomb model is identical to the test bomb, and includes: the shell model and a charging model filled in the shell model; the fuel inlet is high-temperature fuel gas generated by fuel oil combustion of the fuel oil pool, the boundary condition of the fuel inlet is a mass flow inlet boundary, and the mass flow inlet boundary adopts a temperature piecewise function and mass flow rate to fit the test environment temperature; the distance between the lowest part of the test bomb model and the fuel inlet is the same as the distance between the lowest part of the test bomb and the upper surface of the fuel oil pool; the boundary condition of the fuel outlet is a pressure outlet boundary; and simulating the condition of a flame field generated by fuel oil combustion of the fuel oil pool by adjusting the fuel gas mass flow rate and the temperature piecewise function, calculating to obtain a change curve of the environmental temperature of the flame field where the test bomb model is located along with time, and if the difference value of the change curve of the environmental temperature of the flame field where the test bomb model is located along with time and the change curve of the environmental temperature obtained by the test along with time at the same time point is in a set range, indicating that the established calculation model can describe the flame field of the rapid roasting test system.
Further, in the fourth step, a single-phase exponential decay function in Origin software is adopted to fit the corresponding dispersion relation between the heat flux boundary and the diameter of the corresponding charge model.
Further, in the fourth step, Matlab software is adopted to fit the dispersion point correspondence between the heat flux boundary and the diameter of the corresponding charge model.
Further, the scatter point correspondence between the heat flux boundary and the diameter of the corresponding charge model is fit to the following expression after the curve:
where Φ is the heat flux boundary and D is the diameter of the charge model.
Further, in the fourth step, the scatter point correspondence between the heat flux boundary and the diameter of the corresponding charge model is fit to the following expression after the curve:
where Φ is the heat flux boundary and D is the diameter of the charge model.
Further, before the third step, grid division needs to be performed on the rapid combustion-baking calculation model containing the air domain established in the second step, the grid size of the divided air domain is 100mm, and the grid size of the divided test bomb model is 2 mm.
Has the advantages that: the method for evaluating the rapid burning of the explosive provided by the invention optimizes the existing rapid burning calculation method on one hand and provides a new rapid burning calculation method on the other hand.
(1) For the existing fast burning calculation method of the air-containing domain, the temperature piecewise function and the mass flow rate are adopted for fitting the test environment temperature at the mass flow inlet boundary, namely, the temperature piecewise function is adopted for fitting the test environment temperature and the temperature piecewise function is combined with the gas mass flow rate to obtain the inlet boundary condition of the fast burning calculation model of the air-containing domain, so that the problem that the environment temperature calculated by the existing calculation method is poor in coincidence with the test environment temperature is solved.
(2) According to the method, a rapid burning calculation model only considering the test bomb is established, a heat flux boundary is used as a boundary condition for rapid burning numerical calculation, namely the heat flux boundary is used as a heating boundary, so that the calculation model is simplified, and the efficiency of rapid burning numerical simulation calculation is improved; the problems that an existing rapid combustion-baking calculation model containing an air domain is large in calculation amount, complex in influence factors and the like are solved.
(3) The method adopts the single-phase exponential decay function in Origin software to fit the relation between the heat flux boundary and the diameter of the charge model to obtain the relation between the heat flux boundary and the diameter of the charge model, so that the test and calculation quantity can be reduced, the proper heating boundary can be selected according to the size of the charge model to carry out fast burning calculation, and the numerical calculation efficiency of fast burning is greatly improved.
(4) The invention carries out grid convergence analysis, the air domain adopts a large-size grid, the test bomb model adopts a small-size grid, the grids with different sizes are calculated, and the calculation convergence is ensured, thereby improving the calculation efficiency on the premise of ensuring the calculation precision.
Drawings
FIG. 1 is a diagram of a computational model of an air-containing domain in the background art;
FIG. 2 is a graph of environmental temperature for testing and simulation in the background art;
FIG. 3 is a block diagram of a rapid ignition test system according to the present invention;
FIG. 4 is a graph of the environmental temperature of the test and simulation of the present invention over time;
FIG. 5 is a computational model of a fast-burn air-containing domain of the present invention;
fig. 6 is a graph of mesh convergence analysis, (a) is a graph of temperature versus time for different under-mesh charge models for the air domain (b) is a graph of temperature versus time for different under-mesh charge models for the test bomb model;
FIG. 7 is a computational model of a fast-fire without air domains according to the present invention;
FIG. 8 is a graph of the relationship between the heat flux boundary of the present invention and the diameter of the corresponding charge pattern;
the method comprises the following steps of 1-fuel inlet, 2-test bomb model, 3-fuel outlet, 4-air domain, 5-cartridge case model, 6-charging model, 7-outer wall surface, 8-fuel pool, 9-thermocouple, 10-bracket, 11-suspension rod, 12-ignition device, 13-temperature recorder, 14-test bomb, 15-cartridge case and 16-charging.
Detailed Description
The invention is described in detail below by way of example with reference to the accompanying drawings.
The embodiment provides an evaluation method for rapid burning of an explosive, which comprises the following specific steps:
step 1, building a rapid burning test system and developing a rapid burning test, as shown in fig. 3, the test system comprises: the device comprises a fuel oil pool 8, a test bomb 14, a thermocouple 9, a bracket 10, a suspension rod 11, an ignition device 12 and a temperature recorder 13; the test bomb 14 includes: the bullet comprises a bullet shell 15 and a charge 16 filled in the bullet shell 15, wherein the length-diameter ratio of the charge 16 is 2, and the wall thickness of the bullet shell 15 is 6 mm; the test bomb 14 is fixed on the support 10 through the suspension rod 11, the fuel pool 8 is located right below the test bomb 14, the distance between the lowest position of the test bomb 14 and the upper surface of fuel of the fuel pool 8 is 300mm, and the fuel in the fuel pool 8 is connected with the ignition device 12; the thermocouple 9 is positioned and installed outside the test bomb 14 through a mounting rack and rock wool, the thermocouple 9 is located on an axis extension line of the test bomb 14, the closest distance between the thermocouple 9 and the outer end face of the test bomb 14 is 50mm, and the temperature recorder 13 is electrically connected with the thermocouple 9;
when a rapid burning test is carried out, the ignition device 12 ignites the fuel oil, the fuel oil in the fuel oil pool 8 is burnt to generate flame and high-temperature fuel gas, a flame field is formed around the test bomb 14, the temperature of the charge 16 of the test bomb 14 is increased in the flame field, and when the highest temperature of the charge 16 of the test bomb 14 is higher than the burning point of the charge 16, the charge 16 is ignited; the thermocouple 9 measures the ambient temperature of the flame field where the test bomb 14 is located when the fuel oil in the fuel oil pool 8 is combusted, and the temperature recorder 13 records the change of the ambient temperature measured by the thermocouple 9 along with time to obtain the change curve of the tested ambient temperature along with time, as shown by the solid line in fig. 4;
step 2, establishing a rapid combustion-baking calculation model containing an air domain according to the rapid combustion-baking test system for simulation, as shown in fig. 5, wherein the rapid combustion-baking calculation model containing the air domain comprises: the test bomb model 2, the air domain 4, the fuel inlet 1 and the fuel outlet 3; the test bomb model 2 is identical to the test bomb 14 and comprises the following components: a shell model 5 and a charging model 6 filled in the shell model 5; the fuel inlet 1 is high-temperature fuel gas generated by fuel oil combustion of the fuel oil pool 8, the boundary condition of the fuel inlet 1 is a mass flow inlet boundary, the fuel gas mass flow rate of the fuel inlet 1 is specified, the boundary temperature is calculated by adopting a piecewise function, namely the temperature piecewise function to fit the test environment temperature, and finally the temperature piecewise function and the mass flow rate are adopted to fit the test environment temperature on the mass flow inlet boundary; the distance between the lowest part of the test bomb model 2 and the fuel inlet 1 is the same as the distance between the lowest part of the test bomb 14 and the upper surface of the fuel oil pool 8, and the distances are 300 mm; the boundary condition of the fuel outlet 3 is a pressure outlet boundary; simulating the condition of a flame field generated by fuel oil combustion of the fuel oil pool 8 by adjusting the fuel gas mass flow rate and the temperature piecewise function, and calculating to obtain a change curve of the environmental temperature of the flame field where the test bomb model 2 is located along with time, as shown by a dotted line in fig. 4, if the dotted line is basically consistent with the change curve of the environmental temperature along with time (namely a solid line in fig. 4) (namely the difference value of the environmental temperatures of the dotted line and the solid line at the same time point is in a set range), it indicates that the established calculation model can describe the flame field of the rapid combustion test system;
step 3, carrying out grid division on the rapid combustion-baking calculation model containing the air domain established in the step 2, and carrying out grid convergence analysis; because the mesh size of the fast combustion-baking calculation model containing the air domain has a large influence on the calculation result, the mesh convergence calculation needs to be performed on different areas, the calculation of the mesh sizes of 150mm, 100mm and 70mm is performed on the air domain 4, and the ignition time of the charge model 6 is gradually delayed and has a convergence trend along with the reduction of the mesh size, as shown in fig. 6 (a); the calculation of the grid size of the test bomb model 2 to be 2.5mm, 2mm and 1.5mm is respectively carried out, the ignition time of the explosive charging model 6 is gradually delayed along with the reduction of the grid size, and the explosive charging model has a convergence trend, as shown in fig. 6 (b); in order to balance the calculation efficiency and the calculation precision, the size of the grid for dividing the air domain 4 is 100mm, and the size of the grid for dividing the test bomb model 2 is 2 mm;
step 4, calculating different sizes of the charge models 6 in the test bomb model 2 according to the quick combustion-baking calculation model of the air-containing domain after the grid division is finished, namely, obtaining ignition time A of the charge models 6 under different diameters D of the charge models 6 by changing the diameter D of the charge models 6;
step 5, establishing a rapid combustion-baking calculation model without an air domain, as shown in fig. 7, wherein the rapid combustion-baking calculation model without the air domain only comprises a test bomb model 2; the outer wall surface 7 of the cartridge case model 5 of the test cartridge model 2 adopts a heat flux boundary as a heating boundary; according to the fast burning calculation model without the air domain, under the condition that the diameter of the charge model 6 in the step 4 is the same, calculating the ignition time B of the charge model 6, and adjusting the size of a heat flux boundary to enable the ignition time A in the step 4 to be equal to the ignition time B; finally, the relationship between the heat flux boundary and the diameter D of the corresponding charge model 6 is obtained, as shown in the scatter diagram in fig. 8;
step 6, fitting the scatter diagram in the graph 8 by adopting a single-phase exponential decay function or Matlab software in Origin software to obtain a relational expression between the heat flux boundary phi and the diameter D of the charging model 6, wherein the relational expression is as follows:
and 7, loading the heat flux boundary phi to the outer wall surface 7 of the test bomb model 2 for calculation according to any diameter D of the explosive charging model 6 and the corresponding heat flux boundary phi obtained by calculation in the formula (1), acquiring information such as internal temperature change, ignition time and ignition temperature of the explosive charging model 6, and evaluating the rapid ignition characteristic of the explosive.
In summary, the above description is only a preferred embodiment of the present invention, and is not intended to limit the scope of the present invention. Any modification, equivalent replacement, or improvement made within the spirit and principle of the present invention should be included in the protection scope of the present invention.