CN1186605C - Pressure measuring method for energetic material DDT pipe experiment - Google Patents

Pressure measuring method for energetic material DDT pipe experiment Download PDF

Info

Publication number
CN1186605C
CN1186605C CNB031183891A CN03118389A CN1186605C CN 1186605 C CN1186605 C CN 1186605C CN B031183891 A CNB031183891 A CN B031183891A CN 03118389 A CN03118389 A CN 03118389A CN 1186605 C CN1186605 C CN 1186605C
Authority
CN
China
Prior art keywords
ddt
energetic material
pipe
experiment
signal
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.)
Expired - Fee Related
Application number
CNB031183891A
Other languages
Chinese (zh)
Other versions
CN1450344A (en
Inventor
浣石
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
Original Assignee
Hunan University
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 filed Critical Hunan University
Priority to CNB031183891A priority Critical patent/CN1186605C/en
Publication of CN1450344A publication Critical patent/CN1450344A/en
Application granted granted Critical
Publication of CN1186605C publication Critical patent/CN1186605C/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Images

Abstract

The present invention relates to a pressure measuring method for an energetic material DDT pipe experiment. In the pressure measuring method for an energetic material DDT pipe experiment, an inertia block having similar shock impedance with a measured energetic material is embedded into an unburned and unexploded area of a DDT pipe, and one or a plurality of compound Lagrangian sensors are embedded into the inertia block. Each compound Lagrangian sensor is composed of a manganin pressure-resistance meter and a constantan stretching meter. The pressure measuring method for an energetic material DDT pipe experiment can obtain one or a plurality of pressure waveforms, and therefore, the pressure measuring method for an energetic material DDT pipe experiment provides new experimental data for researching and controlling the DDT phenomenon of the energetic material. The present invention has the advantages of real measuring condition, complete measuring process, precise, comprehensive and reliable measuring data, etc.

Description

The pressure measurement method of energetic material DDT pipe experiment
Technical field: the present invention is a kind of dynamic pressure waveform measuring method, and the dynamic pressure waveform that particularly relates to the experiment of energetic material DDT pipe is measured.
Background technology: when the security performance of energetic material (mainly being meant explosive and propellant) was measured and estimated, its COMBUSTION TO DETONATION TRANSITION (DDT) performance was an important indicator.Energetic material DDT performance measurement is to carry out in the metal tube of specific dimensions, is referred to as the experiment of DDT pipe.Because the DDT process is very complicated physics, chemistry and a mechanical process, its burning rate centimetre develops into the thousands of rice of per second by the per second number, corresponding pressure increases to a hundreds of thousands atmospheric pressure from several atmospheric pressure, and laminar flow, forced convection shock wave three phases have then been experienced in particle movement.Pressure waveform problems of measurement for DDT pipe experimentation never solves, and its difficulty is:
If sensor is too thick too big, then will change the actual measurement state; If sensor is too thin too little, then writing time too short, can not finish the measurement of overall process, and the complex flow state in the DDT pipe and high temperature, high pressure conditions will make the very fast inefficacy of general pressure transducer.Therefore the experiment of DDT pipe generally all is by reclaiming the DDT pipe, by similar experiment relatively, drawing the dangerous parameter of qualitative with relative DDT.At present to the mechanism research of DDT phenomenon, to the DDT phenomenon controlled and the demand utilized all an urgent demand test the change curve of the pressure waveform that the DDT process can be provided.
Summary of the invention: technical matters to be solved by this invention provides and a kind ofly measures that state is true, measuring process fully, the measurement data pressure measurement method of energetic material DDT pipe experiment accurately and reliably.
The pressure measurement method of energetic material DDT pipe of the present invention experiment, it is characterized in that the inert block identical with the measured energy material impact impedance imbedded in the unburned and unexploded area of DDT pipe, imbed compound Lagrangian sensor in the inert block, every group of compound Lagrangian sensor imbedding in the inert block is made up of a manganese-copper piezoresistance meter and a constantan tension gage, both have identical geometric configuration, and in experiment, be on the position of symmetry, comprise pressure signal and stretch signal Δ R (t) in the tracer signal of manganese-copper piezoresistance meter m, and only contain stretch signal Δ R (t) in the tracer signal of constantan tension gage c, utilize following formula that experimental result is handled and obtain pressure waveform signal,
P(t)=α*ΔR(t) (1)
ΔR ( t ) = ΔR ( t ) m R m 0 - K m K c * ΔR ( t ) c R co - - - ( 2 )
α wherein: be the piezoresistance coefficient of manganese-copper piezoresistance meter 5;
K m, K c: the drawing coefficient that is respectively manganese-copper piezoresistance meter 5 and constantan tension gage 6;
R M0, R Co: the base voltage signal that is respectively manganese-copper piezoresistance meter 5 and constantan tension gage 6.
As further scheme of the present invention, the described compound Lagrangian sensor of imbedding inert block is one or more groups.
Utilize measuring method of the present invention, both reduced the change (because inert block with the impact impedance of the energetic material of unburned and unexploded area identical) of embedded-type sensor, solved not long problem of sensor record time again measuring state.The many groups pressure waveforms that utilize the compound Lagrangian sensor of many groups to record can cause position, blowback intensity of wave and speed thereof etc. and make quantitative analysis the formation of pressure in COMBUSTION TO DETONATION TRANSITION (DDT) process, its rise speed and velocity of propagation, detonation.Be the further mechanism of research DDT phenomenon, and control and utilize it, new experimental data is provided.Have advantages such as the measurement state is true, measuring process is complete, measurement data is accurate, comprehensive, reliable.
Description of drawings:
Fig. 1 is the pressure measurement method experimental provision structural representation of energetic material DDT pipe of the present invention experiment.
Fig. 2 is the A-A profile of Fig. 1.
Fig. 3 is the oscillograph recording signal graph of manganese-copper piezoresistance meter.
Fig. 4 is the oscillograph recording signal graph of constantan tension gage.
Embodiment:
Realize that step of the present invention is as follows: in the experiment of energetic material DDT pipe (as shown in Figure 1, 2), imbed the inert block 3 close with this energetic material impact impedance at the unburned and unexploded area 2 of metal tube 1, the length of inert block 3 is less than 1/3rd of unburned and unexploded area length.In distance inert block 3, imbed one or more groups compound Lagrangian sensor 4.Every group of compound Lagrangian sensor is made up of a manganese-copper piezoresistance meter 5 and a constantan tension gage 6, and both have identical geometric configuration, and is in experiment on the position of symmetry.Comprise pressure signal and stretch signal Δ R (t) in the tracer signal of manganese-copper piezoresistance meter 5 m(as shown in Figure 3).And only contain stretch signal Δ R (t) in the tracer signal of constantan tension gage 6 c(as shown in Figure 4).Utilize following formula that experimental result is handled and to obtain pressure waveform signal.
P(t)=α*ΔR(t) (1)
ΔR ( t ) = ΔR ( t ) m R m 0 - K m K c * ΔR ( t ) c R co - - - ( 2 )
α wherein: be the piezoresistance coefficient of manganese-copper piezoresistance meter 5;
K m, K c: the drawing coefficient that is respectively manganese-copper piezoresistance meter 5 and constantan tension gage 6;
R M0, R Co: the base voltage signal that is respectively manganese-copper piezoresistance meter 5 and constantan tension gage 6.

Claims (2)

1, the pressure measurement method of a kind of energetic material DDT pipe experiment, it is characterized in that the inert block identical with the measured energy material impact impedance imbedded in the unburned and unexploded area of DDT pipe, imbed compound Lagrangian sensor in the inert block, every group of compound Lagrangian sensor imbedding in the inert block is made up of a manganese-copper piezoresistance meter and a constantan tension gage, both have identical geometric configuration, and in experiment, be on the position of symmetry, comprise pressure signal and stretch signal Δ R (t) in the tracer signal of manganese-copper piezoresistance meter m, and only contain stretch signal Δ R (t) in the tracer signal of constantan tension gage c, utilize following formula that experimental result is handled and obtain pressure waveform signal,
P(t)=α*ΔR(t) (1)
ΔR ( t ) = ΔR ( t ) m R m 0 - K m K c * ΔR ( t ) c R c 0 - - - ( 2 )
α wherein: be the piezoresistance coefficient of manganese-copper piezoresistance meter 5;
K m, K c: the drawing coefficient that is respectively manganese-copper piezoresistance meter 5 and constantan tension gage 6;
R M0, R Co: the base voltage signal that is respectively manganese-copper piezoresistance meter 5 and constantan tension gage 6.
2,, it is characterized in that the compound Lagrangian sensor of imbedding inert block is one or more groups by the pressure measurement method of the described energetic material DDT pipe of claim 1 experiment.
CNB031183891A 2003-05-20 2003-05-20 Pressure measuring method for energetic material DDT pipe experiment Expired - Fee Related CN1186605C (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CNB031183891A CN1186605C (en) 2003-05-20 2003-05-20 Pressure measuring method for energetic material DDT pipe experiment

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CNB031183891A CN1186605C (en) 2003-05-20 2003-05-20 Pressure measuring method for energetic material DDT pipe experiment

Publications (2)

Publication Number Publication Date
CN1450344A CN1450344A (en) 2003-10-22
CN1186605C true CN1186605C (en) 2005-01-26

Family

ID=28684367

Family Applications (1)

Application Number Title Priority Date Filing Date
CNB031183891A Expired - Fee Related CN1186605C (en) 2003-05-20 2003-05-20 Pressure measuring method for energetic material DDT pipe experiment

Country Status (1)

Country Link
CN (1) CN1186605C (en)

Also Published As

Publication number Publication date
CN1450344A (en) 2003-10-22

Similar Documents

Publication Publication Date Title
Graham Solids under high-pressure shock compression: mechanics, physics, and chemistry
Turley et al. Spall response of single-crystal copper
Rogers Engine combustion: pressure measurement and analysis
Brusniak et al. Physics of unsteady blunt-fin-induced shock wave/turbulent boundary layer interactions
CN204329720U (en) Perforating gun gun barrel dynamic response testing arrangement under a kind of blast load
CN102353813A (en) Broadband high range accelerometer frequency response characteristic calibrating device and method thereof
CN103439360A (en) Solid propellant multi-thermocouple dynamic combustion performance testing system and method
CN105954320A (en) Device for studying shock initiation performance of explosive and experiment method of device
CN1186605C (en) Pressure measuring method for energetic material DDT pipe experiment
CN103528925A (en) Rotational viscometer with blade-shape motor, and method of measuring particle fluid viscosity by the rotational viscometer
CN106885617A (en) A kind of liquid level gauge detection means and its detection method
CN102841141A (en) Novel material dynamic mechanics performance testing method and device thereof
CN1609577A (en) Method for detecting sleeve fluid-loss point utilizing direct-reading ultrasound flowmete
CN108088591B (en) Fractal type manganese copper film ultrahigh pressure sensor
CN110220775B (en) Measuring device based on sample transmissivity under impact loading of light gas gun
CN109374682B (en) Monitoring device for cracking time of brittle material
Kline Acoustic emission signal characterization
CN112945034A (en) Method for testing delay precision of electronic detonator based on actual measurement waveform of underwater shock wave
CN1804662A (en) Field test method for selection of seismic exploration trace-to-trace distance and maximum shot-to-geophone distance
Nicholas et al. Shear-strain-rate effects in a high-strength aluminum alloy: Paper describes the results of experiments on a high-strength aluminum alloy, which were undertaken to determine whether incremental plastic waves propagate in such an apparently rate-independent material in the manner predicted by the rate-independent theory
Nelson et al. Acoustic emissions produced by discrete fracture in rock Part 1—Source location and orientation effects
RU2775827C1 (en) Method for continuous recording of the position, profile and velocity of a stationary surface of a plate subjected to shock-wave deformation
CN220231433U (en) Friction sensitivity test system for different powder materials of explosives and powders
CN1039113A (en) The lagrangian measurement of two-dimentional axial symmetry flow field
Brusniak et al. Flowfield dynamics in blunt fin-induced shock wave/turbulent boundary layer interactions

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C14 Grant of patent or utility model
GR01 Patent grant
C19 Lapse of patent right due to non-payment of the annual fee
CF01 Termination of patent right due to non-payment of annual fee