CN107607230A - A kind of probe and method for measuring hall thruster wall ion hot-fluid - Google Patents

A kind of probe and method for measuring hall thruster wall ion hot-fluid Download PDF

Info

Publication number
CN107607230A
CN107607230A CN201710860394.1A CN201710860394A CN107607230A CN 107607230 A CN107607230 A CN 107607230A CN 201710860394 A CN201710860394 A CN 201710860394A CN 107607230 A CN107607230 A CN 107607230A
Authority
CN
China
Prior art keywords
probe
thermometric
temperature
hot
fluid
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.)
Granted
Application number
CN201710860394.1A
Other languages
Chinese (zh)
Other versions
CN107607230B (en
Inventor
李鸿
于达仁
丁永杰
魏立秋
刘星宇
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.)
Harbin Institute of Technology
Original Assignee
Harbin Institute of 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 Harbin Institute of Technology filed Critical Harbin Institute of Technology
Priority to CN201710860394.1A priority Critical patent/CN107607230B/en
Publication of CN107607230A publication Critical patent/CN107607230A/en
Application granted granted Critical
Publication of CN107607230B publication Critical patent/CN107607230B/en
Active legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Landscapes

  • Plasma Technology (AREA)

Abstract

A kind of probe and method for measuring hall thruster wall ion hot-fluid, it is related to a kind of temperature measuring device and method, and to solve the problems, such as that existing measurement hall thruster wall ion deposition power is in technical bottleneck, it includes metallic rod, radiating block and temperature thermometric line;Metallic rod connects radiating block, is also equipped with thermometric boss in metallic rod, thermometric boss connects temperature thermometric line respectively on two surfaces relative with radiating block, and metallic rod, thermometric boss and radiating block are non-magnetic rustproof Steel material.The step of this method is:Step 1: bore mounting hole on hall thruster ceramics wall;Step 2: it is respectively arranged several temperature thermometric lines on two relative faces of thermometric boss and radiating block;Step 3: the metallic rod of cladding heat-insulating material is arranged in mounting hole;Step 4: start hall thruster, probe, which reaches, to be measured the temperature of probe axial direction diverse location after hot stable state and can obtain hot-fluid.The present invention is used for the measurement of hall thruster wall ion deposition hot-fluid.

Description

A kind of probe and method for measuring hall thruster wall ion hot-fluid
Technical field
The present invention relates to a kind of temperature measuring device and method, and in particular to a kind of measurement hall thruster wall ion hot-fluid Probe and method.
Background technology
Hall thruster is a kind of using crossed electric and magnetic field ionization and acceleration working medium, so as to convert electrical energy into the dynamic of kinetic energy Power apparatus.It has it is simple in construction, than leaping high, efficiency high, long working life, that power density is high, in-orbit active time is long etc. is excellent Gesture, suitable for the gesture stability of all kinds of spacecrafts, orbital exponent, Orbit Transformation, power compensation, position keep, reposition, from The tasks such as rail processing, survey of deep space, it is at present in the world using at most most ripe electric thruster.
Compared to chemical propulsion, hall thruster have one it is important the advantages of be efficiency high, at present, hall thruster Gross efficiency generally 50% or so, but the efficiency of high voltage and small-power hall thruster is generally relatively low, it is therefore desirable to grinds Study carefully hall thruster internal energy conversion process, establish rational energy loss system, analyze each several part energy loss.It is existing to grind Study carefully display, the main energy loss in the hall thruster course of work has:Wall heat deposition, anode heat deposition, plume diverging damage Lose.Therefore, wall heat deposition mechanism is studied, and how to reduce wall heat deposition to turn into an important problem.
In the hall thruster course of work, its wall is exposed in plasma environment, wall heat deposition comes from etc. from Daughter and the interaction of insulation wall.Research currently for hall thruster wall heat deposition is concentrated mainly on theoretical model Prediction and numerical value dummy run phase, there are two kinds of different sayings for wall heat deposition mechanism on theory analysis:First, think electronics Quality be far smaller than mass of ion, ignore electronic deposition power;Second, think that electronics and wall action can produce substantial amounts of two Secondary electronics, quantitatively it is more than ion with the electronics of wall action, electronic deposition power is more than ion deposition power, therefore is directed to The research of hall thruster wall heat deposition needs a kind of laboratory facilities to enter electronic deposition power and ion deposition power Row is distinguished.
Wall electronic deposition power Pe=Ie,in·Te,in-Ie,out·Te,out, wherein, Ie,inFor wall incident electron fluence, Te,inFor wall incident electron average energy, Ie,outFor wall outgoing electron flux, Te,outFor wall outgoing electron average energy. Measurement wall electronic deposition power needs average energy to incident electron and outgoing electron and flux to diagnose, at present for The technology of hall thruster plasma diagnostics mainly has two kinds of spectroscopic diagnostics and probe diagnostics, and either spectroscopic diagnostics is still visited Pin measurement can not all be made a distinction to the information of incident electron and outgoing electron, therefore wall heat can only be measured by laboratory facilities Ion deposition power in deposition power.After ion and collision with wall with electronics is compound rebounds out as atom, measurement ion Deposition power needs to diagnose the information such as the angle of wall ionic flux, ion energy and ion incidence wall, at present The means of possessed diagnosis ion energy are mainly RPA probes, and RPA probe volumes are bigger, tied by hall thruster Structure limits, it is impossible to which inside the discharge channel of hall thruster, Langmuir probe small volume can be used in discharge channel Portion, but can only obtain ionic flux, it is impossible to diagnose ion energy.Therefore, discharge plasma environment and existing diagnosis hand The shortcomings that section, forms technical bottleneck to direct measurement wall ion deposition power.
The content of the invention
The present invention is to solve the problems, such as that existing measurement hall thruster wall ion deposition power is in technical bottleneck, carrying A kind of probe and method for measuring hall thruster wall ion hot-fluid is supplied.
The present invention adopts the technical scheme that to solve the above problems:
A kind of probe for measuring hall thruster wall ion hot-fluid includes metallic rod, radiating block and temperature thermometric line;Gold Belong to bar connection radiating block, thermometric boss is also equipped with metallic rod, is distinguished on thermometric boss two surfaces relative with radiating block Temperature thermometric line is connected, metallic rod, thermometric boss and radiating block are non-magnetic rustproof Steel material.
Further, metallic rod, thermometric boss and radiating block are same by being made into integration without magnetic 1Cr18Ni9Ti stainless steels Heart cylinder.
Further, temperature thermometric line is electric thermo-couple temperature thermometric line.
Further, heat-insulating material is adiabatic coating.
Originally return and a kind of method for measuring hall thruster wall ion hot-fluid is provided, be the step of this method:
Step 1: bore mounting hole on hall thruster ceramics wall;
Step 2: it is respectively arranged several temperature thermometric lines, temperature on two relative faces of thermometric boss and radiating block The end of probe of thermometric line is connected on thermometric boss and radiating block, and the output end of temperature thermometric line leads to acquisition system;
Step 3: the end of metallic rod to the metallic rod between thermometric boss and thermometric boss is coated with heat-insulating material, The metallic rod for coating heat-insulating material is arranged in mounting hole, metallic rod front end and heat-insulating material is flushed with ceramic wall face bottom;
Step 4: starting hall thruster, after hall thruster wall surface temperature reaches stable, provided necessarily to probe Negative potential, electronics is masked completely, while the ion that probe receives reaches saturation;
Probe, which reaches, to be measured the temperature of probe axial direction diverse location after hot stable state and can obtain hot-fluid, is expressed as:
Q-probe measurement hot-fluid, unit:Watt;
The thermal conductivity factor of λ-probe;Probe material 1Cr18Ni9Ti thermal conductivity factor is 21W/ (mK);
The temperature of T-probe, unit:K;
A-probe front face area, unit:m2;A=π D2/4;D is metal shank diameter, unit:m;
Z-probe axial distance, unit:m;
Wherein, axial displacement of the temperature thermometric line end of probe apart from radiating block bottom surface is z in thermometric boss surface1, measurement Temperature averages are T1
Temperature thermometric line end of probe distance probes radiating block at the end of the axial displacement on heat dissipation block surface is z2, measurement temperature Average value is T2
Present invention beneficial effect compared with prior art is:The probe of the present invention can be used for macroscopical heat-flow measurement, can will suddenly That thruster course of work plasma and the complicated microphysics process of wall action are showed by macroscopical hot-fluid, and And available for the ion deposition heat-flow measurement in wall heat deposition, so as to which electronic deposition, ion deposition in wall heat deposition be entered Row is distinguished, and a kind of laboratory facilities are provided to research hall thruster internal plasma and the mechanism of wall action.
Brief description of the drawings
Fig. 1 is the probe structure schematic diagram of the present invention;
Fig. 2 is probe temperature measurement location schematic diagram of the present invention;
Fig. 3 is probe and hall thruster assembling schematic diagram;
Fig. 4 is thermal probe biasing circuit figure;
Fig. 5 is emulation detection schematic diagram in the embodiment of the present invention.
Embodiment
Technical solution of the present invention is further described with reference to the accompanying drawings and examples.
As shown in figure 1, a kind of probe for measuring hall thruster wall ion hot-fluid includes metallic rod 1, radiating block 3 and temperature Spend thermometric line 6;Metallic rod 1 connects radiating block 3, and thermometric boss 2, thermometric boss 2 and the phase of radiating block 3 are also equipped with metallic rod 1 To two surfaces on connect temperature thermometric line 6 respectively, metallic rod 1, thermometric boss 2 and radiating block 3 are non-magnetic rustproof steel Material.
Present embodiment totally calculates the technological means of hot-fluid using metal electrode shielding electronics, thermocouple temperature measurement, realizes Hall thruster wall heat deposition intermediate ion deposition power and the purpose of electronic deposition power are distinguished, probe structure is completed and sets Meter, the thermal probe of installation instead of the sub-fraction of original ceramic wall, plasma and probe in the thruster course of work Front end face directly acts on generation heat deposition, and the hot-fluid of deposition can be conducted to other structures, by being connect in probe and thruster Tactile surface spraying heat-insulating material cut-off heat conduction, the hot-fluid that probe receives can only axially conduct along probe, and probe reaches After hot stable state, internal thermal process is regarded as one-dimensional stable heat transfer, and the hot-fluid that probe front face receives is equal to metallic rod rear portion Divide conduction hot-fluid, therefore measure the temperature of probe rear end axially distinct position (outside thruster), utilize Fourier Heat Conduction law It can obtain plasma-deposited hot-fluid.
Illustrate referring to Fig. 1, for the ease of processing probe, and reduce thermal loss, improve the precision of measurement, the spy of design Metallic rod 1, thermometric boss 2 and radiating block 3 are the concentric cylinder by being made into integration without magnetic 1Cr18Ni9Ti stainless steels in pin.Survey Warm boss 2 along metallic rod 1 circumferentially.So ensure the temperature stabilization that the temperature thermometric line 6 arranged on thermometric boss 2 is surveyed Reliably.
The size of probe is mainly determined by the physical dimension and power grade of hall thruster, first can be divided using ANSYS heat Analyse module and calculate temperature, the temperature of 1 front end face of metallic rod 4 is worked with hall thruster to wall surface temperature during hot stable state and be close to Preferably.Present embodiment is for HEP100HV hall thrusters (outlet outer ceramic wall thickness 9mm, discharge power 3000w), as one Individual embodiment, metallic rod 1, thermometric boss 2 and radiating block 3 are concentric cylinder, 1 a diameter of 1mm of metallic rod, and overall length is 40mm, thermometric boss 2 a diameter of 5mm, axial length 1mm, the front end face 5 of thermometric boss 2 and the distance of front end face 4 of metallic rod 1 10mm, ensure that thermometric boss 2 can be placed on outside hall thruster ceramics wall or magnetic cup, on metallic rod front end face 4 to metallic rod 2 1mm is apart from all side sprayed thermal insulants, in order to reduce cost, convenient work, it is preferable that the adiabatic paint of spraying, radiating block 3 it is straight Footpath is 12mm, axial length 10mm.Influence to reduce the heat radiation on each surface, be processed by shot blasting surface during processing, Reduce radiant emissivity.
The present embodiment middle probe is mainly used in the measurement of HEP100HV hall thrusters wall heat flux, due to hall thruster table Face size is smaller, is easily installed, and temperature thermometric line 6 uses thermocouple temperature measurement line.In thermometric boss 2 and the phase of radiating block 3 during measurement To two surfaces on thermocouple temperature measurement line is installed respectively, such as the 7-1 of surface one in Fig. 1 and the 7-2 positions of surface two.Thermocouple temperature measurement Line is arranged as shown in Fig. 2 to avoid uncertainty present in thermocouple individual error and experiment, it is preferable that convex in thermometric Two thermocouple temperature measurement lines are installed, the surface of radiating block 3 is larger, installs four thermocouple temperature measurement lines on platform 2.The principle of measurement is Based on Fourier Heat Conduction law, when probe does not have outside heat transfer, the thermal process in metallic rod 1 can be approximately that one-dimensional stable is led Thermal process, probe, which reaches, to be measured the temperature of probe axial direction diverse location after hot stable state and can obtain hot-fluid, and its heat conduction heat flux can table It is shown as:
Q-probe heat conduction heat flux;
The thermal conductivity factor of λ-probe;Probe material 1Cr18Ni9Ti thermal conductivity factor is 21W/ (mK);
The temperature of T-probe;
A-probe receiving area;
Z-probe axial distance.
With reference to Fig. 1-Fig. 3 illustrate, using probe measurement hall thruster wall ion hot-fluid method the step of be:
Step 1: bore mounting hole on 8 ceramic wall of hall thruster;
Step 2: several temperature thermometric lines are respectively arranged on two relative faces of thermometric boss 2 and radiating block 3, temperature The end of probe of degree thermometric line is connected on thermometric boss 2 and radiating block 3, and the output end of temperature thermometric line leads to acquisition system;
Step 3: by the end of metallic rod 1 to the metallic rod 1 between thermometric boss 2 and the heat-insulating material bag of thermometric boss 2 Cover, the metallic rod 1 for coating heat-insulating material is arranged in mounting hole, makes the front end of metallic rod 1 and heat-insulating material and ceramic wall face bottom Flush;
Step 4: starting hall thruster 8, after the wall surface temperature of hall thruster 8 reaches stable, provided to probe certain Negative potential, electronics is masked completely, at the same probe receive ion reach saturation;
Probe, which reaches, to be measured the temperature of probe axial direction diverse location after hot stable state and can obtain hot-fluid, is expressed as:
Q-probe measurement hot-fluid, unit:Watt;
The thermal conductivity factor of λ-probe;Probe material 1Cr18Ni9Ti thermal conductivity factor is 21W/ (mK);
The temperature of T-probe, unit:K;
A-probe front face area, unit:m2;A=π D2/4;D is metal shank diameter, unit:m;
Z-probe axial distance, unit:m;
Wherein, axial displacement of the end of probe of temperature thermometric line 6 apart from the bottom surface of radiating block 3 is z on the surface of thermometric boss 21, survey Amount temperature average value is T1
The at the end of the axial displacement of 6 end of probe distance probes radiating block of temperature thermometric line 3 on the surface of radiating block 3 is z2, measurement Temperature averages are T2
Simply illustrate the principle of probe measurement hot-fluid herein and the Method And Principle of hot-fluid is obtained by temperature.
Punched during use on thruster ceramics wall (magnetic cup), by the side surface of metallic rod 1 of probe (position 9 in such as Fig. 3 The shown adiabatic paint (thermal conductivity factor is less than 0.2W/ (mK)) of spraying is installed afterwards, as shown in figure 3, making the front end of metallic rod 1 of probe Face, adiabatic lacquer coat are concordant with the inside of ceramic wall 8.
The energy obtained in the electric field directly and wall action, is converted into wall by thruster course of work plasma Heat energy, this part energy, which, is converted into the kinetic energy of propulsion, but transfers heat to shell etc. by heat transfer and tie Structure, and then be dissipated in the form of heat radiation in environment.The thermal probe of installation instead of original pottery in the thruster course of work The sub-fraction of porcelain wall, plasma directly act on generation heat deposition with probe front face, and the hot-fluid of deposition can be tied to other Structure is conducted, and separating heat by the surface spraying heat-insulating material contacted in probe with thruster conducts, the heat that probe receives Stream can only axially conduct along probe, and after probe reaches hot stable state, internal thermal process is regarded as one-dimensional stable heat transfer, probe The hot-fluid that front end face receives is equal to partial conductance hot-fluid after metallic rod, therefore it is axially distinct (outside thruster) to measure probe rear end The temperature of position, plasma-deposited hot-fluid is can obtain using Fourier Heat Conduction law, plasma-deposited hot-fluid can represent For:
qplasma- plasma-deposited hot-fluid, unit:Watt;
qconduct- probe axially conducts hot-fluid, unit:Watt;
The thermal conductivity factor of λ-probe;Probe material 1Cr18Ni9Ti thermal conductivity factor is 21W/ (mK);
The temperature of T-probe, unit:K;
A-probe front face area, unit:m2;A=π D2/4;D is metal shank diameter, unit:m;
Z-probe axial distance, unit:m.
Thruster course of work middle probe receives the hot-fluid of electronics, ion deposition simultaneously, if probe is connected to such as Fig. 4 institutes In the external circuitses shown, certain negative potential is provided to probe, electronics is masked completely, while the ion that probe receives reaches Saturation, the hot-fluid that now probe receives is exactly ion deposition hot-fluid.Because the negative bias potential added by probe can change probe The local ion velocity of reception, therefore the hot-fluid measured is more than wall ion deposition hot-fluid in the thruster course of work, therefore first Using thermal probe as Langmuir Single probe, C-V characteristic is measured, obtains the scope of ion saturation region bias potential, within this range Select several bias potential U1、U2、U3、U4, measure ion hot-fluid respectively under different bias potentials, obtain the potential of thermal probe- Heatflow characteristics relation.
The ion hot-fluid of deposited probes is represented by:
qion=qi·ΔUi·Ii (3)
qion- ion deposition hot-fluid, unit:Watt;
qiElectrically charged, the unit of-ion:Storehouse;
ΔUi- ion is poor when earth potential and probe potential, unit:Volt;
IiThe ionic flux of-sensing wall.
The energy that electric charge obtains in the electric field is multiplied by electrical potential difference equal to the quantity of electric charge, and ion is got on wall and just transmits energy Wall has been given, has formed the hot-fluid of wall, but the position that probe is installed in thruster course of normal operation is ceramic wall, is not have There is applying electrical potential, the effect of probe applying electrical potential is that electron repelling is walked, and the additional effect brought is exactly to change ion Speed, thus measure in the case of probe applying electrical potential the hot-fluid come and the hot-fluid that actual ions deposit be it is unequal, because This is needed to measure hot-fluid under different bias potentials, and actual ion deposition is obtained by potential-heatflow characteristics relation of thermal probe Hot-fluid.
As shown in formula (3), the hot-fluid of ion deposition and ion are linear when earth potential and probe potential difference, by heat The potential of probe-heatflow characteristics relation (straight line seeks slope), counter can push away ion hot-fluid when bias potential is zero, i.e. thruster Ion truly deposits to the hot-fluid of wall formation during normal work.
Thermal probe be typically mounted at hall thruster channel outlet nearby wall, thruster work when thermal probe exposed to etc. In gas ions environment, can plasma electric discharge produce slight interference, therefore the size of metal electrode is small, with reduce equity from The interference of daughter electric discharge, probe adds negative bias potentials when measuring ion hot-fluid, therefore thermal probe is carried out in installation process with pushing away Insulating, be adiabatic between power device structure.
The present embodiment by taking the physical dimension of high voltage hall thruster as an example, introduce apply for a patent probe structure design, Heat probe measurement principle, data processing method, Fig. 1 give probe Each part schematic diagram, and Fig. 2 is thermal probe temperature measurement location Schematic diagram, Fig. 3 are thermal probe and hall thruster assembling schematic diagram, and Fig. 4 is thermal probe biasing circuit figure.The design of probe needs root Factually the thruster structural member size used in test amount and power grade determine, the design of radiating block can be first with ANSYS heat point Analyse module and calculate probe temperature distribution, adjustment size makes probe tip temperature be approached with temperature in use environment, reduces spy with this Heat radiation of the needle tip into environment on caused by measurement accuracy influence, while it is noted that probe use material temperature limiting, Adjusting probe size according to result of calculation makes probe face temperature less than the fusing point of material.
Thermal probe Proof-Of Principle process of the present invention:Model is established, is calculated using the temperature of ANSYS thermal analysis modules calculating Probe measures hot-fluid.Thermal probe material uses 1Cr18Ni9Ti, and thermal conductivity factor is 21W/ (mK), and the thermal conductivity factor of thermal insulation paint is set 0.1W/ (mK) is set to, applies 0.1w thermal forces in probe front face, and considers the environment spoke in probe front face in a model Penetrate, result of calculation is as shown in Figure 5.Two temperature measuring point temperature computation results during thermal probe use be respectively 259.26 DEG C and It is 115.42 DEG C, as follows to calculate hot-fluid by the use of this temperature as probe measurement temperature:
The hot-fluid that is calculated and the hot-fluid error that truly inputs are 1.1%, and therefore, this detecting probe method is reliable.Formula (4) This is exactly the calculating temperature obtained with formula (2) and emulation.
Consider that factor, measurement result and the actual hot-fluids such as thermocouple measurement error have deviation in actual measurement, it is therefore desirable to Experimental result is verified, in ANSYS thermal analysis modules, the heat flow value for testing measurement set as primary condition, meter Probe each several part Temperature Distribution is calculated, takes the temperature computation result of experiment middle probe temperature measuring point, then carry out with the temperature of experiment measurement Contrast, if deviation, within 10%, measurement result is reliable.
The present invention is disclosed as above with preferable case study on implementation, but is not limited to the present invention, any to be familiar with this specialty Technical staff, without departing from the scope of the present invention, according to the present invention technical spirit to above case study on implementation institute Any simple modification, equivalent change and modification done, still belongs to technical solution of the present invention scope.

Claims (8)

  1. A kind of 1. probe for measuring hall thruster wall ion hot-fluid, it is characterised in that:It includes metallic rod (1), radiating block And temperature thermometric line (6) (3);Metallic rod (1) connects radiating block (3), and thermometric boss (2), thermometric are also equipped with metallic rod (1) Temperature thermometric line (6), metallic rod (1), thermometric boss (2) are connected on boss (2) two surfaces relative with radiating block (3) respectively It is non-magnetic rustproof Steel material with radiating block (3).
  2. A kind of 2. probe for measuring hall thruster wall ion hot-fluid according to claim 1, it is characterised in that:Thermometric is convex Platform (2) along metallic rod (1) circumferentially.
  3. A kind of 3. probe for measuring hall thruster wall ion hot-fluid according to claim 1 or claim 2, it is characterised in that:Gold Category bar (1), thermometric boss (2) and radiating block (3) are the concentric cylinder by being made into integration without magnetic 1Cr18Ni9Ti stainless steels.
  4. A kind of 4. probe for measuring hall thruster wall ion hot-fluid according to claim 3, it is characterised in that:Temperature is surveyed Warm line (6) is electric thermo-couple temperature thermometric line.
  5. 5. according to a kind of probe for measuring hall thruster wall ion hot-fluid of claim 1,2 or 4, it is characterised in that: All sides of metallic rod (1) scribble heat-insulating material.
  6. A kind of 6. probe for measuring hall thruster wall ion hot-fluid according to claim 5, it is characterised in that:Heat insulating material Expect for adiabatic coating.
  7. 7. according to a kind of probe for measuring hall thruster wall ion hot-fluid of claim 1,2,4 or 6, its feature exists In:The distance of the front end face (5) of thermometric boss (2) and the front end face (4) of metallic rod (1) is 10mm.
  8. A kind of 8. method for measuring hall thruster wall ion hot-fluid, it is characterised in that:The step of this method is:
    Step 1: bore mounting hole on hall thruster ceramics wall;
    Step 2: several temperature thermometric lines (6) are respectively arranged on two relative faces of thermometric boss (2) and radiating block (3), The end of probe of temperature thermometric line (6) is connected on thermometric boss (2) and radiating block (3), and the output end of temperature thermometric line (6) is drawn To acquisition system;
    Step 3: heat insulating material is used into the end of metallic rod (1) to the metallic rod (1) between thermometric boss (2) and thermometric boss (2) Material cladding, the metallic rod (1) for coating heat-insulating material are arranged in mounting hole, make metallic rod (1) front end and heat-insulating material and ceramics Wall bottom hole flushes;
    Step 4: starting hall thruster, after hall thruster wall surface temperature reaches stable, certain negative electricity is provided to probe Position, electronics is masked completely, while the ion that probe receives reaches saturation;
    Probe, which reaches, to be measured the temperature of probe axial direction diverse location after hot stable state and can obtain hot-fluid, is expressed as:
    <mrow> <mi>q</mi> <mo>=</mo> <mi>&amp;lambda;</mi> <mi>A</mi> <mfrac> <mrow> <mi>d</mi> <mi>T</mi> </mrow> <mrow> <mi>d</mi> <mi>z</mi> </mrow> </mfrac> <mo>=</mo> <mi>&amp;lambda;</mi> <mi>A</mi> <mfrac> <mrow> <msub> <mi>T</mi> <mn>1</mn> </msub> <mo>-</mo> <msub> <mi>T</mi> <mn>2</mn> </msub> </mrow> <mrow> <msub> <mi>z</mi> <mn>1</mn> </msub> <mo>-</mo> <msub> <mi>z</mi> <mn>2</mn> </msub> </mrow> </mfrac> </mrow>
    Q-probe measurement hot-fluid, unit:Watt;
    The thermal conductivity factor of λ-probe;Probe material 1Cr18Ni9Ti thermal conductivity factor is 21W/ (mK);
    The temperature of T-probe, unit:K;
    A-probe front face area, unit:m2;A=π D2/4;D is metal shank diameter, unit:m;
    Z-probe axial distance, unit:m;
    Wherein, axial displacement of temperature thermometric line (6) end of probe apart from radiating block (3) bottom surface is z on thermometric boss (2) surface1, Measurement temperature average value is T1
    Temperature thermometric line (6) end of probe distance probes radiating block (3) at the end of the axial displacement on radiating block (3) surface is z2, measurement Temperature averages are T2
CN201710860394.1A 2017-09-21 2017-09-21 A method of measurement hall thruster wall surface ion hot-fluid Active CN107607230B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201710860394.1A CN107607230B (en) 2017-09-21 2017-09-21 A method of measurement hall thruster wall surface ion hot-fluid

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201710860394.1A CN107607230B (en) 2017-09-21 2017-09-21 A method of measurement hall thruster wall surface ion hot-fluid

Publications (2)

Publication Number Publication Date
CN107607230A true CN107607230A (en) 2018-01-19
CN107607230B CN107607230B (en) 2019-10-22

Family

ID=61061717

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201710860394.1A Active CN107607230B (en) 2017-09-21 2017-09-21 A method of measurement hall thruster wall surface ion hot-fluid

Country Status (1)

Country Link
CN (1) CN107607230B (en)

Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
SU838429A1 (en) * 1979-08-06 1981-06-15 Предприятие П/Я М-5539 Thermal flow gage in shock tube
US20040028117A1 (en) * 2001-12-17 2004-02-12 Cordes Steven Alan Scanning heat flow probe
CN103674330A (en) * 2013-12-13 2014-03-26 绵阳富林岚科技有限责任公司 Thermal current sensor
CN104048767A (en) * 2014-05-29 2014-09-17 北京航空航天大学 Strip-shaped foil type transient radiation heat flow meter
CN104950344A (en) * 2015-06-03 2015-09-30 中国科学院南海海洋研究所 Seabed heat flow long-term observation probe based on underwater robot platform

Patent Citations (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
SU838429A1 (en) * 1979-08-06 1981-06-15 Предприятие П/Я М-5539 Thermal flow gage in shock tube
US20040028117A1 (en) * 2001-12-17 2004-02-12 Cordes Steven Alan Scanning heat flow probe
CN103674330A (en) * 2013-12-13 2014-03-26 绵阳富林岚科技有限责任公司 Thermal current sensor
CN104048767A (en) * 2014-05-29 2014-09-17 北京航空航天大学 Strip-shaped foil type transient radiation heat flow meter
CN104950344A (en) * 2015-06-03 2015-09-30 中国科学院南海海洋研究所 Seabed heat flow long-term observation probe based on underwater robot platform

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
田立成等: ""LHT-100自励磁霍尔推力器热特性测试和热真空实验研究"", 《推进技术》 *

Also Published As

Publication number Publication date
CN107607230B (en) 2019-10-22

Similar Documents

Publication Publication Date Title
CN102288641B (en) Method for measuring high temperature thermal conductivity coefficient
Sanderson et al. Transient heat flux measurement using a surface junction thermocouple
Chavers et al. Momentum flux measuring instrument for neutral and charged particle flows
Book et al. Effect of anode temperature on hall thruster performance
CN103884646B (en) A kind of NOZZLE ARC ablate metals vapour concentration measuring system based on Fibre Optical Sensor
CN107543634B (en) Striped formula radiant heat flux measuring device based on fexible film thermoelectric pile
CN111879443A (en) Tool for measuring density of gas-liquid two-phase heat flow in rocket engine
CN103471738A (en) Method for on-line temperature monitoring of exciting winding of plasma Hall effect thruster
Stöckel et al. Advanced probes for edge plasma diagnostics on the CASTOR tokamak
Wu et al. Analytical investigation of outflow currents in applied field magnetoplasmadynamic thrusters
CN107607230B (en) A method of measurement hall thruster wall surface ion hot-fluid
Bobzin et al. Macroscopic particle modeling in air plasma spraying
CN106771703B (en) Hall thruster anode thermal power measurement method
Datta et al. The structure of 3-D collisional magnetized bow shocks in pulsed-power-driven plasma flows
Vukoslavĉević et al. Influence of velocity gradients on measurements of velocity and streamwise vorticity with hot‐wire X‐array probes
CN110677968B (en) Method and device for monitoring plasma jet velocity
Zhang et al. Calibrated cylindrical mach probe in a plasma wind tunnel
Burton et al. Exit-plane electrostatic probe measurements of a low-power arcjet
CN104048767A (en) Strip-shaped foil type transient radiation heat flow meter
Cao et al. Specific signal imaging velocimetry for rarefied plasma flows
Sapozhnikov et al. Heatmenry
CN103592046A (en) Integral type thermocouple
Zhao et al. A review on plasma diagnosis technology of pulsed plasma thruster
Bufton et al. Measured plasma properties at the exit plane of a 1 kW arcjet
Paul Irudayaraj et al. Determination of Electrical Conductivity in Potassium Seeded Oxy-Fuel Flame using RF Coil Approach

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