CN103832599A - Composite shielding method for satellite to resist total dose effect - Google Patents

Composite shielding method for satellite to resist total dose effect Download PDF

Info

Publication number
CN103832599A
CN103832599A CN201210490975.8A CN201210490975A CN103832599A CN 103832599 A CN103832599 A CN 103832599A CN 201210490975 A CN201210490975 A CN 201210490975A CN 103832599 A CN103832599 A CN 103832599A
Authority
CN
China
Prior art keywords
shielding
metal
satellite
total dose
atomic number
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.)
Pending
Application number
CN201210490975.8A
Other languages
Chinese (zh)
Inventor
胡鉴航
冯颖
韩建伟
蔡明辉
杨涛
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.)
National Space Science Center of CAS
Original Assignee
National Space Science Center of CAS
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 National Space Science Center of CAS filed Critical National Space Science Center of CAS
Priority to CN201210490975.8A priority Critical patent/CN103832599A/en
Publication of CN103832599A publication Critical patent/CN103832599A/en
Pending legal-status Critical Current

Links

Images

Abstract

The invention provides a composite shielding method for a satellite to resist a total dose effect. The composite shielding method for the satellite to resist the total dose effect is characterized in that according to the method, double-layer materials are used for shielding, metal with the low atomic number is used for an outer layer, and metal with the high atomic number is used for an inner layer. The metal with the low atomic number is aluminium, and the metal with the high atomic number is tantalum. According to the composite shielding method, the mass ratio of the metal aluminium and the metal tantalum is determined according to the specific orbit environment where the satellite is placed. According to the technical scheme, under the condition that the same shielding effect as a traditional method is achieved, the total quantity of the used shielding materials is smaller; or under the condition of the same shielding quality, a better shielding effect can be achieved.

Description

A kind of composite shielding method for resistant to total dose effect on satellite
Technical field
The present invention relates to a kind of anti-radiation shield method, is mainly the shielding to the suffered total dose of electronics package on satellite, the invention provides a kind of composite shielding method for resistant to total dose effect on satellite.
Background technology
Satellite orbits and is faced with severe space radiation environment, comprise solar proton, radiation belts of the Earth and galactic cosmic ray etc., the above two are the main particle sources of causing total dose effect, these high energy charged particles incident satellite electron devices, make device material ionization produce total dose effect, the performance of electronics package is caused and had a strong impact on.Conventionally its total dose suffering of satellite about several years time in orbit has substantially exceeded the level of general electronics package resistant to total dose, and therefore radiation-resistant work is very necessary.
The means of defence of total dose mainly contains two kinds: 1) microelectronics radiation hardening technology, by microelectronic material choose, the measure such as microcircuit design, technological design, topology layout reduces the impact of total dose on parameters of electronic device; 2) adopt exterior material to shield device.
Method proposed by the invention belongs to the second.Common shielding material is to adopt simple aluminium, and effect is often unsatisfactory, and for reaching the shield effectiveness of expection, needs the aluminum that thickness is larger to shield, and has wasted the limited quality resource of satellite.
Summary of the invention
The object of the invention is to, for overcoming the problems referred to above, the invention provides the composite shielding method of resistant to total dose effect on a kind of satellite.
For achieving the above object, the invention provides a kind of composite shielding method for resistant to total dose effect on satellite, it is characterized in that, described method is: adopt double layer material to shield, outer adopt the metal of low atomic number and internal layer adopts the metal of high atomic number.
The metal of above-mentioned low atomic number is aluminium, and the metal of high atomic number is tantalum.
Compared with prior art, technical advantage of the present invention is:
In the case of reaching the shield effectiveness identical with orthodox method, the shielding material total mass of the double layer material that adopts is less; And the in the situation that of same screening mass, can reach better shield effectiveness.
Accompanying drawing explanation
Fig. 1-a and 1-b are the dosage of certain electron spectrum after different equivalent thickness and different component shielding material;
Fig. 2 is the Contrast on effect of the shielding of traditional fine aluminium and pure tantalum screen and composite shielding.
The specific embodiment
Below in conjunction with accompanying drawing, content of the present invention is described in detail.
Adopt double layer material to shield in order to reduce the quality of shielding material under the prerequisite reaching expection shield effectiveness, to the present invention proposes, concrete scheme is the outer metal (as aluminium) that adopts low atomic number, and internal layer adopts the metal (as tantalum) of high atomic number.
From nuclear physics correlation theory, the material actv. scattered electron more that atomic number (Z) is high, but the stopping power of low Z materials unit mass is lower, and produce more bremsstrahlung (bremsstrahlung coefficient is directly proportional to atomic number and the incident electron energy of material), if and pass through again low Z materials after first allowing electronics underspeed by high Z materials, can effectively reduce by high Z materials like this energy of electronics, the bremsstrahlung producing in low Z materials thus reduces, and in this way the electron dose after shielding can significantly reduce.Therefore main problem is exactly will solve in the situation that shielding material equivalent thickness is constant, and high atomic number material and low atomic number material can obtain optimum shield effectiveness with which kind of ratio combination.
The present invention, in conjunction with the space environment feature of typical satellite orbit, regulates the thickness of two-layer screen layer, filters out optimum factors for radiation shielding design under the condition that takies minimum quality resource.
Concrete thinking is, choose respectively metallic aluminium and tantalum as low Z and high Z metal composition double layer screen material, allow particle pass through after shielding, record the total dose that particle produces in detector, under the constant condition of shielding material equivalent thickness, make the percent by weight of aluminium be increased to 100% from 0%, obtain the curve that a total dose changes with the percent by weight of aluminium, and then change shielding material equivalent thickness, make many such curves, can draw optimum assembly in different equivalent thickness situation (being the percentum of hour aluminium of dosage) by analyzing.According to the concrete orbital environment at satellite place, metallic aluminium accounts for the 20%-40% of total screening mass.
Embodiment mono-:
Make analogue computing as an example of the electron spectrum of certain track example, the equivalent thickness of aluminium of shielding material from 2 millimeters, 2.5 millimeters to 20 millimeters not etc., the mass ratio that wherein every kind of equivalent thickness of aluminium is got respectively aluminium be 0%, 5% to 100% totally 12 kinds of combinations carry out analogue computing.
Result of calculation as shown in Fig. 1-a and 1-b, the percent by weight that wherein abscissa is aluminium, ordinate be shielding after relative total dose, different curves represent different equivalent thickness of aluminiums.As seen from the figure, compare with traditional fine aluminium shielding, adopt composite shielding post dose to reduce a lot, while being 2.5mm such as equivalent thickness of aluminium, the composite shielding effect of 10% aluminium is best; If increase equivalent thickness, dosage nadir can move to the heavy larger side of aluminum ratio, and during such as 3.0mm, nadir is 15%, and nadir is 25% during to 5.5mm.
Fig. 2 be fine aluminium and pure tantalum to the depth curve of electron spectrum with carry out the contrast after composite shielding optimal design, visible composite shielding can effectively reduce total dose, and the larger effect of equivalent thickness is more obvious.Such as the 3mm equivalent thickness of aluminium in the situation that, the shield effectiveness of this composite shielding method is 4 times of left and right of common fine aluminium.
It should be noted last that, above embodiment is only unrestricted in order to technical scheme of the present invention to be described.Although the present invention is had been described in detail with reference to embodiment, those of ordinary skill in the art is to be understood that, technical scheme of the present invention is modified or is equal to replacement, do not depart from the spirit and scope of technical solution of the present invention, it all should be encompassed in the middle of claim scope of the present invention.

Claims (4)

1. for a composite shielding method for resistant to total dose effect on satellite, it is characterized in that, described method is:
Adopt double layer material to shield, outer adopt the metal of low atomic number and internal layer adopts the metal of high atomic number.
2. the composite shielding method for resistant to total dose effect on satellite according to claim 1, is characterized in that, the metal of described low atomic number is aluminium.
3. the composite shielding method for resistant to total dose effect on satellite according to claim 1 and 2, is characterized in that, the metal of described high atomic number is tantalum.
4. the composite shielding method for resistant to total dose effect on satellite according to claim 3, is characterized in that, described metallic aluminium accounts for the 20%-40% of total screening mass.
CN201210490975.8A 2012-11-27 2012-11-27 Composite shielding method for satellite to resist total dose effect Pending CN103832599A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201210490975.8A CN103832599A (en) 2012-11-27 2012-11-27 Composite shielding method for satellite to resist total dose effect

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201210490975.8A CN103832599A (en) 2012-11-27 2012-11-27 Composite shielding method for satellite to resist total dose effect

Publications (1)

Publication Number Publication Date
CN103832599A true CN103832599A (en) 2014-06-04

Family

ID=50796563

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201210490975.8A Pending CN103832599A (en) 2012-11-27 2012-11-27 Composite shielding method for satellite to resist total dose effect

Country Status (1)

Country Link
CN (1) CN103832599A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106675391A (en) * 2015-11-11 2017-05-17 北京卫星环境工程研究所 Radiation-proof thermal control coating and manufacturing method thereof
CN113543615A (en) * 2021-06-29 2021-10-22 中国科学院长春光学精密机械与物理研究所 Irradiation protection method for space electronic equipment

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP2151704A1 (en) * 2008-08-07 2010-02-10 Thales Alenia Space Italia S.p.A. Shielding device for optical and/or electronic apparatuses, and space vehicle comprising such device
CN102490913A (en) * 2011-11-15 2012-06-13 上海卫星工程研究所 Anti-total-dose shielding device

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP2151704A1 (en) * 2008-08-07 2010-02-10 Thales Alenia Space Italia S.p.A. Shielding device for optical and/or electronic apparatuses, and space vehicle comprising such device
CN102490913A (en) * 2011-11-15 2012-06-13 上海卫星工程研究所 Anti-total-dose shielding device

Non-Patent Citations (1)

* Cited by examiner, † Cited by third party
Title
杨晓军等: "金属/聚合物复合材料对中能电子的屏蔽作用研究", 《核技术》, vol. 29, no. 11, 10 November 2006 (2006-11-10), pages 817 - 820 *

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN106675391A (en) * 2015-11-11 2017-05-17 北京卫星环境工程研究所 Radiation-proof thermal control coating and manufacturing method thereof
CN106675391B (en) * 2015-11-11 2019-03-05 北京卫星环境工程研究所 Radiation protection thermal control coating and its manufacturing method
CN113543615A (en) * 2021-06-29 2021-10-22 中国科学院长春光学精密机械与物理研究所 Irradiation protection method for space electronic equipment

Similar Documents

Publication Publication Date Title
CN102490913A (en) Anti-total-dose shielding device
Zeynali et al. Shielding protection of electronic circuits against radiation effects of space high energy particles
CN103832599A (en) Composite shielding method for satellite to resist total dose effect
CN102127391B (en) Radiation-proof composite material and preparation method thereof
Atwell et al. Mitigating the effects of the space radiation environment: a novel approach of using graded-z materials
CN104962128B (en) A kind of preparation of resistant to total dose curtain coating material and coating method
CN105609151B (en) A kind of X-ray shield structure based on ABSORPTION EDGE principle
Pang et al. Development of high quantum efficiency flat panel detectors for portal imaging: Intrinsic spatial resolution
CN105719716B (en) A method of mitigating radiation hardness robot and shields weight
CN111554426B (en) Hard X-ray and photoelectron shielding composite material
US11887743B2 (en) Metal oxide impregnated conformal coatings for ionizing radiation shielding
Bogomolov et al. The Deuterium Cosmic Ray Intensity from Balloon Measurement in Energy Range 0.8-1.8 GeV/nucl.
Birch et al. Investigation of background in large-area neutron detectors due to alpha emission from impurities in aluminium
Escuder et al. Numerical correction for secondary fluorescence across phase boundaries in EPMA
Cherry Measuring the Lorentz factors of energetic particles with transition radiation
O’Connor et al. Mitigating space radiation using magnesium (-lithium) and boron carbide composites
Mann et al. Sensitivity of ion induced X-ray analysis for surface layers on thick silicon substrates
Bozhko et al. A STUDY OF IMPROVEMENT OF A TECHNOLOGY FOR OBTAINING RADIATION-PROTECTING MATERIALS FOR SPACECRAFT AND ROCKETRY SYSTEMS
Smallcombe et al. SPectrometer for Internal Conversion Electrons (SPICE) at TRIUMF-ISAC
RU2619455C1 (en) Composition for the protection of electronic devices from the impact of radiation of the space matter
Hajdas et al. Spacecraft activation and South Atlantic Anomaly profiles measured with RHESSI satellite
Deiev et al. The research of X-ray and gamma radiation absorption by layered structures
Dachev et al. Observation of the earth radiation environment by R3D-B2 instrument on Foton M2 satellite
CN112967938A (en) Aerospace-level integrated circuit total dose shielding method and anti-radiation reinforcement effect verification method
Yunfei et al. Study on correction factor of synchrotron radiation x-ray free air ionization chamber composite loss

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C02 Deemed withdrawal of patent application after publication (patent law 2001)
WD01 Invention patent application deemed withdrawn after publication

Application publication date: 20140604