ASTM F1263-1999(2005) Standard Guide for Analysis of Overtest Data in Radiation Testing of Electronic Parts《电子元件辐射试验中超限试验数据的分析》.pdf
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1、Designation: F 1263 99 (Reapproved 2005)Standard Guide forAnalysis of Overtest Data in Radiation Testing of ElectronicParts1This standard is issued under the fixed designation F 1263; the number immediately following the designation indicates the year oforiginal adoption or, in the case of revision,
2、 the year of last revision. A number in parentheses indicates the year of last reapproval. Asuperscript epsilon (e) indicates an editorial change since the last revision or reapproval.1. Scope1.1 This guide covers the use of overtesting in order toreduce the required number of parts that must be tes
3、ted to meeta given quality acceptance standard. Overtesting is testing asample number of parts at a stress higher than their specifica-tion stress in order to reduce the amount of necessary datataking. This guide discusses when and how overtesting may beapplied to forming probabilistic estimates for
4、 the survival ofelectronic piece parts subjected to radiation stress. Someknowledge of the probability distribution governing the stress-to-failure of the parts is necessary though exact knowledgemay be replaced by over-conservative estimates of this distri-bution.2. Referenced Documents2.1 Military
5、 Standards:MIL-PRF 19500 Semiconductor Devices, General Specifi-cations for2MIL-PRF 38535 Integrated Circuits (Microcircuit Manu-facturing)23. Terminology3.1 Description of Term:3.1.1 confidencethe probability, C, that at least a fraction,P, of the electronic parts from a test lot will survive in ac
6、tualservice; since radiation testing of electronic parts is generallydestructive, this probability must be calculated from tests onselected specimens from the lot.3.1.2 rejection confidencethe probability, R, that a lot willbe rejected based on destructive tests of selected specimens ifmore than a s
7、pecified fraction P of the parts in the lot will failin actual service.3.1.3 Discussion of Preceding TermsStrictly speaking,most lot acceptance tests (be they testing by attributes orvariables) do not guarantee survivability, but rather that infe-rior lots, where the survival probability of the part
8、s is less thanprobability, P, will be rejected with confidence, C. In order toinfer a true confidence, it would require a Bayes Theoremcalculation. In many cases, the distinction between confidenceand rejection confidence is of little practical importance.However, in other cases (typically when a la
9、rge number of lotsare rejected) the distinction between these two kinds ofconfidence can be significant. The formulas given in this guideapply whether one is dealing with confidence or rejectionconfidence.4. Summary of Guide4.1 This guide is intended to primarily apply to sampling byattribute plans
10、typified by Lot Tolerance Percent Defective(LTPD) tables given in MIL-PRF 38535 and MIL-PRF 19500,and contains the following:4.1.1 An equation for estimating the effectiveness of over-testing in terms of increased probability of survival,4.1.2 An equation for the required amount of overtestinggiven
11、a necessary survival probability, and4.1.3 Cautions and limitations on the method.5. Significance and Use5.1 Overtesting should be done when (a) testing by vari-ables is impractical because of time and cost considerations orbecause the probability distribution of stress to failure cannotbe estimated
12、 with sufficient accuracy, and (b) an unrealisticallylarge number of parts would have to be tested at the specifi-cation stress for the necessary confidence and survival prob-ability.6. Interferences6.1 Probability DistributionsIn overtesting, a knowledgeof the probability distribution governing str
13、ess to failure isrequired, though it need not be specified with the sameaccuracy necessary for testing by variables. For bipolar tran-sistors exposed to neutron radiation, the failure mechanism isusually gain degradation and the stress to failure is known tofollow a lognormal distribution.3For bipol
14、ar transistors ex-posed to total dose the use of the lognormal distribution is also1This guide is under the jurisdiction of ASTM Committee F01 on Electronicsand is the direct responsibility of Subcommittee F01.11 on Quality and HardnessAssurance.Current edition approved Jan. 1, 2005. Published Janua
15、ry 2005. Originallyapproved in 1989. Last previous edition approved in 1999 as F 1263 99.2Available from Standardization Documents Order Desk, Bldg. 4 Section D, 700Robbins Ave., Philadelphia, PA 19111-5094, Attn: NPODS.3Messenger, G. C., Steele, E. L., “Statistical Modeling of SemiconductorDevices
16、for the TREE Environment, Transactions on Nuclear Science NS-15,1968, p. 4691.1Copyright ASTM International, 100 Barr Harbor Drive, PO Box C700, West Conshohocken, PA 19428-2959, United States.fairly good.4For more complex electronics and other kinds ofradiation stress, the lognormal distribution is
17、 widely used inestimating the failure probabilities of electronic piece parts,and therefore this standard governs the use of a lognormaldistribution. However, caution should be exercised when theprobability distribution of stress to failure is not well estab-lished. Nevertheless, even if the lognorm
18、al distribution doesnot strictly apply, the equations given in Section 7 will hold aslong as a sufficiently conservative estimate was made of thevariability of the parts within the stress range of interest.56.2 Time Dependent Post Radiation EffectsIn total dosetesting annealing and rebound effects c
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