NATL INST. OF STAND & TECH
AlllDS T73TD7 igg
REFERENGt Publi-
cations
^~So.
NBS TECHNICAL NOTE 1185
U.S. DEPARTMENT OF COMMERCE/National Bureau of Standards
-QC—100
. U5753
I Jo . 118
1934
J
Bibliography of
Data on Electrical
Breakdown in Gases
NATSONAL BUREAU OF STANDARDS
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NATIONAL BUREAtfOF STANDARDS
LIBRABY
Bibliography of Data on -^^i'
Electrical Breakdown in Gases Qc\oo
Ho. i\^^
R. J. Van Brunt 1 R 2 4-
W. E. Anderson
Center for Electronics and Electrical Engineering
National Engineering Laboratory
National Bureau of StandardsWashington, DC 20234
Sponsored by:
Office of Electric Energy SystemsDepartment of EnergyWashington, DC 20585
*<"fCAU O*
U.S. DEPARTMENT OF COMMERCE, Malcolm Baldrige, Secretary
NATIONAL BUREAU OF STANDARDS, Ernest Ambler, Director
Issued April 1984
National Bureau of Standards Technical Note 1185Natl. Bur. Stand. (U.S.),Tech. Note 1185, 170 pages (Apr. 1984)
CODEN: NBTNAE
U.S. GOVERNMENT PRINTING OFFICEWASHINGTON: 1984
For sale by the Superintendent of Documents, U.S. Government Printing Office, Washington, DC 20402
TABLE OF CONTENTS
Page
LIST OF TABLES iv
Abstract 1
I, Introduction 1
II, Criteria for Selection 3
II. Arrangement of Bibliography 5
IV. Definitions of Codesand Notations 5
V. Acknowledgments 9
VI. Gas Index 10
VII. Author Index 102
VIII. References 122
IX. Technical Conference Proceedings 164
111
LIST OF TABLES
Page
Table I. Definition of Category Code 6
IV
BIBLIOGRAPHY OF DATA ON ELECTRICAL BREAKDOWN IN GASES
R. J. Van Brunt and W. E. Anderson
This report consists of a bibliography ofcurrently published data on electrical breakdownin gases. The bibliography contains a list ofarchival papers and books published since 1950, anindex indicating the references that giveparticular types of data for each gas, an authorindex, and a list of relevant, regular technicalconferences. The citations given in thebibliography contain experimental or theoreticaldata on breakdown which include:
1) sparking potentials;2) breakdown voltages;3) critical fields, or field-to-gas density
ratios;4) corona inception voltages;5) voltage-time characteristics;6) relative and absolute dielectric
strengths; and7) breakdown probabilities.
Types of data considered include those whichapply to uniform and nonuniform fields; ac, dc,and impulse voltages; and possible effects ofparticles, surfaces, interfaces, and corona. Thisbibliography is intended to serve as a guide inlocating data on breakdown which are most relevantto particular applications.
Key words: bibliography; critical fields; coronaonset; discharge inception; electrical breakdown;gases; sparking potentials.
I . Introduction
This bibliography is intended to serve as a guide tothe currently available published data on electricalbreakdown for gases and vapors. It is generally recognizedthat although an enormous quantity of data exists, it isoften difficult to locate those most applicable to a givenset of conditions. This is due to the complex nature ofdata on electrical breakdown which depend on a broad rangeof conditions including widely different gas pressures andtemperatures, gas composition, electrode materials,electrode configurations, voltage waveforms, proximity ofsolid dielectrics, etc. All of these parameters can beexpected to have a significant influence on the electricalbreakdown characteristics of a system. Thus, for example.
data obtained for aniform-electr ic-f ield configurationscannot generally give reliable predictions of breakdown inhighly nonuniform electric-field configurations. Similarlydata found for slowly varying or constant electric fieldsmay not be applicable to situations where there are rapidlyvarying fields. In general, the breakdown potential of anelectrode gap is not solely a property of the insulating gasmedium. With this complexity in mind, this bibliography isdesigned to help simplify the task of finding data whichcorrespond to configurations or operating conditions thatmost nearly match those for particular applications ofinterest.
The information contained in this bibliography existsin computerized form which can be easily updated andperiodically printed out as additional relevant referencesare found. Revised and updated versions of thisbibliography, either as computer printout or in floppy diskform, will periodically be made available upon request tothe National Bureau of Standards, Electrosystems Division,Washington, DC 20234.
The bibliography in its present form is believed toinclude most of the major archival papers and bookspublished since 1950 which contain data on electricalbreakdown for insulating gases. All of the referenceslisted have been examined to determine that they do indeedcontain breakdown data. In the category of electrical-breakdown data are included:
1) sparking potentials;2) breakdown voltages;3) critical fields, or field-to-gas density ratios;4) corona inception voltages;5) voltage-time characteristics;6) relative and absolute dielectric strengths; and7) breakdown probabilities.
These are all closely related quantities in the sense thatthey indicate the applied potential or electric field atwhich a sufficiently high rate of ionization occurs so thatthe conductivity of the gas reaches the point wheredischarge initiation or electrical breakdown will occur withsignificant probability. There are, however, distinctionsamong these quantities which are not always clearly definedor discussed in the literature, and no attempt has been madeto address these issues in preparing the bibliography.
As an example, corona inception (also called"discharge inception" or "partial discharge inception")usually refers to the onset of a self-sustaining, localizeddischarge near the most highly stressed electrode in anonuniform-electr ic-f ield gap. Although a corona dischargeenhances the conductivity of the gas, it is not usually
considered to be a true breakdown because it does not bridgethe electrode gap, i.e. , it is not associated withionization of the gas along the entire distance between twoelectrodes. In most papers, the distinction between coronainceptions and breakdown voltages is made quite clear and,as a general rule, corona inception will occur at a lowervoltage than complete breakdown in nonuniform-f ield gaps.
It is nevertheless evident that in some cases there aredisagreements or uncertainties in the definitions of thequantities considered here for inclusion as breakdown data."Dielectric strength" in most cases, but not always,corresponds to breakdown for uniform, static-electric-fieldconfigurations under gap and pressure conditions where thesimilarity law holds, namely that the breakdown voltage is afunction only of the product of gas pressure and electrodegap spacing. Data on critical-field to gas-density ratiosalso presumably apply only to uniform-electric fieldsituations inasmuch as they are usually derived frommeasurements or calculations of ionization growth orionization and attachment coefficients for gases at lowpressures in uniform fields. The extent to which these datamay be reliably applied to nonuniform-f ield conditions or togas pressures different from those at which the coefficientswere determined is generally unknown. Caution should beexercised in the application of such data to configurationsthat deviate even slightly from uniformity such as spheregaps or as might result from electrode surfaceirregularities. The effects of minute surface protrusions,small particles, dust, surface charges, etc., which canperturb the electric field in a gas are discussed in anumber of references included. Where possible these havebeen indicated by the code assigned to each reference asdiscussed below.
II . Criteria for Selection
The references cited in this bibliography were selectedaccording to the following criteria:
a) they correspond to an archival publication;b) they contain experimental or theoretical data on
breakdown or corona inception voltages or fields;c) they include gases and conditions considered
applicable to electrical insulation; andd) they have been published since 1950.
The list has been restricted to archival publications,i.e., journal publications and books, because: a) these arereadily available to almost everyone; and b) data presentedin these articles have presumably been subjected to criticalreview and thus have a greater likelihood of being correct.There are, of course, many conference proceedings andtechnical reports which may be assumed to contain useful and
reliable data on breakdown. On the other hand, datapresented at conferences or in reports, unless previouslypublished, are generally considered to be preliminary.Also, there are many conference proceedings and technicalreports that are not widely distributed and thus may bedifficult to obtain. Some of the major regular technicalconferences where data on gas breakdown have been presentedand for which proceedings or abstracts were usuallypublished are listed here separately (Section IX), Noattempt has been made to identify specific papers or datagiven at these conferences.
All of the papers listed have been examined to verifythat they do indeed contain data on electrical breakdown asdefined in the Introduction, No attempt was made toevaluate critically any data given in these references as abasis for selection. It is clear that in some cases thereare obvious disagreements and disputes which may or may nothave been resolved. Included here are all data independentof their known or assumed reliability. Papers which dealonly with the phenomenology or physics of gas breakdown werenot included despite their possible importance in adding toour understanding of the mechanisms involved. Again thisbibliography is intended to be an aid to those in need ofdata on breakdown.
The list has been restricted to gases consideredrelevant to electrical-insulation technology. Gases such asmetal vapors which are unlikely components in gaseousinsulation have been excluded unless they happen to havebeen studied along with other gases which are of relevance.There are, however, metal vapors like Hg which might beunavoidable components or important contaminants in gaseousinsulation. Serious consideration will be given toincluding these in future versions of the bibliography.
The data in the bibliography cover a wide range of gaspressures and temperatures, and although in some casessignificant and interesting dependences on these parametersare observed, no attempt is made to indicate the rangesconsidered in each case. Thus, for example, two or morereferences indicated as having data on static-uniform-fieldbreakdown for N^ may actually correspond to results obtainedat quite different pressures and temperatures.
The electrode and field configurations considered varyover a wide range, e,g,, from small uniform field gaps tolarge, practical electric-power-line simulations. Theresults for static, uniform field conditions are generallyconsidered to be more fundamental in indicating thedielectric strength for coll is ional-ionizat ion processes.It is clear, however, that the gas will generally behavequite differently under less uniform-gap and t ime-vary ing-voltage conditions and, therefore, because results for these
conditions are of considerable importance in the design ofthe insulating systems, their inclusion was consideredimperative.
For alternating voltages, only data on breakdown at thepower frequencies of 60 Hz and 50 Hz have been included. Itmight be argued that measurements or calculations performedfor higher frequencies are also relevant to insulationapplications. Perhaps these should be included in futureversions of this bibliography. They were arbitrarilyexcluded here because of difficulties in agreeing on anacceptable way of categorizing these data, and because ofthe limited usefulness of this kind of information for thedesign and testing of electrical insulation, particularly inelectric-power applications.
The exclusion of papers and books published before 1950should not be interpreted as a denigration of these works.Although it is true that some earlier studies have sincebeen supplanted by more recent works, there certainlyremains much valuable information on breakdown frominvestigations carried out before 1950. It was essential toplace some restrictions on the number of references to beincluded, and it seemed unnecessary to include papers whichhave already been adequately discussed in the previousreviews listed here. The absence of any publications whichmight be perceived as meeting the above criteria is mostlikely due to the fact that they have not been found.Hopefully, such omissions can be corrected in futureversions of this bibliography.
III. Arrangement of Bibliography
The report is arranged in four parts: an index to thebibliography which indicates the types of breakdown dataavailable for each gas; an author index; a list of citationswith assigned numbers determined by the alphabetical orderof principal author; and a list of relevant technicalconferences. The index lists the gases and gas mixturesalphabetically according to the stoichiometric chemicalformulae. The symbols "x" beside the reference numbers inthe index indicate that they contain information on theinfluences of particles, surfaces, interfaces, or corona onbreakdown.
IV. Definitions of Codes and Notations
All references that are cited here were entered into acomputer with a corresponding code which gives an indicationof the type of data which they contain. The code consistsof two parts. The first part gives the gas or gases thathave been included according, where possible, to theirchemical formulae, and the second part gives the nature ofthe investigation. Included in the latter are:
a) an identifier indicating that the work is eitherexperimental, theoretical, a review, or somecombination of these;
b) an identifier indicating if the electric fieldconfiguration is either uniform or nonuniform;
c) an identifier indicating the type of voltagesapplied, i.e., either dc, ac (at power frequenciesof 60 or 50 Hz), or impulse; and
d) an identifier of special effects considered, whichwas limited to:
1) surface effects;2) particle effects;3) interface effects; and4) corona.
The computer code used in the categorization of eachreference is defined in Table I. The code assigned to eachreference consists of at least one entry each from sets 1-3,and one or more possible entries from set 4 as indicated inthe Table. These codes do not appear explicitly in thepresent printed version, although they are implied in theindex. The codes do, however, appear in the computer diskfile format. It is important to emphasize that the codeshave been assigned to references and not to the gases.References which include more than one gas may notnecessarily include the same types of data for all gases.This is especially likely in review articles. Therefore,the index should be interpreted only as indicating thepossible types of data which might be available for eachgas. The actual existence of such data can, of course, onlybe verified by examination of the references cited.
Table I. Definition of Category Code
Set Code Category
1 E ExperimentalT TheoreticalR Review
2 U Uniform FieldN Nonuniform Field
3 D Direct VoltageA Alternating VoltageI Impulse
4 S Surface EffectsP Particle EffectsF Interface EffectsC Corona
It should be noted that special difficulties were oftenencountered in attempting to decide on the proper code to beentered for each citation. Attention should be drawn tosome of these. First it should be clear that all papers fitinto one or more of the categories of experimental,theoretical, or review. There are cases where more than oneof these applied. For some of these cases, however, onlyone category may be indicated. This was generally not anoversight, but rather a judgment based upon what appeared tobe the predominant emphasis of the work.
There was another difficulty sometimes encountered inattempting to decide if a particular work applied to eitheruniform or nonuniform fields. Results obtained in weaklynonuniforra-f ield gaps, e.g., sphere-sphere gaps, are oftenreferred to in the literature as "uniform-field breakdown."Some authors, however, would disagree with this inferenceand prefer a stricter definition of uniformity as applied togaps used for breakdown measurements. In cases where,despite the claims of the authors, doubt seemed to existabout the appropriateness for inclusion under uniform-fieldbreakdown, both the uniform and nonuniform field categorieswere assigned even though the results for only one electrodeconfiguration may have been reported.
Data included here under the category of alternatingvoltage (ac) relate only to the power frequencies of 50 or60 Hz. Sometimes the references indicated in this categoryalso present data at other frequencies. These, however,were not considered in determining the codes which wereassigned.
In considering the category of impulse breakdown, nodistinction was made as to the type of impulse voltage used.Thus, data in this category may include standard lightningand switching impulses as well as other non-standard impulseshapes and repetition rates. They may also include impulsessuperimposed on dc or ac voltages.
In the category of surface effects are includedinvestigations of the dependence of breakdown on propertiesof the electrode surfaces such as material roughness. Allother "surface" effects are placed in the category ofinterface effects which mainly have to do with breakdown inthe gas near or along a solid insulating surface. Thecategory of particle effects includes investigations of therole of both conducting and non-conducting solid particleson breakdown in a gas. The positions of the particles,although significant, have not been specified here. Theparticles may either be suspended in the gas, attached toelectrodes or interface surfaces, or be in random motion inthe discharge gap.
If papers are included under the category of corona,this usually means that data on corona inception or onsetvoltages are given. In a few special cases it may indicatethat effects of corona on breakdown have been considered orevaluated. In general, corona-onset voltages give anothermeasure of the dielectric strength of the gas can often bemore easily predicted theoretically than the breakdownvoltage in nonuniform-electr ic-f ield gaps.
The gases are denoted and listed alphabeticallyaccording to their presumed stoichiometric formulae withnotation given if possible to indicate molecular structure.All isomers are grouped together in the index listing. Forsome of the more complex molecular species, such as thefluorocarbon and hydrocarbon gases, there is a lack ofconsistency in denoting these by chemical formulae. In somecases only names of the compounds were given withoutindication of their molecular structures. In a few cases itwas admitted that the correct structure was unknown. Tradenames or non-standard terms have also been used to denotethe gases studied. Special difficulties appeared in thedesignations of isomers. Sometimes only the molecularstoich iometry , or relative proportions of the atomicconstituents were given without regard to the actualmolecular structure. Because of these difficulties, theidentities of some of the organic molecular species givenhere may be questionable. They are listed here according totheir presumed stoichiometric formulae with indicationsgiven, where possible, about the molecular structure. Insome cases the specific isomers considered may not becorrectly indicated here, and it may be necessary to examinethe original references to determine the possible correctmolecular structure. It should also be cautioned that fordata obtained at very high temperatures where moleculardissociation can occur, the identity of molecular gases maybe brought into question due to the possible presence ofatomic species and free radicals.
For gas mixtures, the constituents are listed inalphabetical order independent of their known relativeconcentrations, e.g., c-C.F„ + N^ + SF-. and CO2 + He + N^.Air, however, is treated as a special mixture and is simplydenoted here as AIR. The mixture N^ + o which is alsolisted may or may not contain the proper proportions of N-and Op to be considered as "air."
In the case of breakdown in air, the effect of humiditycan be quite important. When the gas is here denoted byAIR + H2O, it can be assumed that the data apply to humidair in which the water vapor content is known and specified.If the gas is simply denoted as AIR, then it was eitherindicated in the paper as being "dry" air, or the moisturecontent was not explicitly defined. While most authorsindicate whether or not the air is "dry," some do not.
For this bibliography electrical-breakdown data incomposite insulation have been included only if the gas is a
major, distinct, and well-separated component. Thus, forexample, breakdown in solids impregnated with gases has notbeen included. The possible presence of other nongaseousinsulating materials has been indicated, if possible, byinclusion in one or more of the categories corresponding tosurface, particle, or interface effects.
V. Acknowledgments
This report was prepared at the request andencouragement of the IEEE Insulation Society TechnicalCommittee S-32-11 on Gaseous Dielectrics, We would like toexpress our appreciation for the valuable suggestions andcontributions of the various members of the committee,especially Dr. S, J. Dale, Committee Chairman, WestinghouseCorp.; Dr. R. Hackam, University of Windsor, Canada;Dr. C. Miller, General Electric Company; Dr. W. Pfeiffer,Technische Hochschule, Darmstadt, West Germany;Dr. A. Pedersen, The Technical University, Lyngby, Denmark;Dr. J. K. Nelson, Rensselaer Polytechnic Institute, Troy,NY; and Dr. K. D. Srivastava, University of Waterloo,Canada.
VI, Gas Index
AIRPARTICLE SURFACE INTERFACE CORONA
EXPERIMENTALDC UNIFORM 4
374258617188
106117126138140145148151164168173193194243262263266273279313326357360364381389390395399408442
X
X
X
X
X
X
X
X
X
X
X
XX
X
X
DC NONUNIFORM 19 X38 X X507194 X
118141 X142 X149 X160 X
10
AIR (cont.
)
AC
AC
PARTICLE SURFACE INTERFACE CORONA) 162 X
164168 s X174 X193 X194 X204219237266279 X288293 X307313 X325326328 X332 X333357 X378 X379 X396 X407 X415 X421 X433440 X
UNIFORM 36 X37 X47 X70 X7172 X
168 X173 X194 X208 X X X279 X313 X326392395 X
NONUNIFORM 22 X23 X47 X5070 X7172 X8794 X
168 X
11
PARTICLE SURFACE INTERFACE CORONAAIR (cont.
)
175 X176 X182 X X194 X204208 XXX219231 X257 /
2 79 X313 X314 X X325326328 X358 X375 X407 X440 X453
IMPULSE UNIFORM 47 X70 X7172 X
117 X139140148187296313 X341381391405455
IMPULSE NONUNIFORM 2
5
6
J
11 X12 X20 X2627 X3135 X X47 X5070 X7172 X7475
12
AIR (cont.
)
100118
PARTICLE SURFACE INTERFACE CORONA
146147149 X159175 X176 X177179 X181 X189191210213220 X237247248 X X255256257259286287288289 X290291293 X307313 X327332 X339340341370 X371 X375 X380382 X388407 X409 X411 X412418 X420427429431441 X443 X
13
AIR (cont.
)
THEORETICALDC UNIFORM
DC NONUNIFORM
ACAC
UNIFORMNONUNIFORM
IMPULSE UNIFORMIMPULSE NONUNIFORM
444445448449452453455463
152163205207209232268273374414442
1
1916320420721623228133233533734638541436
204257297
5
7
13147189192210211235255257265332383384
PARTICLE SURFACE INTERFACE CORONA
XX
X
X
XX
XXXX
XXXXX
XX
14
AIR (cont.
)
REVIEWDC UNIFORM
DC NONUNIFORM
AC UNIFORM
AC NONUNIFORM
45486671738896
105119148163209244260264285334368422435454866717396
158163204234244260264285334422447456670717396
105285422456670717396
PARTICLE SURFACE INTERFACE CORONA
X
X X
XXX
XX
XX
X
XX
XX
XX
XX
XXX
X
X
X
X
XXXXXXXX
XXXXX
XX
15
PARTICLE SURFACE INTERFACE CORONAAIR (cont.
)
IMPULSE UNIFORM
IMPULSE NONUNIFORM
2042122222342572854224474570717396
148244285422354570717396
212221222234244257285422447
XX
XX
XX
X
X
X
XXXXX
XXXXXX
X
XXX
IR+CCl^F^REVIEWDC UNIFORM 96 X X XDC NONUNIFORM 96 X X XAC UNIFORM 96 X X XAC NONUNIFORM 96 X X XIMPULSE UNIFORM 96 X X XIMPULSE NONUNIFORM 96 X X X
AIR+CO^EXPERIMENTALDC NONUNIFORM 160
AIR+H^EXPERIMENTALDC UNIFORM 262
AIR+H^OEXPERIMENTALDC UNIFORM 8
58
16
PARTICLE SURFACE INTERFACE CORONAAIR+H-O (cont.
)
61 X238243357 X361381387393394
DC NONUNIFORM 160162328357387433
XXXX
AC NONUNIFORM 176328375386453
X
XX
IMPULSE UNIFORM 187381387
IMPULSE NONUNIFORM 2
9
1011 X35 X X69
176 X177179 X180226240241247248 X X287318 X371 X375 X386387388410420426428430431432439444
X
X
17
PARTICLE SURFACE INTERFACE CORONAAIR+H2O (cont.)
REVIEWDC UNIFORM
DC NONUNIFORM
AC
AC
UNIFORM
NONUNIFORM
IMPULSE UNIFORM
IMPULSE NONUNIFORM
446453
4596
2442854224596
2442854224474596
2854224596
2222854224474596
244285422354596
222244285422447
XXX
XXX
XX
XXX
XXX
XXXX
XX
XXX
XX
XXXX
XXXXX
XXX
XXXX
XXXXX
XXXX
AIR+N2EXPERIMENTALDC UNIFORMREVIEWDC UNIFORM
88
88
X
X
AIR+NO+NOEXPERIMENTALDC NONUNIFORM 160
AIR+SF,EXPERIMENTALDC UNIFORM 88
245273276
18
AIR+SF^ (cont.
)
b278399
DC NONUNIFORM 245274
AC NONUNIFORM 133IMPULSE UNIFORM 245IMPULSE NONUNIFORM 133
245382443
THEORETICALDC UNIFORM 273
278316
DC NONUNIFORM 316REVIEWDC UNIFORM 88 X
251 X X270 X X435
DC NONUNIFORM 251 X X270 X X
AC UNIFORM 251 X XAC NONUNIFORM 251 X XIMPULSE UNIFORM 270 X XIMPULSE NONUNIFORM 270 X X
ArEXPERIMENTALDC UNIFORM 81
82157 X164196197198199224 X292329353389390
DC NONUNIFORM 107149164170 X309
AC NONUNIFORM 67IMPULSE UNIFORM 139
— - 224 X324 X
IMPULSE NONUNIFORM 149324 X
PARTICLE SURFACE INTERFACE CORONA
XX
XXX
XX
XX
XX
19
PARTICLE SURFACE INTERFACE CORONAAr (cont.
)
THEORETICALDC UNIFORM 163DC NONUNIFORM 163IMPULSE UNIFORM 324 XIMPULSE NONUNIFORM 324 X
REVIEW-DC UNIFORM 45
646692 X
163244253260261264280285334438
DC NONUNIFORM 4566
163244260264285334
AC UNIFORM 4566
285AC NONUNIFORM 45
66285
IMPULSE UNIFORM 4592
244285
X
IMPULSE NONUNIFORM 45244285
Ar+C^HEXPERIMENTALDC UNIFORM 198
XX
XX
XXX
XX
XX
XX
XX
XXX
XX
XX
X
X
XX
XX
X
XXXXXXXXXX
XXXXX
Ar+C^HEXPERIMENTALDC UNIFORM 198
199
20
PARTICLE SURFACE INTERFACE CORONAAr+C^HEXPERIMENTALDC UNIFORM 197
Ar+C^Fj,EXPERIMENTALDC UNIFORM 81
Ar+C-jHgEXPERIMENTALDC UNIFORM 196
Ar+C^HEXPERIMENTALDC UNIFORM 199
Ar+n-Cc-H,^
EXPERIMENTALDC UNIFORM 198DC UNIFORM 199
Ar+C^HEXPERIMENTALDC UNIFORM 199
Ar+n-Cj.H,j.EXPERIMENTALDC UNIFORM 199
Ar+CH.EXPERIMENTALDC UNIFORM 196
Ar+CO^EXPERIMEI^TALDC NONUNIFORM 107
Ar+CsEXPERIMENTALDC UNIFORM 127
Ar+HREVIEWDC UNIFORM 264DC NONUNIFORM 264
Ar+H^OREVIEWDC UNIFORM 244
264DC NONUNIFORM 244
264IMPULSE UNIFORM 244IMPULSE NONUNIFORM 244
XX
X XX
X XX
X XX X
21
PARTICLE SURFACE INTERFACE CORONAAr+HeEXPERIMENTALDC UNIFORM 80 X
Ar+HgREVIEWDC UNIFORM 264 XDC NONUNIFORM 264 X
Ar+Hg+NeEXPERIMENTALDC UNIFORM 345 X
Ar+KEXPERIMENTALDC UNIFORM 127
Ar+N„EXPERIMENTALDC NONUNIFORM 107 X
REVIEWDC UNIFORM 264 XDC NONUNIFORM 264 X
Ar+N +SF^EXPERIMENTALDC UNIFORM 82
Ar+NaEXPERIMENTALDC UNIFORM 127
Ar+NeEXPERIMENTALDC UNIFORM 77
345DC NONUNIFORM 107
REVIEWDC UNIFORM 45
66244280
DC NONUNIFORM 4566
244AC UNIFORM 45
66AC NONUNIFORM 45
66IMPULSE UNIFORM 45
244IMPULSE NONUNIFORM 45
244
XX XX XX X
XX XX X
XX X
XX X
XX X
XX X
22
PARTICLE SURFACE INTERFACE CORONAAr+OpEXPERIMENTALDC NONUNIFORM 107
REVIEWDC UNIFORM 264DC NONUNIFORM 264
XX
Ar+SF,EXPERIMENTALDC UNIFORM 82
BCl^REVIEWDC UNIFORM
DC NONUNIFORM
AC UNIFORM
AC NONUNIFORM
IMPULSE UNIFORM
IMPULSE NONUNIFORM
4528543845
28545
28545
28545
28545
285
X
X
X
X
X
XX
XXXXXXXXXX
BF^EXPERIMENTALDC UNIFORM 110DC NONUNIFORM 283
REVIEWDC UNIFORM 45
438DC NONUNIFORM 45AC UNIFORM 45AC NONUNIFORM 45IMPULSE UNIFORM 45IMPULSE NONUNIFORM 45
EXPERIMENTALDC UNIFORM 367
373THEORETICALDC UNIFORM
C FiSpJlSlMENTALDC UNIFORM
373
315
XXXXX
ExifiR^^ENTALDC UNIFORM 301
23
C F
iip^filMENTALDC UNIFORM
PARTICLE SURFACE INTERFACE CORONA
315
EXPERIMENTALAC UNIFORM 33
70AC NONUNIFORM 33
70IMPULSE UNIFORM 33
70IMPULSE NONUNIFORM 33
70REVIEWDC UNIFORM 32
45438
DC NONUNIFORM 45AC UNIFORM 45
70AC NONUNIFORM 45
70IMPULSE UNIFORM 45
70IMPULSE NONUNIFORM 45
70
Mp^^imentalAC UNIFORM 70AC NONUNIFORM 70IMPULSE UNIFORM 70IMPULSE NONUNIFORM
REVIEW70
DC UNIFORM 45150438
DC NONUNIFORM 45150
AC UNIFORM 4570
150AC NONUNIFORM 45
70150
IMPULSE UNIFORM 4570
150IMPULSE NONUNIFORM 45
70150
X
X
X
X
XXXXXXXXX
XXXX
XX
XX
XX
XX
24
PARTICLE SURFACE INTERFACE CORONAC CI F^xp^rImentalDC UNIFORM 114
203DC NONUNIFORM 114AC UNIFORM 392IMPULSE UNIFORM 139
REVIEWDC UNIFORM 45
73203258285437438
DC NONUNIFORM 4573
258285
AC UNIFORM 4573
285AC NONUNIFORM 45
73285
IMPULSE UNIFORM 4573
258285
IMPULSE NONUNIFORM 4573
258285
X
X
XX
XX
X
X
X
X
XX
XXX
XX
XX
XXX
XX
CjCl^F-EXPERIMENTALDC UNIFORM 114
156DC NONUNIFORM 114
155THEORETICALDC UNIFORM 156
REVIEWDC UNIFORM 45
DC NONUNIFORM
731502582854384573
150258285
X
X
XX
X
XX
25
PARTICLE SURFACE INTERFACE CORONAC^Cl^F. (cont.)
AC UNIFORM 45 X73 X
150285 X X X
AC NONUNIFORM 4573
150X
X
285 X X XIMPULSE UNIFORM 45
73150258
XX
X285 X X X
IMPULSE NONUNIFORM 4573
150258
XX
X285 X X X
l,lrl-C,Cl^F^REVIEW ^ ^
DC UNIFORM 64
1,1,2-C5C1^F^REVIEWDC UNIFORM 64
C^Cl^F^+SF,experimentaldc uniform 156
theoreticaldc uniform 156
SevIe^dc uniform 73 xdc nonuniform 73 xac uniform 73 xac nonuniform 73 ximpulse uniform 73 ximpulse nonuniform 73 x
CjClFEXPERIMENTALDC UNIFORM 114DC NONUNIFORM 114
REVIEWDC UNIFORM 64
73253
DC NONUNIFORM 73AC UNIFORM 73AC NONUNIFORM 73
XXX
26
C^CIF-. (cont. )
IMPULSE UNIFORM 73IMPULSE NONUNIFORM 73
PARTICLE SURFACE INTERFACE CORONA
XX
C^CIFEXPERIMENTALDC UNIFORM 114DC NONUNIFORM 114AC UNIFORM 392REVIEWDC UNIFORM 45
73150253437438
DC NONUNIFORM 4573
150AC UNIFORM 45
73150
AC NONUNIFORM 4573
150IMPULSE UNIFORM 45
73150
IMPULSE NONUNIFORM 4573
150
C^CIF^REVIEWDC UNIFORM 258DC NONUNIFORM 258IMPULSE UNIFORM 258IMPULSE NONUNIFORM 258
XXXX
Ie^iewDC UNIFORM 253
C^F-NEXPERIMENTALDC UNIFORM 114DC NONUNIFORM 114
REVIEWDC UNIFORM 45
150280435436437
27
PARTICLE; SURFACE INTERFACE CORONAC^F-N (cont.
)
438^D^ NONUNIFORM 45
150X
AC UNIFORM 45150
X
AC NONUNIFORM 45150
X
IMPULSE UNIFORM 45150
X
IMPULSE NONUNIFORM 45150
X
C F^xIerimentalDC UNIFORM 55
63114310
DC NONUNIFORM 114AC UNIFORM 33
72 X392457
AC NONUNIFORM 3372 X
457' i-
.;s .; 460IMPULSE UNIFORM 33
72 XIMPULSE NONUNIFORM 33
72 XTHEORETICALDC UNIFORM 55
REVIEWDC UNIFORM 45 X
DC
AC
AC
UNIFORM 456473
150253258435436437438
NONUNIFORM 4573
150258
UNIFORM 4573
150NONUNIFORM 45
73150
XX
28
PARTICLE SURFACE INTERFACE CORONACpF, (cont.
)
IHPULSE UNIFORM 4573 X
150258 X
IMPULSE NONUNIFORM 45 X73 X
150258 X
C^F OREVIEWDC UNIFORM 253
C^F,SREVIEWdc uniform 253
Experimentaldc uniform 198
201202
DC NONUNIFORM 169THEORETICALDC UNIFORM 342
343REVIEWDC UNIFORM 64
253258 X437438
DC NONUNIFORM 2 58 XIMPULSE UNIFORM 258 XIMPULSE NONUNIFORM 258 X
1,1,1-C^H F^+2-C4F.EXPERIMENTALDC UNIFORM 83
1,1,1-C^H F-+2-C.F3EXPERIMENTALDC UNIFORM 85DC NONUNIFORM 8 5
THEORETICALDC UNIFORM 317
1,1,1-CtH,F,+SF^EXPERIMENTALDC UNIFORM 83
85DC NONUNIFORM 8 5
29
1,1,1-C2H3F3"^SF (cont.)THEORETICALDC UNIFORM 317
PARTICLE SURFACE INTERFACE CORONA
CpH-.NEXPERIMENTALDC UNIFORM 83REVIEWDC UNIFORM 64
C^H^N+SF^EXPERIMEl^TALDC UNIFORM 83
CpH.EXPERIMENTALDC UNIFORM 104
198200201202
DC NONUNIFORM 104REVIEWDC UNIFORM 45
258280
DC NONUNIFORM 45258
AC UNIFORM 45AC NONUNIFORM 45IMPULSE UNIFORM 45
258IMPULSE NONUNIFORM 45
258
XX
XXXXXXXX
C^H.+KrEXPERIMENTALDC UNIFORM 200
REVIEWDC UNIFORM 45DC NONUNIFORM 45AC UNIFORM 45AC NONUNIFORM 45IMPULSE UNIFORM 45IMPULSE NONUNIFORM 45
C H CIREVIEWDC UNIFORM 285DC NONUNIFORM 285AC UNIFORM 285AC NONUNIFORM 285IMPULSE UNIFORM 285IMPULSE NONUNIFORM 285
XXXXXX
XXXXXX
XXXXXX
XXXXXX
30
1,1-C2H CIREVIEWDC UNIFORM
PARTICLE SURFACE INTERFACE CORONA
64
C H OREVIEWDC UNIFORM 437
438
CpH^BrREVIEWDC UNIFORMDC NONUNIFORMAC UNIFORMAC NONUNIFORMIMPULSE UNIFORMIMPULSE NONUNIFORM
C2H CIREVIEWDC UNIFORM
DC NONUNIFORM
AC UNIFORM
AC NONUNIFORM
IMPULSE UNIFORM
IMPULSE NONUNIFORM
REVIEWDCDCACAC
UNIFORMNONUNIFORMUNIFORMNONUNIFORM
IMPULSE UNIFORMIMPULSE NONUNIFORM
285285285285285285
4528543743845
28545
28545
28545
28545
285
285285285285285285
XXXXXX
X
X
X
X
X
XXXXXX
XXXXXX
X
X
X
X
X
XXXXXX
XXXXXX
XX
XXXXXXXXXX
XXXXXX
CjHgEXPERIMENTALDC UNIFORM
DC NONUNIFORM
114115197201202114115
31
n-C^HREVIEWDC UNIFORM 258DC NONUNIFORM 258IMPULSE UNIFORM
C FExperimental
258impulse nonuniform 258
C^H NREVIEWDC UNIFORM 437
438
CpN^EXPERIMENTALDC NONUNIFORM 283
EXPERIMENTALDC UNIFORM 114DC NONUNIFORM 114
REVIEWDC UNIFORM 45
150280435436437438
DC NONUNIFORM 45150
AC UNIFORM 45150
AC NONUNIFORM 45150
IMPULSE UNIFORM 45150
IMPULSE NONUNIFORM 45150
DC UNIFORM 21REVIEWDC UNIFORM 64
150253
DC NONUNIFORM 150AC UNIFORM 150AC NONUNIFORM 150IMPULSE UNIFORM 150IMPULSE NONUNIFORM 150
PARTICLE SURFACE INTERFACE CORONA
XX
X
X
X
X
X
32
PARTICLE SURFACE INTERFACE CORONAC-C^FgREVIEWDC UNIFORM 253
C^F^+SF^THEORETICALDC UNIFORM 78
C-jF^+SOpTHEORETICALDC UNIFORM 78
C.FgOEXPERIMENTALDC UNIFORM 114DC NONUNIFORM 114
C FExperimentaldc uniform 81
114304310
DC NONUNIFORM 114AC UNIFORM 33
70 X72 X
457AC NONUNIFORM 33
70 X72 X
457460
IMPULSE UNIFORM 3370 X72 X
IMPULSE NONUNIFORM 3370 X72 X
452THEORETICALDC UNIFORM 65
103165
DC NONUNIFORM 103REVIEWDC UNIFORM 32
45 X646573 X
150165253
33
PARTICLE SURFACE INTERFACE CORONAC^Fg (cont.) 258 X
436437438
DC NONUNIFORM 45 X73 X
150258 X
AC UNIFORM 45 X70 X73 X
150AC NONUNIFORM 45 X
70 X73 X
150IMPULSE UNIFORM 45 X
70 X73 X
150258 X
IMPULSE NONUNIFORM 45 X70 X73 X
150258 X
c—C FEXPERIMENTALDC UNIFORM 331DC NONUNIFORM 331
REVIEWDC UNIFORM 331DC NONUNIFORM 331
C^F +C.F,+N„+SF^THEORfiTlCAEDC UNIFORM 65
REVIEWDC UNIFORM 65
C^Fg+CO^THEORETICALDC
REVIEWDC
UNIFORM
UNIFORM
C.F +C0THEORETDC
REVIEWDC
+N2ICALUNIFORM
UNIFORM
65
65
65
65
34
C-.F^+NTHEORETICAL
PARTICLE SURFACE INTERFACE CORONA
DC UNIFORM 65REVIEWDC UNIFORM 65
C^Fp+N^+SF^THEORETICALDC
REVIEWDC
UNIFORM
UNIFORM
65
65
C F NREVIEWDC UNIFORM 253
C ^H ^F ^REVIEWDC UNIFORM 64
C-.H^IREVIEWDCDCACAC
UNIFORM 285NONUNIFORM 285UNIFORM 285NONUNIFORM 285
IMPULSE UNIFORM 285IMPULSE NONUNIFORM 285
XXXXXX
XXXXXX
XXXXXX
ReviewDC UNIFORM 253
EXPERIMENTALDC UNIFORM 104
195200201202
DC NONUNIFORM 104EVIEWDC UNIFORM 45
253258
DC NONUNIFORM 45258
AC UNIFORM 45AC NONUNIFORM 45IMPULSE UNIFORM 45
258IMPULSE NONUNIFORM 45
258
XXXXXXXXX
35
PARTICLE SURFACE INTERFACE CORONAC-C-.HEXPERIMENTALDC UNIFORM 104DC NONUNIFORM 104
REVIEWDC UNIFORM 253
C-jH^+KrEXPERIMENTALDC UNIFORM 200
REVIEWDC UNIFORM 45DC NONUNIFORM 45AC UNIFORM 45AC NONUNIFORM 45IMPULSE UNIFORM 45IMPULSE NONUNIFORM 45
C^H^ClREVIEWDC UNIFORM 285DC NONUNIFORM 285AC UNIFORM 285AC NONUNIFORM 285IMPULSE UNIFORMIMPULSE NONUNIFORM
XXXXXX
XXXXXX
XXXXXX
XXXXXX
C H
EXPERIMENTALDC UNIFORM 114
115196201202
DC NONUNIFORM 114115
n-C-.HREVIEWDC UNIFORM 258DC NONUNIFORM 258IMPULSE UNIFORM 258IMPULSE NONUNIFORM 258
XXXX
C F
ixi^RIMENTALDC UNIFORM 114
310366
DC NONUNIFORM 114AC UNIFORM 33
72457
AC NONUNIFORM 33
36
PARTICLE SURFACE INTERFACE CORONA^4^10 (cont.) 72
457460
IMPULSE UNIFORM 3372
IMPULSE NONUNIFORM 3372
REVIEWDC UNIFORM 45
73150258436437438
DC NONUNIFORM 4573
150258
AC UNIFORM 4573
150AC NONUNIFORM 45
73150
IMPULSE UNIFORM 4573
150258
IMPULSE NONUNIFORM 4573
150258
^eWewDC UNIFORM 73DC NONUNIFORM 73AC UNIFORM 73AC NONUNIFORM 73
X
X
X
XX
XX
C.F,Q+N2EXPERIWENTALAC UNIFORM 72 XAC NONUNIFORM 72 XIMPULSE UNIFORM 72 XIMPULSE NONUNIFORM 72 X
"-C.F +NEXPERIMENTALAC UNIFORM 47 XAC NONUNIFORM 47 XIMPULSE UNIFORM 47 XIMPULSE NONUNIFORM 47 X
XXXX
37
C.F,^0 (cont.
)
IMPULSE UNIFORM 73IMPULSE NONUNIFORM 73
PARTICLE SURFACE INTERFACE CORONA
XX
C Fix?ERIMENTALDC UNIFORM 114DC NONUNIFORM 114
Ae^iewDC UNIFORM 438
C FSxIerimentalDC UNIFORM 114
330DC NONUNIFORM 114
THEORETICALDC
.UNIFORM 65
165167
REVIEWDC UNIFORM 45
6465
150165253270438
DC NONUNIFORM 45150270
AC UNIFORM 45150
AC NONUNIFORM 45150
IMPULSE UNIFORM 45150270
IMPULSE NONUNIFORM 45150270
x
x
x
X
1,3-C.F^EXPERIMENTALDC UNIFORM 331DC NONUNIFORM 331
REVIEWDC UNIFORM 331DC NONUNIFORM 331
38
PARTICLE SURFACE INTERFACE CORONA2-C4F,EXPERIMENTALDC UNIFORM 331DC NONUNIFORM 331
REVIEWDC UNIFORM 331DC NONUNIFORM 331
c-C FEXPERIMENTALDC UNIFORM 331DC NONUNIFORM 331
REVIEWDC UNIFORM 270
331X
DC NONUNIFORM 270331
X
IMPULSE UNIFORM 270 XIMPULSE NONUNIFORM 270 X
2-C.F^+CH^F^EXPERIMENTALDC UNIFORM 8 3
2-C.F^+CHF^EXPERIMENTALDC UNIFORM 83
C.F^+CO^thBoreticalDC UNIFORM 65
REVIEWDC UNIFORM 65
C>F^+CO^+NTHEORETICALDC UNIFORM 65
REVIEWDC UNIFORM 65
C.F^+NTHEORETICALDC UNIFORM 65
REVIEWDC UNIFORM 65
C.Fg+N +SF^EXPERIMENTALDC UNIFORM 330
THEORETICALDC UNIFORM 65REVIEWDC UNIFORM 65
X
X
XX
39
PARTICLE SURFACE INTERFACE CORONA
THEORETICALDC
REVIEWDC
C.F-N
UNIFORM
UNIFORM
EXPERIMENTALDC UNIFORMDC NONUNIFORMREVIEWDC UNIFORM
DC NONUNIFORM
AC UNIFORM
AC NONUNIFORM
IMPULSE UNIFORM
IMPULSE NONUNIFORM
C FixIfiRIMENTAL
65167
65
114114
4515043543643743845
15045
15045
15045
15045
150
DC UNIFORM 330AC UNIFORM 72
392AC NONUNIFORM 72IMPULSE UNIFORM 72IMPULSE NONUNIFORM 72
REVIEWDC UNIFORM 45
150270436437438
DC NONUNIFORM 45150270
AC UNIFORM 45150
AC NONUNIFORM 45150
IMPULSE UNIFORM 45150
X
X
X
X
X
XXX
X
X
X
40
PARTICLE SURFACE INTERFACE CORONAC.Fp (cont.) 270 X X
IRPULSE NONUNIFORM 45 X150270 X X
2-C FexIeSimentalDC UNIFORM 331DC NONUNIFORM 331
REVIEWDC UNIFORM 331DC NONUNIFORM 331
C-C FEXPERIMENTALDC UNIFORM 83
114311330331
DC NONUNIFORM 114331
AC UNIFORM 47AC NONUNIFORM 47IMPULSE UNIFORM 47
139IMPULSE NONUNIFORM 47
THEORETICALDC UNIFORM 65
165167
REVIEWDC UNIFORM 64
65150165253258270331
DC NONUNIFORM 150258270331
AC UNIFORM 150AC NONUNIFORM 150IMPULSE UNIFORM 150
258270
IMPULSE NONUNIFORM 150258270
XXX
X
41
PARTICLE SURFACE INTERFACE CORONAiso-C.F^EXPERIMENTALDC UNIFORM 311
REVIEWDC UNIFORM 150DC NONUNIFORM 150AC UNIFORM 150AC NONUNIFORM 150IMPULSE UNIFORM 150IMPULSE NONUNIFORM 150
C-C.F +1,1,1-C^H F
EXPERIMENTALDC UNIFORM 83
85DC NONUNIFORM 85
THEORETICALDC UNIFORM 317
C-C^Fj^ + l-C^F.EXPERIMENTALDC UNIFORM 83
C-C.Fo+C^H^NEXPERIMENTALDC UNIFORM 83
C-C.Fj.+C.F,+N2+SFEXPERIMENTALDC UNIFORM 330
C-C F +CFEXPERIMENTALDC UNIFORM 83
THEORETICALDC UNIFORM 317
2-C.F +CHFEXPERIMENTALDC UNIFORM 85DC NONUNIFORM 85
C-C.F +CHF^EXPERIMENTALDC UNIFORM 83
85DC NONUNIFORM 8 5
THEORETICALDC UNIFORM 317
C-C.Fo+COEXPERIMENTALAC NONUNIFORM 363IMPULSE NONUNIFORM 363
42
PARTICLE SURFACE INTERFACE CORONAC-C.Fo+CO+SF^EXPERIMENTALAC NONUNIFORM 363IMPULSE NONUNIFORM 363
C-C.Fq+CO^THEORETICALDC UNIFORM 65
REVIEWDC UNIFORM 65
C-C.F^+COj+N^THEORETICALDC UNIFORM 65EVIEWDC UNIFORM 65
2-c F +NexIeSim^ntaldc uniform 85dc nonuniform 85
theoreticaldc uniform 317
C-C.Fj.+N^EXPERIMENTALDC UNIFORM 85DC NONUNIFORM 8 5
AC UNIFORM 47 XAC NONUNIFORM 47 XIMPULSE UNIFORM 47 XIMPULSE NONUNIFORM 47 X
THEORETICALDC UNIFORM 65
317REVIEWDC UNIFORM 65
C-C.Fo+N^+SF^EXPERIMENTALAC NONUNIFORM 363IMPULSE NONUNIFORM 363
C.FSe^iew^DC UNIFORM 150DC NONUNIFORM 150AC UNIFORM 150AC NONUNIFORM 150IMPULSE UNIFORM 150IMPULSE NONUNIFORM 150
43
PARTICLE SURFACE INTERFACE CORONA^-C.F +SFTHEORETICALDC UNIFORM 167
C-C F OREVIEWdc uniform 73 xdc nonuniform 73 xac uniform 73 xac nonuniform 73 ximpulse uniform 73 ximpulse nonuniform 73 x
^xJ>8rimentaldc uniform 115dc nonuniform 115
ExIsfefMENTALdc uniform 115dc nonuniform 115
expeJiASntalDC UNIFORM 201
202
EX^EiiMENTALDC UNIFORM 201
202REVIEWDC UNIFORM 258DC NONUNIFORM 258IMPULSE UNIFORM 258IMPULSE NONUNIFORM 258
ixt^RIMENTALdc uniform 372
Experimentaldc uniform 195
xxxX
C-H,REVIEWDC UNIFORM 258 XDC NONUNIFORM 258 XIMPULSE UNIFORM 258 XIMPULSE NONUNIFORM 258 X
44
1,3-C HEXPERIMENTALDC UNIFORM
DC
104195201202
NONUNIFORM 104
PARTICLE SURFACE INTERFACE CORONA
ix?ERIMENTALDC UNIFORM 104
199DC NONUNIFORM 104
REVIEWDC UNIFORM 258DC NONUNIFORM 258IMPULSE UNIFORM 258IMPULSE NONUNIFORM 258
XXXX
EXPERIMENTALDC
DC
UNIFORM
NONUNIFORM
104195201202104
ex^eIimentaldc uniformdc nonuniform
104104
cis-C -HoEXPERIMENTALDC UNIFORM 195
iso-C ,HoEXPERIMENTALDC UNIFORM 195
trans-C .H„EXPERIMENTALDC UNIFORM 195
C.H CIREVIEWDC UNIFORM 285DC NONUNIFORM 285AC UNIFORM 28 5
AC NONUNIFORM 285IMPULSE UNIFORM 285IMPULSE NONUNIFORM 285
XXXXXX
XXXXXX
XXXXXX
45
PARTICLE SURFACE INTERFACE CORONA
5e^9ewDC UNIFORM 45
438DC NONUNIFORM 45AC UNIFORM 45AC NONUNIFORM 45IMPULSE UNIFORM 45IMPULSE NONUNIFORM 45
EXPERIMENTALDC UNIFORM 114
315DC NONUNIFORM 114AC UNIFORM 33
457AC NONUNIFORM 33
457460
IMPULSE UNIFORM 33IMPULSE NONUNIFORM 33
REVIEWDC UNIFORM 45
73150258438
DC NONUNIFORM 4573
150258
AC UNIFORM 4573
150AC NONUNIFORM 45
73150
IMPULSE UNIFORM 4573
150258
IMPULSE NONUNIFORM 4573
150258
C.FqREVIEWDC UNIFORM 45
270435436437
XXXXX
X
X
XX
XX
X
46
C F (cont .
)
NONUNIFORM
ACACIMPULSE
UNIFORMNONUNIFORMUNIFORM
IMPULSE NONUNIFORM
43845
270454545
27045
270
PARTICLE SURFACE INTERFACE CORONA
X
XXX
X
C-C F
EXPERIMENTALDC UNIFORM 331DC NONUNIFORM 331
REVIEWDC UNIFORM 331DC NONUNIFORM 331
C-CcFp+CHF^EXPERIMENTALDCDC
UNIFORM 85NONUNIFORM 85
Q-C F +NexIeSim^ntaldc uniformdc nonuniform
8585
exIe^Jmentaldc uniformdc nonuniform
104104
exIeJIPmentaldc uniform 195
exIeJSmentalDC UNIFORM 115
202DC NONUNIFORM 115
reviewDC UNIFORM 285DC NONUNIFORM 285AC UNIFORM 285AC NONUNIFORM 285IMPULSE UNIFORM 285IMPULSE NONUNIFORM 285
XXXXXX
XXXXXX
XXXXXX
47
PARTICLE SURFACE INTERFACE CORONA
EXPERIMENTALDC UNIFORM 114
115202
DC NONUNIFORM 114115
exIeJJmentaldc uniform 115dc nonuniform 115
2 f 2""C J.H , ^
experimentaldc uniform 115dc nonuniform 115
exIeJi?mentaldc uniform 198
202301
C.H^EXPERIMENTALDC UNIFORM 195
C-C HEXPERIMENTALDC UNIFORM 195
Se^SewDC UNIFORM 270 X XDC NONUNIFORM 270 X XIMPULSE UNIFORM 270 X XIMPULSE NONUNIFORM 270 X X
C-C FexIe^SmentalDC UNIFORM 331DC NONUNIFORM 331
REVIEWDC UNIFORM 331DC NONUNIFORM 331
c-CgF +CHFEXPERIMENTALDC UNIFORM 85DC NONUNIFORM 85
48
PARTICLE SURFACE INTERFACE CORONAC-C^F,^+N^EXPERIMENTALDC UNIFORM 85DC NONUNIFORM 85
6e^?ewDC UNIFORM 150
270 X XDC NONUNIFORM 150
270 X XAC UNIFORM 150AC NONUNIFORM 150IMPULSE UNIFORM 150
270 X XIMPULSE NONUNIFORM 150
270 X X
c-C FexIe^ImentalDC UNIFORM 331DC NONUNIFORM 331
REVIEWDC UNIFORM 64
331DC NONUNIFORM 331
C^F. .
EXPERIMENTALDC UNIFORM 114
315DC NONUNIFORM 114
REVIEWDC UNIFORM 45
150258438
DC NONUNIFORM 45150258
AC UNIFORM 45150
AC NONUNIFORM 45150
IMPULSE UNIFORM 45150258
IMPULSE NONUNIFORM 45150
- 258
X
X
X
XX
X
X
XX
C F NixJ§RIMENTALAC UNIFORM 33
49
PARTICLE SURFACE INTERFACE CORONAC^F,^N (C(Dnt. ) 70
NONUNIFORM 3370
IMPULSE UNIFORM 3370
IMPULSE NONUNIFORM 3370
REVIEWDC UNIFORM 45
438DC NONUNIFORM 45AC UNIFORM 45
70AC NONUNIFORM 45
70IMPULSE UNIFORM 45
70IMPULSE NONUNIFORM 45
70
1-C.HEXPERIMENTALDC UNIFORM 104
202DC NONUNIFORM 104
C-CgHEXPERIMENTALDC UNIFORM 115
202DC NONUNIFORM 115
IxJiRIMENTALDC UNIFORM 114
115DC NONUNIFORM 114
115
EXPE^lAiNTALDC UNIFORM 115DC NONUNIFORM 115
n-C^H, .
EXPERIMENTALDC UNIFORM 202
301IMPULSE UNIFORM 398
C^H CIREVIEWDC UNIFORM 45
438
XXXXXXXXX
50
C^H^Cl (cont.)DC NONUNIFORM 45AC UNIFORM 45AC NONUNIFORM 45IMPULSE UNIFORM 45IMPULSE NONUNIFORM 45
PARTICLE SURFACE INTERFACE CORONA
XXXXX
EXPERIMENTALDC UNIFORM 104
199DC NONUNIFORM 104
REVIEWDC UNIFORM 280
C^Cl^F^REVIEWDC UNIFORM 45
438DC NONUNIFORM 45AC UNIFORM -4-5
AC NONUNIFORM 45IMPULSE UNIFORM 45IMPULSE NONUNIFORM 45
XXXXX
?EV?E§DC UNIFORM
DC NONUNIFORMAC UNIFORMAC NONUNIFORMIMPULSE UNIFORMIMPULSE NONUNIFORM
454384545454545
XXXXX
C-C^Cl^FcEXPERIMENTALAC NONUNIFORM 460
C^CIF-REVIEWDC UNIFORM
DC NONUNIFORMAC UNIFORMAC NONUNIFORMIMPULSE UNIFORMIMPULSE NONUNIFORM
454384545454545
XXXXX
C-C^C1F_EXPERIMENTALAC NONUNIFORM 460
51
C F
2e^?ewDC UNIFORM 438
PARTICLE SURFACE INTERFACE CORONA
C F2xJ>iRIMENTALDC UNIFORM 315AC UNIFORM 70AC NONUNIFORM 70IMPULSE UNIFORM 70IMPULSE NONUNIFORM 70
REVIEWDC UNIFORM 45
150270438
DC NONUNIFORM 45150270
AC UNIFORM 4570
150AC NONUNIFORM 45
70150
IMPULSE UNIFORM 4570
150270
IMPULSE NONUNIFORM 4570
150270
EX?ERfMENTALAC UNIFORM 33AC NONUNIFORM 33
460IMPULSE UNIFORM 33IMPULSE NONUNIFORM 33
XXXX
XX
XX
XX
XX
EX?EifME^TALAC UNIFORM 33AC NONUNIFORM 33IMPULSE UNIFORM 33IMPULSE NONUNIFORM 33
C-C_F, 4+SFgEXPERIMENTALAC UNIFORM 33AC NONUNIFORM 33IMPULSE UNIFORM 33
52
C-C-F, A+SFf.IMPOLSE NONUNIFORM 33
PARTICLE SURFACE INTERFACE CORONA
C F2xJ>6rimentalAC UNIFORM 33
70AC NONUNIFORM 33
70IMPULSE UNIFORM 33
70IMPULSE NONUNIFORM 33
70REVIEWDC UNIFORM 45
150438
DC NONUNIFORM 45150
AC UNIFORM 4570
150AC NONUNIFORM 45
70150
IMPULSE UNIFORM 4570
150IMPULSE NONUNIFORM 45
70150
X
X
X
X
X
XX
XX
XX
XX
C F2xIerimentalDC UNIFORM 331DC NONUNIFORM 331AC UNIFORM 70AC NONUNIFORM 70IMPULSE UNIFORM 70IMPULSE NONUNIFORM 70
REVIEWDC UNIFORM 45
150270331438
DC NONUNIFORM 45150270331
AC UNIFORM 4570
150AC NONUNIFORM 45
X
XXXX
XX
X
53
PARTICLE SURFACE INTERFACE CORONAC^Fg (cont.) 70
150IMPULSE UNIFORM 45 X
70 X150270 X X
IMPULSE NONUNIFORM 45 X70 X
150
C-C FEXPERIMENTAL
270
AC UNIFORM 33AC NONUNIFORM 33
460IMPULSE UNIFORM 33IMPULSE NONUNIFORM 33
n-C^HEXPERIMENTALDC UNIFORM 301
C H CIFREVIEWDC UNIFORM 45DC NONUNIFORM 45AC UNIFORM 45AC NONUNIFORM 45IMPULSE UNIFORM 45IMPULSE NONUNIFORM 45
C H CIFREVIEWDC UNIFORM 45
438DC NONUNIFORM 45AC UNIFORM 45AC NONUNIFORM 45IMPULSE UNIFORM 45IMPULSE NONUNIFORM 45
C-C^H.CIF^EXPERIMENTALAC NONUNIFORM 460
C FixJ^RIMENTALDC UNIFORM 315
331DC NONUNIFORM 331AC UNIFORM 70AC NONUNIFORM 70IMPULSE UNIFORM 70
XXXXXX
XXXXX
XXX
54
PARTICLE SURFACE INTERFACE CORONA' F,, (cont.)IWPULSE NONUNIFORM
REVIEWDC UNIFORM
DC
AC
AC
NONUNIFORM
UNIFORM
NONUNIFORM
IMPULSE UNIFORM
IMPULSE NONUNIFORM
70
4515027033143845
1502703314570
1504570
1504570
1502704570
150270
X
XX
XX
XX
XX
C-C FEXpE^fMENTALAC UNIFORMAC NONUNIFORM
IMPULSE UNIFORMIMPULSE NONUNIFORM
3333
4603333
C F OixJ^RIMENTALDCDCREVIEWDCDCACAC
UNIFORMNONUNIFORM
UNIFORMNONUNIFORMUNIFORMNONUNIFORM
IMPULSE UNIFORMIMPULSE NONUNIFORM
397397
150150150150150150
c-C„F,gOREVIEWDC UNIFORM 32
Cj.F,^0+SF,EXPERIMENTALDC UNIFORM 397
55
S^jeO^SFg (cont.
)
NONUNIFORM
PARTICLE SURFACE INTERFACE CORONA
397
EXPERIMENTALAC UNIFORM 33
70AC NONUNIFORM 33
70IMPULSE UNIFORM 33
70IMPULSE NONUNIFORM 33
70REVIEWDC UNIFORM 45
438DC NONUNIFORM 45AC UNIFORM 45
70AC NONUNIFORM 45
70IMPULSE UNIFORM 45
70IMPULSE NONUNIFORM 45
70
n-CoH,
g
EXPERIMENTALDC UNIFORM 199
202301
X
X
XXXXXXXXX
C-CoH-.ClF^EXPERIMENTALAC NONUNIFORM 460
CBrClF^EXPERIMENTALDC UNIFORM 114
156DC NONUNIFORM 114
THEORETICALDC UNIFORM 65
156165167
REVIEWDC UNIFORM 64
65150165258438
DC NONUNIFORM 150
56
CBrClF (cont.)AC UNIFORM
258150
AC NONUNIFORM 150IMPULSE UNIFORM 150
258IMPULSE NONUNIFORM 150
258
CBrClF2+N2EXPERIMENTALDC UNIFORM 156
THEORETICALDC UNIFORM 65
156REVIEWDC UNIFORM 65
PARTICLE SURFACE INTERFACE CORONAX
X
CBrClF2+SFgEXPERIMENTALDC UNIFORM
THEORETICAL156
DC UNIFORM 65156167
EVIEWDC UNIFORM 65
CBrF^EXPERIMENTALDC UNIFORM 114DC NONUNIFORM 114
283AC UNIFORM 72AC NONUNIFORM 72IMPULSE UNIFORM 72IMPULSE NONUNIFORM 72
REVIEWDC UNIFORM 64
73150253258437438
DC NONUNIFORM 73150258
AC UNIFORM 73150
AC NONUNIFORM 73150
IMPULSE UNIFORM 73150258
XXXX
X
X
X
57
\
CBrF^ (cont.
)
IMPULSE NONUNIFORM
EXPERIMENTAL
PARTICLE SURFACE INTERFACE CORONA
73150258
DC UNIFORM 7688
114151203206303313373
DC NONUNIFORM 114141142206283313
AC UNIFORM 206313
AC NONUNIFORM 206313460
IMPULSE UNIFORM 139206313
IMPULSE NONUNIFORM 206313
THEORETICALDC UNIFORM 152
165167207373419
DC NONUNIFORM 207REVIEWDC UNIFORM 45
64738896
150165203253258280285368
X
X
X
X
X
XXX
X
X
XXX
XXXXX
XXXX
X
X
XX
XX
X
X
58
PARTICLE SURFACE INTERFACE CORONACCI2F2 (cont.
)
DC NONUNIFORM
AC UNIFORM
AC NONUNIFORM
IMPULSE UNIFORM
IMPULSE NONUNIFORM
435436437438457396
150258285457396
150285457396
150285457396
150258285457396
150258285
XX
XX
X
XX
XX
XX
X
X
X
X
XXX
XX
XX
XXX
XX
CCljF^+CFEXPERIMENTALDC UNIFORM 206DC NONUNIFORM 206AC UNIFORM 206AC NONUNIFORM 206IMPULSE UNIFORM 206IMPULSE NONUNIFORM 206
XXXXXX
XXXXXX
CClpFj+CO^THEORETICALDC UNIFORM 317
CCl^F^+NEXPERIMENTALDC UNIFORM 88
206276373402403
59
PARTICLE SURFACE INTERFACE CORONACl^P.^N, (cont. )
NONUNIFORM 142206
AC UNIFORM 206AC NONUNIFORM 206IMPULSE UNIFORM 206IMPULSE NONUNIFORM 206
THEORETICALDC UNIFORM 317
373419
REVIEWDC UNIFORM 88
XXXXX
XXXXXX
CCljF^+SFgEXPERIMENTALDC UNIFORM 206DC NONUNIFORM 206AC UNIFORM 206AC NONUNIFORM 206IMPULSE UNIFORM 206IMPULSE NONUNIFORM 206
THEORETICALDC UNIFORM 167
XXXXXX
XXXXXX
CCl^FEXPERIMENTALDC UNIFORM 88
114203206
DC NONUNIFORM 114206283
AC UNIFORM 206AC NONUNIFORM 206
460IMPULSE UNIFORM 206IMPULSE NONUNIFORM 206
REVIEWDC UNIFORM 45
647388
150203258285437438
DC NONUNIFORM 4573
150258
XX
X
X
XX
XX
X
X
XX
XX
XX
60
PARTICLE SURFACE INTERFACE CORONACCl^F (cont.) 285
Ad UNIFORM 4573
150285
AC NONUNIFORM 4573
150285
IMPULSE UNIFORM 4573
150258285
IMPULSE NONUNIFORM 4573
150258285
CCl.EXPERIMENTALDC UNIFORM 88
114203
DC NONUNIFORM 114AC NONUNIFORM 460THEORETICALDC UNIFORM 152
REVIEWDC UNIFORM 45
6488
203285436437438
DC NONUNIFORM 45285
AC UNIFORM 45285
AC NONUNIFORM 45285
IMPULSE UNIFORM 45285
IMPULSE NONUNIFORM 45285
CCIF^EXPERIMENTALDC UNIFORM
X
X
X
X
X
X
X
X
X
X
X
X
X
X
X
X
X
X
X
X
XX
XX
XX
XXX
XX
XXXXXXXXXX
88114203
61
PARTICLE SURFACE INTERFACE CORONACCIF^ (cont.)
DC NONUNIFORM206 X X38 X X
114206 X X283
AC UNIFORM 206 X XAC NONUNIFORM 206
460X X
IMPULSE UNIFORM 206 X XIMPULSE NONUNIFORM 206 X X
REVIEWDC UNIFORM 45
647388
150203253258436437438
XX
X
X
DC NONUNIFORM 4573
150258
XX
XAC UNIFORM 45
73150
XX
AC NONUNIFORM 4573
150X
X
IMPULSE UNIFORM 4573
150258
XX
XIMPULSE NONUNIFORM 45
73150258
XX
X
CCIF^+NEXPERIMENTALDC UNIFORM 88 XREVIEWDC UNIFORM 88 X
CDEXPERIMENTALDC UNIFORM 84DC NONUNIFORM 84
62
PARTICLE SURFACE INTERFACE CORONACF-IEXPERIMENTALDC NONUNIFORM 283
REVIEWDC UNIFORM 45
438DC NONUNIFORM 45AC UNIFORM 45AC NONUNIFORM 45IMPULSE UNIFORM 45IMPULSE NONUNIFORM 45
CF-jNOEXPERIMENTALDC UNIFORM 114DC NONUNIFORM 114
REVIEWDC UNIFORM 438
CF^NO^REVIEWDC UNIFORM 150
253DC NONUNIFORM 150AC UNIFORM 150AC NONUNIFORM 150IMPULSE UNIFORM 150IMPULSE NONUNIFORM 150
XXXXX
CFEXPERIMENTALDC UNIFORM
DC
AC
NONUNIFORM
UNIFORM
AC NONUNIFORM
IMPULSE UNIFORM
5563
114203206252310401114206283337072
206392337072
2064603370
X
X
XXX
XXX
63
CF. (cont.
)
IMPULSE NONUNIFORM
THEORETICALDC UNIFORM
DC NONUNIFORMREVIEWDC UNIFORM
DC
AC
AC
NONUNIFORM
UNIFORM
NONUNIFORM
IMPULSE UNIFORM
IMPULSE NONUNIFORM
72206337072
206
55207207
456473
2032532584364374384573
258457073457073457073
258457073
258
PARTICLE SURFACE INTERFACE CORONAX
X X
X
XXX
XX
XXX
XX
XX
XXX
CF.+SF^EXPERIMENTALDC UNIFORM 83
THEORETICALDC UNIFORM 317
CF.SO^REVIEWDC UNIFORM 253
CFcNSEXPERIMENTALDC UNIFORM 114DC NONUNIFORM 114
REVIEWDC UNIFORM 4 38
64
PARTICLE SURFACE INTERFACE CORONACFy.SEXPERIMENTALDC UNIFORM 1^4
151263
DC NONUNIFORM lUTHEORETICALDC UNIFORM 1,152
REVIEWDC UNIFORM 150
DC NONUNIFORM
AC UNIFORM
AC NONUNIFORM
IMPULSE UNIFORM
IMPULSE NONUNIFORM
CF^SOREVIEWDC UNIFORM
2032532g0 X X2B5 XXX438150285 XXX150285 XXX1^0285 XXX150285 XXX150285 XXX253
CH^Cl^;
EXPERIMENTAL >
DC UNIFORM 114DC NONUNIFORM 114AC NONUNIFORM 460REVIEWDC UNIFORM 45 X
64258 X285 XXX438
DC NONUNIFORM 45 X258 X285 XXX
AC UNIFORM 45 Xlis XXX
AC NONUNIFORM 45 X285 XXX
IMPULSE UNIFORM 45 , X258 X285 XXX
IMPULSE NONUNIFORM 45 X258 X285 X X X
65
PARTICLE SURFACE INTERFACE CORONACH^CIFEXPERIMENTALDC UNIFORM 88
114DC NONUNIFORM 114AC NONUNIFORM 460REVIEWDC UNIFORM 45
88258437438
DC NONUNIFORM 45258
AC UNIFORM 45AC NONUNIFORM 45IMPULSE UNIFORM 45
258IMPULSE NONUNIFORM 45
258
X
X
XXXXXXXX
CH^F«REVIEWDC UNIFORM 45
64258438
DC NONUNIFORM 45258
AC UNIFORM 45AC NONUNIFORM 45IMPULSE UNIFORM 45
258IMPULSE NONUNIFORM 45
258
CH^F^+SFgEXPERIMEl^TALDC UNIFORM 83
CH-BrEXPERIMENTALDC UNIFORM 114DC NONUNIFORM 114REVIEWDC UNIFORM 64
258285438
DC NONUNIFORM 258285
AC UNIFORM 285AC NONUNIFORM 285IMPULSE UNIFORM 258
XXX
XXX
X
X
XXXXXXXX
XX
XXXXX
66
CH Br (cont.
)
285IMPULSE NONUNIFORM 258
285
CH^ClEXPERIMENTALDC UNIFORM 88
114DG NONUNIFORM 114AC NONUNIFORM 460REVIEWDC UNIFORM 45
6488
258285438
DC NONUNIFORM 45258285
AC UNIFORM 45285
AC NONUNIFORM 45285
IMPULSE UNIFORM 45258285
IMPULSE NONUNIFORM 45258285
PARTICLE SURFACE INTERFACE CORONAXXXXXXX
X
X
X
X
X
X
X
X
X
X
XX
XXXXXXXXXXXXX
CH^FREVIEWDC UNIFORM 45DC NONUNIFORM 45AC UNIFORM 45AC NONUNIFORM 45IMPULSE UNIFORM 45IMPULSE NONUNIFORM 45
CH^IEXPERIMENTALDC UNIFORM 114DC NONUNIFORM 114
REVIEWDC UNIFORM 64
258285437438
DC NONUNIFORM 258285
AC UNIFORM 285AC NONUNIFORM 285
XXX
XXX
XXXXXX
XX
XXXX
67
PARTICLE SURFACE INTERFACE CORONACH^I (cont.)
IMPULSE UNIFORM 258285
IMPULSE NONUNIFORM 258285
CH.EXPERIMENTALDC UNIFORM 84
88114115196201202
DC NONUNIFORM 84114115169
AC NONUNIFORM 460REVIEWDC UNIFORM 45
6488
253285437438
DC NONUNIFORM 45285
AC UNIFORM 45285
AC NONUNIFORM 45285
IMPULSE UNIFORM 45285
IMPULSE NONUNIFORM 45285
n-CHREVIEWDC UNIFORM 258DC NONUNIFORM 258IMPULSE UNIFORM 258IMPULSE NONUNIFORM 258
CH NREVIEWDC UNIFORM 437
438
CHCI2FEXPERIMENTALDC UNIFORM 88
X
X
X
X
X
X
X
X
X
XXXX
XXXXXXXXXX
XXXX
68
PARTICLE SURFACE INTERFACE CORONACHCI2F (c<Dnt. ) 114
203206
DC NONUNIFORM 114206
AC UNIFORM 206AC NONUNIFORM 206
460IMPULSE UNIFORM 206IMPULSE NONUNIFORM 206
REVIEWDC UNIFORM 45
6488
150203258437438
DC NONUNIFORM 45150258
AC UNIFORM 45150
AC NONUNIFORM 45150
IMPULSE UNIFORM 45150258
IMPULSE NONUNIFORM 45150258
CHCl^EXPERIMENTALDC UNIFORM 88
114DC NONUNIFORM 114AC NONUNIFORM 460REVIEWDC UNIFORM 45
6488
150258285437
- 438DC NONUNIFORM 45
150258285
AC UNIFORM 45150
XXX
XX
X
X
XXX
XX
XX
X
X
XX
XX
XXX
69
CHC1-, (cont.) 285AC-^ NONUNIFORM 45
150285
IMPULSE UNIFORM 45150258285
IMPULSE NONUNIFORM 45150258285
CHClFpEXPERIMEIVITALDC UNIFORM 88
114206
DC NONUNIFORM 114206
AC UNIFORM 206AC NONUNIFORM 206
460IMPULSE UNIFORM 206IMPULSE NONUNIFORM 206
REVIEWDC UNIFORM 45
647388
150253258437438
DC NONUNIFORM 4573
150258
AC UNIFORM 4573
150AC NONUNIFORM 45
73150
IMPULSE UNIFORM 4573
150258
IMPULSE NONUNIFORM 4573
150258
PARTICLE SURFACE INTERFACE CORONAXXXX
XX
XXX
XX
XXX
XX
XX
XXX
XX
XX
XX
70
CHF,EXPERIMENTALDC
DC
ACACIMPULSEIMPULSE
REVIEWDC
UNIFORM
NONUNIFORM
UNIFORMNONUNIFORMUNIFORMNONUNIFORM
UNIFORM
DC
AC
AC
NONUNIFORM
UNIFORM
NONUNIFORM
IMPULSE UNIFORM
IMPULSE NONUNIFORM
CHF^+SF^EXPERIMENTALDC UNIFORM
DC NONUNIFORMTHEORETICALDC UNIFORM
COEXPERIMENTALDC UNIFORMDC NONUNIFORMAC NONUNIFORMIMPULSE NONUNIFORM
THEORETICALDC UNIFORM
PARTICLE SURFACE INTERFACE CORONA
88114206114206206206206206
45647388
1502584384573
150258
I
45I 731504573
^50I 45I 731502584573
150258
838585
317
112169363363
342
X
X XX XX XX XX X
XX
X
XX
X
XX
71
CO (cont.
)
REVIEWDC UNIFORM
DC NONUNIFORM
AC UNIFORM
AC NONUNIFORM
IMPULSE UNIFORM
IMPULSE NONUNIFORM
CO+SF^EXPERIMENTALAC NONUNIFORMIMPULSE NONUNIFORM
CO^EXPERIMENTALDC UNIFORM
DC NONUNIFORM
AC UNIFORM
AC NONUNIFORM
IMPULSE NONUNIFORM
THEORETICALDC UNIFORM
343
4564
28543743845
28545
28545
28545
28545
285
363363
408889
11127332635337338939010716932646232635132635125
382
6578
273342343373374
PARTICLE SURFACE INTERFACE CORONA
I
XXXXX
X
X
X
X
X
X
X
X
X
XXXXXXXXXX
72
PARTICLE SURFACE INTERFACE CORONACO^ (cont.)REVIEWDC UNIFORM 45
6465
X
66 X X88 X92 X X X96 X X X
119 X150244 X X253270 X X285 X X X334 X X368437438
DC NONUNIFORM 45 X66 X X96 X X X
150244 X X270 X X285 X X X334 X X
AC UNIFORM 45 X66 X X96 X X X
150285 X X X
AC NONUNIFORM 45 X66 X X96 X X X
150285 X X X
IMPULSE UNIFORM 45 X92 X X X96 X X X
150244 X X270 X X285 X X X
IMPULSE NONUNIFORM 45 X96 X X X
150244 X X270 X X285 X X X
CO,+He+N,EXPERIMENTALDC UNIFORM 111
73
PARTICLE SURFACE INTERFACE CORONACO^+N^EXPERIMEl^TALDC UNIFORM 88
REVIEWDC UNIFORM 88
96285
DC NONUNIFORM 96285
AC UNIFORM 96285
AC NONUNIFORM 96285
IMPULSE UNIFORM 96285
IMPULSE NONUNIFORM 96285
X
XXXXXXXXXXXXX
XXXXXXXXXXXX
X
CO^+N^+SFgTHEORETICALDC
REVIEWDC
UNIFORM
UNIFORM
65
65
CO^+NeEXPERIMENTALDC NONUNIFORM 107
CO,+SFgEXPERIMENTALDC UNIFORM 254
273DC NONUNIFORM 254
274AC UNIFORM 351AC NONUNIFORM 351IMPULSE NONUNIFORM 382
THEORETICALDC UNIFORM 273
316317
DC NONUNIFORM 316REVIEWDC UNIFORM 270 X XDC NONUNIFORM 270 X XIMPULSE UNIFORM 270 X XIMPULSE NONUNIFORM 270 X X
csREVIEWDC UNIFORM 285 XDC NONUNIFORM 285 XAC UNIFORM 285 XAC NONUNIFORM 285 X
XXXX
X
X
X
XXXX
74
PARTICLE SURFACE INTERFACE CORONACSp (cont.)
IMPULSE UNIFORM 285IMPULSE NONUNIFORM 285
XX
XX
XX
CSOREVIEWDC UNIFORM 64
253
^^2EXPERIMENTALDC UNIFORM
DC NONUNIFORMTHEORETICALDC UNIFORM
REVIEWDC UNIFORM
DC NONUNIFORMAC UNIFORMAC NONUNIFORMIMPULSE UNIFORMIMPULSE NONUNIFORM
62373283
373
285437438285285285285285
XXXXX
XXXXX
XXXXX
CI SREVIEWDC UNIFORM 437
438
CIF^SREVIEWDC UNIFORM 253
CIFO^EXPERIMENTALDC UNIFORM
REVIEWDC UNIFORM
DC NONUNIFORMAC UNIFORMAC NONUNIFORMIMPULSE UNIFORMIMPULSE NONUNIFORM
203
452034374384545454545
XXXXX
Cs+HeEXPERIMENTALDC UNIFORM 127
75
PARTICLE SURFACE INTERFACE CORONA
EXPERIMENTALDC UNIFORM 84DC NONUNIFORM 84
282
F^SOREVIEWDC UNIFORM 150
253285437438
DC NONUNIFORM 150285
AC UNIFORM 150285
AC NONUNIFORM 150285
IMPULSE UNIFORM 150285
IMPULSE NONUNIFORM 150285
F SOREVIEWDC
F^NSREVIEWDC
UNIFORM
UNIFORM
H.
EXPERIMENTALDC UNIFORM
DC NONUNIFORM
AC NONUNIFORM
253
253
4
5684
1081091481512622663083893905684
1692662822838799
X
X
X
X
X
X
X
X
X
X
X
X
X
X
X
XX
X
X
76
PARTICLE SURFACE INTERFACE CORONAH^ (cont. )
'^IMPULSE UNIFORM 148IMPULSE NONUNIFORM 135
136THEORETICALDC UNIFORM 163
190343374
DC NONUNIFORM 163REVIEWDC UNIFORM 45
646696
119148163244253260261264280285334435436437438
DC NONUNIFORM 456696
163244260264285334
AC UNIFORM 456696
285AC NONUNIFORM 45
6696
285IMPULSE UNIFORM 45
96- 148
244285
IMPULSE NONUNIFORM 4596
XXX
XX
XXX
XX
XX
XX
XXX
XXX
XX
XX
XX
XX
X
X
XX
XX
XXXXX
XXX
XX
XXX
77
H^ (cont .
)
PARTICLE SURFACE INTERFACE CORONA244 X X285 XXX
H^+HeEXPERIMENTALDC UNIFORM 77
H^+NeEXPERIMENTALDC UNIFORM 77
H +0REVIEWDCDC
UNIFORM 264NONUNIFORM 264
XX
H^+SF^EXPERIMENTALAC NONUNIFORMIMPULSE NONUNIFORM
99135136
XX
H^OEXPERIMENTALDC UNIFORM 171
172361
DC NONUNIFORM 162
H^SREVIEWDC UNIFORM 244
285DC NONUNIFORM 244
285AC UNIFORM 285AC NONUNIFORM 285IMPULSE UNIFORM 244
285IMPULSE NONUNIFORM 244
285
X XX X XX XX X XX X XX X XX XX X XX XX X X
HBrREVIEWDCDCACAC
UNIFORM 285NONUNIFORM 285UNIFORM 285NONUNIFORM 285
IMPULSE UNIFORM 285IMPULSE NONUNIFORM 285
XXXXXX
XXXXXX
XXXXXX
HClREVIEWDC UNIFORM 285
78
PARTICLE SURFACE INTERFACE CORONAHCl (cont,.)
DC NONUNIFORM 285AC UNIFORM 285AC NONUNIFORM 285IMPULSE UNIFORM 285IMPULSE NONUNIFORM 285
HIREVIEWDC UNIFORM 285DC NONUNIFORM 285AC UNIFORM 285AC NONUNIFORM 285IMPULSE UNIFORM 285IMPULSE NONUNIFORM 285
HeEXPERIMENTALDC UNIFORM
DC
AC
AC
NONUNIFORM
UNIFORM
NONUNIFORM
IMPULSE UNIFORM
IMPULSE NONUNIFORMTHEORETICALDC UNIFORMDC NONUNIFORMIMPULSE UNIFORMIMPULSE NONUNIFORM
REVIEWDC UNIFORM
4
8012515416424228432638939040045116417032632635187
13432635142351
13945652
1631635152
456692
119
XXXXX
XXXXXX
XX
XX
XXX
XXXXX
XXXXXX
XXXXX
XXXXXX
XX
79
He (cont.
)
163244253260264280285436437438
DC NONUNIFORM 4566
163244260264285
AC UNIFORM 4566
285AC NONUNIFORM 45
66285
IMPULSE UNIFORM 4592
244285
IMPULSE NONUNIFORM 45244285
He+KEXPERIMENTALDC UNIFORM 127
He+N^EXPERIMENTALAC UNIFORM 351AC NONUNIFORM 351
PARTICLE SURFACE INTERFACE CORONA
X X
X
XX
XX
XX
XX
XXX
XX
XX
X
X
XX
XXXXXXXXX
XXXXX
He+NeEXPERIMENTALDC UNIFORM 125
451
He+O^REVIEWDCDCACAC
UNIFORM 285NONUNIFORM 285UNIFORM 285NONUNIFORM 285
IMPULSE UNIFORM 285IMPULSE NONUNIFORM 285
XXXXXX
XXXXXX
XXXXXX
80
PARTICLE SURFACE INTERFACE CORONAHe+SF,EXPERIMEI^TALDC UNIFORM 400AC NONUNIFORM 87THEORETICALDC UNIFORM 78
236REVIEWDC UNIFORM 45DC NONUNIFORM 45AC UNIFORM 45AC NONUNIFORM 45IMPULSE UNIFORM 45IMPULSE NONUNIFORM 45
XXXXXX
HgEXPERIMENTALDC UNIFORM 4
390REVIEWDC UNIFORM 119
260334
DC NONUNIFORM 260334
Hg+NeEXPERIMENTALDC UNIFORM 344
K+NeEXPERIMENTALDC UNIFORM 127
KrEXPERIMENTALDC UNIFORM 200
389390
DC NONUNIFORM 170THEORETICALDC UNIFORM 163DC NONUNIFORM 163
REVIEWDC UNIFORM 45
66163260261285438
DC NONUNIFORM 4566
163
XXXXX
X
X
XXX
XX
X
XX
81
Kr (cont,
)
260285
AC UNIFORM 4566
285AC NONUNIFORM 45
66285
IMPULSE UNIFORM 45285
IMPULSE NONUNIFORM 45285
PARTICLE SURFACE INTERFACE CORONAXXXX
XX XXX X
XX XXXX
XXXXXXXX
N,
EXPERIMENTALDC
DC
UNIFORM 29435556718688
106114121138145148156161164201206218223225266273299308326330353377 X389390450
NONUNIFORM 343844567194 X95 X
XX
XX
82
PARTICLE SURFACE INTERFACE CORONAN^ (cont.) 107 X^
114141 X142 X164169206 X X266275283298 X309325326332 X377 X459 X
AC UNIFORM 3370 X71
130137 X206 X X326351377 X457
AC NONUNIFORM 3334 X4470 X7194 X95 X X
206 X X323 X325326336 X351363377 X453457459 X
IMPULSE UNIFORM 3343 X70 X71
137 X139148206 X X225
83
INTERFACE CORONAN.
PARTICLE SURFACE
2 (cont.
)
267 X X324 X356404 X
IMPULSE NONUNIFORM 33347071
206246324 X332355363380382404 X443453459461
THEORETICALDC UNIFORM 55
65103156163209217268271273342343352374377 X419
DC NONUNIFORM 103163271332377 X
AC UNIFORM 137 X377 X
AC NONUNIFORM 336 X377 X
IMPULSE UNIFORM 137297
X
324 XIMPULSE NONUNIFORM 324
332X
REVIEWDC UNIFORM 32
XX
XX
XX
XX
84
PARTICLE SURFACE INTERFACE CORONANj (cont.
)
DC NONUNIFORM
AC UNIFORM
AC NONUNIFORM
456465667173889296
1051191481501632092442532642702802853684354364374384566717396150163244264270285447456670717396
105150285456670717396
150
XX
XXXX
X
XXX
XX
XX
XX
X
X
XX
XX
XX
X
X
X
XX
XX
XXXXX
XXXX
85
N2 (cont.
)
IMPULSE UNIFORM
IMPULSE NONUNIFORM
28544745707173919296
1481502442702854570717396
150244270285447
PARTICLE SURFACE INTERFACE CORONAXXXXXX
XXX
XXXX
XXX
XX
XXX
XXX
XXX
XX
N +NeEXPERIMENTALDC NONUNIFORM 107
N^+Ne+SFgEXPERIMENTALDC UNIFORM 82
N2+02EXPERIMENTALDC NONUNIFORM 298
REVIEWDC UNIFORM 264
285435
DC NONUNIFORM 264285
AC UNIFORM 285AC NONUNIFORM 285IMPULSE UNIFORM 285IMPULSE NONUNIFORM 285
XXXXX
XXXXX
XX
XXXXXX
N, ,+SFixpeI
DCTMENTAL
UNIFORM 8588
161206
86
PARTICLE SURFACEN2+SFg (cont.) 218
273402403 -'
DC NONUNIFORM 4485
142206275
AC UNIFORM 130137 X206351
AC NONUNIFORM 44206351363
IMPULSE UNIFORM 137206
X
IMPULSE NONUNIFORM 132206246363376382443461
X
THEORETICALDC UNIFORM 65
78166217236271273316419454
DC NONUNIFORM 271316454
AC UNIFORM 137 XIMPULSE UNIFORM 137 XIMPULSE NONUNIFORM 132
376X
REVIEWDC UNIFORM 45
6588 X96150250
X X
251 X X270 X X
INTERFACE CORONA
XX
X
XX
XXX
X
87
PARTICLE SURFACE INTERFACE CORONAN^+SF^ (cont.)
DC NONUNIFORM 45 X96 X X X
150250 X251 X X X270 X X
AC UNIFORM 45 X96 X X X
150250 X251 X X X
AC NONUNIFORM 45 X96 X X X
150250 X251 X X X
IMPULSE UNIFORM 45 X96 X X X
150250 X270 X X
IMPULSE NONUNIFORM 45 X96 X X X
150250 X270 X X
N^OEXPERIMENTALDC UNIFORM 121
122DC NONUNIFORM 365
THEORETICALDC UNIFORM 166
342343
REVIEWDC UNIFORM 64
150244 X X253285 X X X438
DC NONUNIFORM 150244 X X285 X X X
AC UNIFORM 150285 X X X
AC NONUNIFORM 150285 X X X
IMPULSE UNIFORM 150244 X X285 X X X
88
N„0 (cont.)IMPULSE NONUNIFORM
PARTICLE SURFACE INTERFACE CORONA
150244285
XX
XX
N^O+0^EXPERIMENTALDC UNIFORM 123
N^O+SF^EXPERIMENTALDC UNIFORM 122
THEORETICALDC UNIFORM 166
316DC NONUNIFORM 316
REVIEWDC UNIFORM 270 XDC NONUNIFORM 270 XIMPULSE UNIFORM 270 XIMPULSE NONUNIFORM 270 X
NH^EXPERIMENTALDC UNIFORM 389
390REVIEWDC UNIFORM 285DC NONUNIFORM 285AC UNIFORM 285AC NONUNIFORM 285IMPULSE UNIFORM 285IMPULSE NONUNIFORM 285
NOREVIEWDC UNIFORM 66
285DC NONUNIFORM 66
285AC UNIFORM 66
285AC NONUNIFORM 66
285IMPULSE UNIFORM 285IMPULSE NONUNIFORM 285
NeEXPERIMENTALDC UNIFORM 82
125242300344
XXXX
XXXXXX
XXXXXXXXXX
XXXXXX
X
X
X
XXX
XX
XXXXXX
XXXXXXXXXX
X
89
Ne (cont. ) 389390451
DC NONUNIFORM 107149170
IMPULSE NONUNIFORM 149THEORETICALDC UNIFORM 163DC NONUNIFORM 163
REVIEWDC UNIFORM 45
6466
163260261264280285334435436437438
DC NONUNIFORM 4566
163260264285334
AC UNIFORM 4566
285AC NONUNIFORM 45
66285
IMPULSE UNIFORM 45285
IMPULSE NONUNIFORM 45285
Ne+0„EXPERIMENTALDC NONUNIFORM 107
Ne+SF^EXPERIMENTALDC UNIFORM
OExperimentaldc uniform
82
46
PARTICLE SURFACE INTERFACE CORONA
XXXX
XX
XXX
XX
X
X
XX
XX
XX
X
X
X
X
XX
XX
XXXXXXXXXXXXX
90
PARTICLE SURFACE INTERFACE CORONAOj (cont. ) 113
120143362389390442
DC NONUNIFORM 38107169298
IMPULSE UNIFORM 139THEORETICALDC UNIFORM 152
163343374442465
DC NONUNIFORM 163REVIEWDC UNIFORM 45
64163244253264285
DC NONUNIFORM 45163244264285
AC UNIFORM 45285
AC NONUNIFORM 45285
IMPULSE UNIFORM 45244285
IMPULSE NONUNIFORM 45244285
S^fiEXPERIMENTALDC UNIFORM 42
43535559607176
X
X
X
X
XX
XX X
XX
XX
X
XXX
XXXXXXXXXXXXX
91
SF, (cont.)
DC NONUNIFORM
79828388
1011141211221241281291531561611642032062182452542662732772782953133193263303493503543733773973994004024033034383944505354577190939495
114
PARTICLE SURFACE INTERFACE CORONAX
XX
XX
XX
XX
XX
92
PARTICLE SURFACE INTERFACE CORONASF^ (cont.)
AC UNIFORM
AC NONUNIFORM
1161181281291311411421491641882062452542662722742752832953023053133193263493773974074344591533364770717298
1301372062292953133193223263513773924244571516
XX
XX
XX
X
X
X
X
XXX
XXX
XX
XX
XXX
XX
XX
XX
93
PARTICLE SURFACE INTERFACE CORONASFg (cont.) 24
28 X K X3334 X39 X4447 X5068 X X70 X7172 X8794 X95 X X97 X X98 X X99 X
102 X133182 X X183 X206 X X214 X X228 X229 X230233239 X249 X294295 X X302 X305312 X X313 X319 X322 X326336 X351363377 X407 X424 X425 X X434 X457459
IMPULSE UNIFORM 153343 X47 X70 X
94
PARTICLE SURFACE INTERFACE CORONASFg (cont.) 71
72 X79 X
137 X139206 X X229 X245 X267 X X295 X X313 X320 X X324 X356404 X413424
IMPULSE NONUNIFORM 1415 X16 X18 X28 X X X3334 X39 X47 X5070 X7172 X97 X X
102 X118132 X133135 X144 X149 X178 X185 X206 X X214 X X228 X229 X230233239 X245 X246 X249 X294295 X X302 X305
95
PARTICLE SURFACE INTERFACE CORONAFg (cont.) 312 X X
313 X320 X X324 X355 X363369 X376382 X404 X407 X413416 X418 X424 X443 X459 X
THEORETICALDC UNIFORM 55
6578
101152156165166167184186207209217227236268271273278316319348349352373377406414417419454
X
X
X
X
XX
X
464 X XDC NONUNIFORM 188
207271
XX
96
PARTICLE SURFACE INTERFACE CORONA
XXXX
g (cont. ) 306316319337338348 X349359377 X406414417434454464 X
AC UNIFORM 1536
137184319348377406
X
X
XXX
X
AC NONUNIFORM 15230319336348377406434
X
X
XX
IMPULSE UNIFORM 15137184324417
X
X
XX
IMPULSE NONUNIFORM 15132230324347359376417
XX
X
REVIEWDC UNIFORM 45
486465
- 717388
XX
92 X X X96 X X X
X
97
PARTICLE SURFACE INTERFACE CORONASF^ (cont.
)
DC
AC
AC
) 105119 X150165184 X203209244 X X250 X251 X X X253258 X269 X X270 X X280 X X285 X X X368435436437438
NONUNIFORM 17 X45 X487173 X96 X X X
150234244 X X250 X251 X X X258 X270 X X285 X X X447 X
UNIFORM 45 X70 X7173 X96 X X X
105150184 X250 X251 X X X269 X X285 X X X
NONUNIFORM 45 X70 X7173 X96 X X X
150
98
PARTICLE SURFACE INTERFACE CORONASFg (cont.
)
183 X215 X X234250 X251 X X X285 X X X321 X X447 X458 X X
IMPULSE UNIFORM 45707173 X
XX
91 X X X92 X X X96 X X X
150184 X244 X X250 X258 X270 X X285 X X X
IMPULSE NONUNIFORM 174549707173
X
X
XX
X
96 X X X150215 X X234244 X X250 X258 X270 X X285 X X X321 X X447 X458 X X
SF^+SO^THEORETICALDC UNIFORM 78
SO^EXPERIMENTALDC UNIFORM 203
REVIEWDC UNIFORM 64
66 X X203244 X X
99
PARTICLE SURFACE INTERFACE CORONASO2 (cont..) 253
285334435436437438
DC NONUNIFORM 66244285334
AC UNIFORM 66285
AC NONUNIFORM 66285
IMPULSE UNIFORM 244285
IMPULSE NONUNIFORM 244285
SeFgEXPERIMENTALDC UNIFORM 203DC NONUNIFORM 30
REVIEWDC UNIFORM 150
203285438
DC NONUNIFORM 150285
AC UNIFORM 150285
AC NONUNIFORM 150285
IMPULSE UNIFORM 150285
IMPULSE NONUNIFORM 150285
TeF,REVIEWDC UNIFORM
TiCl,REVIEWDCDCACAC
UNIFORMNONUNIFORMUNIFORMNONUNIFORM
IMPULSE UNIFORMIMPULSE NONUNIFORM
438
285285285285285285
XX
XXXXXXXXXXXX
X
X
X
X
X
XXXXXX
XXXXXX
XX
XXXXXXXXXXXX
X X
X X
X X
X X
X X
XXXXXX
100
PARTICLE SURFACE INTERFACE CORONAXeEXPERIMENTALDC UNIFORM 389
390DC NONUNIFORM 170 X X
THEORETICALDC UNIFORM 163DC NONUNIFORM 163
REVIEWDC UNIFORM 45 X
66 X X163438
DC NONUNIFORM 45 X66 X X
163AC UNIFORM 45 X
66 X XAC NONUNIFORM 4 5 X
66 X XIMPULSE UNIFORM 45 XIMPULSE NONUNIFORM 45 X
101
VII. Author Index
Abdel-Salam, M.
Abdullah, M.
Abon-Seada, M. S,
Aihara, Y.
Akazaki, M.
Albrecht, H,
Aleksandrov, D. D.
Aleksandrov, G. N.
All, K.
Allen, K. R.
Allen, N. L.
Allibone, T. E.
Altoheh, L.
Ando, N.
Anis, H.
An jo, K.
Aoshima, Y.
Aoyagi, H.
Arahata, Y.
Aral, K.
Arima, J,
Arnesen, A.
Aschwanden, T.
Awad, M.
Azer, A. A,
1
244
465
2
179
3
4
5
232
8
11
9
173
302
1217
410
2
294
249
19
20
369
21
22
24
180
426
6 7
10 11
13 14 15 1618
144 180
321
23
102
Babu Rajendran, T. V,
Bahder, G.
Baldo, G.
Banford, H. M.
Banks, A. A.
Barnes, H. C.
Bashara, N. M.
Baumgartner, R,
Bederson, B,
Berberich, L. J,
Berg, D.
Berger, G.
Berger, S.
Bertein, H.
Berthold, V.
Bhalla, M. S.
Biasiutt, G.
Binns, D. F.
Blaha, J.
Blair, D. T. A.
Blodgett, F. W,
Bloss, W, H.
Bobo, J. C.
Boeck, W.
Boecker, H.
Bohme , H
.
Boillot, A.
25
26
27
28 29
30
26 31
32
464
140
33
34 203 313
35
36 37
38
39
40 41 42
21
43 44
380
45 45 46
47
3
423
48 49
177 370 463
23 50
35
103
Bortnik, I. M. 51 52 53 54 55
Bouillard, J. G. 256
Bouldin, D. W. 330
Boulloud, A. 56
Bouvier, B. 57 134
Boyd, H. A. 58 59 60 61
Bozin, S. E. 62 63
Brand, K. P. 64 65
Bregnsbo, E. 349
Brice, T. J. 457
Brown, S. C. 66
Bruce, F. M. 58
Brzosko, J, S, 67
Brzostek, E. 231
Buchholz, K. H. 68 239
Burger, W. 255
Busch, W. 69
Bychkov, Y. I. 296
Calderwood, J. H. 301
Camilli, G. 70 71 72 73
Carrara, G. 74 75
Carter, J. G. 81
Cernysev, V. J. 439
Chakravarty, B. 342 343
Chalmers, I. D. 76
Chanin, L. M. 77
Chantry, P. J. 78 236
104
Chee-Hing, D. J,
Chen, C. L,
Chiba, M.
Chistyakov, P. N.
Christodoulides, A. A,
Christophorou, L. G.
Coates, R.
Cobine, J. D.
Cohen, E. H.
Comsa, R. P.
Cones, H. N.
Conti, V. J.
Cooke, C. M.
Cookson, A. H.
Cortina, R.
Craggs, J. D.
Crichton, B, H.
Crichton, G. C.
Cronin, J. C.
Crowe, R. W.
Dakin, T. W.
Dale, S. J.
Daniel, T. N.
Das, M. K.
Davies, D, E.
79
236
415
80
331
81330
86
87
88
13
341
89
5494
9299
82331
83 84 85
24 377 440
9095
95267
91
96
92
97
93
98
100 340
40304
101
59
102
103
105
135
106
107
108
41311 361
137
60
104 115
313 459
136
42 283 285362
109 262
105
Davies, D. K. 110 111 236
Davis, G. H. L. 112
DeBitetto, D, J. 113
Degnan, W. J. 176
Dellera, L. 74
Devins, J. C. 104 114 115
Diessner, A. 116
Dincer, M. S. 161
Dring, D. 9 10 11
Driver, C. 117
Dubois, A. 423
Dupuy, J. 118
Dutton, J. 86 106 119 120 121122 123 124 125 126
Ellington, H. I. 127
Endo, F. 128 129
Ermel, M. 130 131
Eteiba, M. B. 132 376
Evans, N. B. 120
Facklam, T. 133
Fallou, B. 134
Farish, 0. 97 98 135 136 137138
Felsenthal, P. 139
Fiklik, V. 240
Fischer, A. 177 463
Fisher, L. H. 113 140 143 157 224225 293
106
Fitch, R. K. 108
Fleming, S. P. 178
Foord, T. R. 141 142
Freely, J. B. 143
Frost, L. S. 253
Fujinama, H. 144
Fujita, H. 145
Fujiwara, Y. 320 321 322
Galand, J. 134
Gallet, G. 35 146 147 256 257
Gallimberti, I. 27
Ganger, B. 148 149 150
Garcia, F. G. 26
Garcia, H. N. 27 35
Gary, C. 3 5
Geballe, R. 151 152
George, D. W. 153
Gerhold, J. 154
Gervais, Y. 326 351
Gilbert, A. 118
Gockenbach, E. 155 156
Golden, D. E. 157
Goldman, M. 35 158
Goodyear, C. C. 62 63 366 367
Gordon, G. S. 71
Gorin, B. N. 159
Gosho, Y. 160
107
Govinda Raju, G. R.
Grenon, J. F,
Griffiths, R. F.
Grunberg, P.
Hackam, R.
Hagenguth, J. H.
Hahn, G.
Hampton, B. F.
Hara, M.
Harada, T.
Harbec, G.
Harris, F, M.
Hasebe, K.
Hasegawa, H.
Hauschild, W.
Hayashi, H.
Hayashi, M.
Hazel, R,
Heilbronner, F. W.
Heisen, A.
Hepworth, J. K.
Hermstein, W.
Heylen, A. E. D.
Hickam, W. M.
161 162 163 164 165166 167 174 364 365
289 290
357
168
162 163 164 165 166167 169 170 171 172173 174 365
175 176
177
178
179
2 180
286 287 288 289 290
86 106 121 122 123124
181
401
68 182 183 184 185186 239 305 306
413
187
188
189
190
191 192
193 194
195 196 197 198 199200 201 202
203
108
Higashino, T,
Hileman, A. R.
Hixson, W. A.
Hoffman, R. L.
Hoh, S.
Honda, K.
Hood, R. J.
Hopkins, B. J.
Horii, K.
Howard, P. R.
Hughes, D. B.
Hughes, M. H,
Hunter, S. R,
Husain, E.
Hutzler, B.
Hutzler-Barre, D,
IEEE Committee Report
Ibrahim, O, E.
Ichihara, Y.
Ikeda, C.
Iliceto, F.
Inamura, S.
Inuishi, Y,
Isa, H.
Isaksson, K.
Ishikawd, R.
Iskoldskii, A. I.
413
441
204
204
325
205
43
109
323
206
121
125
81
208
27
210
212
137
213
214
237
249
215
216
291
129
296
324
207
122 123
209 316 317
35 146 210 211
211
109
Itaka, K.
Ito, Y.
Itoh, H.
Ivanov, V. L.
Jahn, G.
Jahn, H.
James, D. R.
Jervis-Hunter , G.
Johansen, I.
Jones, B.
Jones, G. J.
Jones, J.
Jones, R. E.
Jouaire, J.
Kachickas, G. A.
Kachler, A. J.
Karlsson, P. W.
Kawaguchi, Y.
Kawai, H.
Kawane, K,
Kedzia, J.
Khalifa, M.
Kichikawa, T.
Kielmann, F.
Kind, D.
Kishijima, I.
Kita, K.
413
2
217
6
380
219
82
220
369
221
124
223
448
27
224
226
227
228
181
318
231
232
128
186
234
410
419
218 399
83 84 85 330
222
449
35
225
349 350
229 230
129
233
110
Klewe, R. C.
Kline, L. E.
Klobukowska, J.
Knudsen, N.
Kohrman, W,
Kopainsky, J.
Korshunov, G. S.
Kosztaluk, R.
Kouno, T.
Kourtev, J.
Kremnev, V, V.
Krey, B.
Kromer, I. L.
Kucera, J.
Kucukarpaci, H. N,
Kuffel, E.
Kuffel, J.
Kulkarni, S. V.
Kuttner, H.
Kuwahara, H.
LaForest, J. J.
Lacey, R.
Laghari, J. R.
Lakshminarasimha, C. S.
Lanoue, T. J.
Lautensclager, H. G.
Lebeda, J.
191
235
67
237
238
65
297
257
145
344
297
68
147
240
242
188363
247
316
248
249
226
147
250
25
453
133
350
192
236
325
345
239
257
241
243 244 245 246461
317
321
251
252 402 403
111
Lee, A.
Lee, Z. Y.
Lemke, E,
Leon, B.
Leroy, G.
Lewis, T. J.
Liao, T. W.
Linck, H.
Lindsay, E. W,
Linn, F. S.
Llewellyn-Jones, F,
Lobley, E. H.
Loeb, L. B.
Los, E. J.
Lucas, J.
Luxa, G.
Lyapin, A. G.
MacAlpine, J. M. K,
Malik, N. H.
Mailer, V. N.
Mansoor, F. F.
Manterfield, R. J.
Marton, J. P.
Masetti, C,
Mason, J. H.
Mastovsky, J.
253
254
255
423
35
201
72
259
33
151
260
191
264
265
242
105
266
267
268273
276
44
315
332
377
280
380
307
147 256 257
202
175 241 258
460
261 262 263
298
252
269 270 271 272274 275 382 461
277 278 279
i112
Mathis, R. A.
Matsuo, H,
McAllister, I. W.
McClure, G. W.
McCorkle, D. L.
McCormick, N. R,
McElroy, A, J,
McNeall, P. I.
Meats, R. J.
Meek, J. M.
Menemenlis, C.
Menemenlis, H.
Menes, M.
Menju, S.
Mesyats, G, A,
Miller, C. G.
Miller, H. C.
Mirza, J. S,
Misakian, M.
Miyachi, I.
Miyake, K.
Miyoshi, Y.
Mizukami, T,
Morgan, G, B.
Mori, N.
Morris, W. T.
81330
328
281
282
85
283
26
404
284
285
286291
7
292
228
296
298
299
301
434
309
411
187
302
120
213
126
82 83 84 85
287 288 289 290
293
229 230 294 295
297
300
412
113
Moruzzi, J. L.
Mosch, W.
Mukhedkar, D,
Muller, E. K.
Murai, Y.
Nagata, M.
Nagata, S.
Naidu, M. S.
Nakanishi, K,
Narbut, P.
Naumann, W.
Nelson, J. K.
Nema, R. S.
Nielsen, T. M.
Niemeyer, L.
Nishihara, S,
Nitta, T.
Noguchi, T,
Noguchi, Y.
Ohno, H.
Ohuch, Y.
Olendzkaia, N. F,
Olivier, G.
Oppermann, G.
Orlinov, V.
Oshige, T,
303 304
305 306 307
326 351
308
20
309
20
25 276 277 278 310311 373 402 403
312
313
314
315
208 209 316 317
349
359
413
312 318 319 320 321322
323 324
145 325
294
410
4
326
105
344 345
327 328
114
Ozawa, J. 129
Pace, J. D. 329
Pace, M. O. 330
Pai, R. Y. 330 331
Pai, S. T. 332
Panov, A. A. 55
Papadias, B. C. 333
Papoular, R. 334
Parekh, H. 335 336 337 338 383384 385
Paris, L. 339 340
Park, J. H. 341
Parker, A, B. 263 329
Paul, J. C. 342 343
Pech, P. 344 345
Pedersen, A. 227 281 346 347 348349 350
Pelletier, J. M. 351
Penney, G. W. 387
Perlin, A. S. 352
Perry, E. R. 102
Pfeiffer, W. 353 354 355 356
Phelps, C. T. 357
Phillips, K. 8
Pilling, J. 358
Pinnekamp, F. 359
Plump, R. E. 71 72 73 258
Podporkyn, G. V. 5 7
115
Prasad, A. N.
Price, D. A,
Proud, J. M.
Ptitsyn, S. V.
Oiu, Y.
Oureshi, A. H,
Radwan, R.
Radwan, R. M.
Radwan, R. O.
Raja Rao, C.
Razzak, S. A. A.
Reeves, M. L,
Reichman, J.
Rein, A.
Rejngold, A. S.
Remde, H. E.
Renardieres Group, Les
Richards, P. H,
Richter, K.
Risbud, A. V.
Ritow, H,
Riu, J.
Rizk, F, A. M.
Robinson, M,
Rohlfs, A. F.
Rork, G. D,
310 311 360 361 362
Z3«
139
4
363
250 251 269 270 271272 273 274 275 382461
232
465
245
364 365
366 367
152
247
368 369
439
370
371
153
372
373
374
146
132 375 376 377 424
378 379
176 241
77
116
Rothhardt, L.
Rudge, A. J.
RyzkOr H.
Saelee, H. T.
Safar, Y. A.
Saha» T. N.
Sakamoto^ S.
Sakata, K.
Salanir N. A.
Salamar N. M. A.
Sartorior G.
SatOr H.
Scheiber D.
Schmiedl, G.
Schmitz, L. S.
Schneider^ H. M.
Schonhuber» M. J.
Schramm, J.
Schrier, S.
Schroderr G. A.
Schulz, W.
Schwabr A.
Sforzinir M,
Sharbaugh, A. H*
Shibuya» Y.
Shimozumar N«
Shkilev, A. V.
380
30
381
242
274 382
342 343
218
229 230
232
335 383 384 385
74
302
314
386
387
388
389 390
391
392
393 394
395
396
100
397 398 450
312 319 320 321
217 218 399 400 401
159
117
Siddagangappa, M, C,
Sigmond, R. S.
Sikolov, S. M.
S imon , M , F
,
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Taschini, A.
Tatuso, T.
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374. H. Ritow, "The Role of Space Charge in Gas Break-through Between Equal Parallel Plane Electrodes Belowthe Paschen Minimum", J. Electron. Control., Vol. 7,
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154
375. F. A. M. Rizk, "Effect of Large Electrodes on SparkoverCharacteristics of Air Gaps and Station Insulators",IEEE Trans, on Power Appar. Syst, , Vol. PAS-97, no. 4,
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376. F. A. M. Rizk and M. B. Eteiba, "Impulse BreakdownVoltage-Time Curves of SF>. and SF,-N2 Coaxial-CylinderGaps", IEEE Trans, on Power Appar. Syst. , Vol. PAS-101,no. 12, pp. 4460-4471 (1982).
377. F. A. M. Rizk, C. Masetti, and R. P. Comsa, "Particle-Initiated Breakdown in SF^ Insulated Systems Under HighDirect Voltage", IEEE Trans, on Power Appar. Syst.,Vol. PAS-98, no. 3, pp. 825-836 (1979).
378. M. Robinson, "The Corona Threshold for CoaxialCylinders in Air at High Pressures", IEEE Trans, onPower Appar. Syst., Vol. PAS-86, no. 2, pp. 185-189(1967).
379. M. Robinson, "Critical Pressures of the Positive CoronaDischarge between Concentric Cylinders in Air",J. Appl. Phys., Vol. 40, no. 13, pp. 5107-5112 (1969).
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388. H. M, Schneider and F. J. Turner, "Switching-SurgeFlashover Characteristics of Long Sphere-Plane Gaps forUHV Station Design", IEEE Trans, on Power Appar, Syst.,Vol. PAS-94, no. 2, pp. 551-560 (1975).
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156
i
397. A. H. Sharbaugh and P. K. Watson, "Breakdown Strengthsof a Perf luorocarbon Vapor (FC-75) and Mixtures of theVapor with SF^", IEEE Trans, on Power Appar. Syst.,Vol. PAS-83, pp. 131-136 (1964).
398. A. H. Sharbaugh and P. K. Watson, "The ElectricStrength of Hexane Vapor and Liquid in the CriticalRegion", J. Appl. Phys., Vol. 48, no. 3, pp. 943-950(1977).
399. M. Shimozuma, H, Itoh, and H. Tagashira, "Measurementof the Ionization and Attachment Coefficients in SFgand Air Mixtures", J. Phys. D: Appl. Phys., Vol. 15,pp. 2443-2449 (1982).
400. M. Shimozuma and H. Tagashira, "Measurement of theIonization and Attachment Coefficients in SF, andHelium Mixtures", J. Phys. D: Appl. Phys., Vol. 16,pp. 1283-1291 (1983).
401. M. Shimozuma, H. Tagashira, and H. Hasegawa, "TheIonization and Attachment Coefficients in CarbonTetraf luoride", J. Phys. D: Appl. Phys., Vol. 16,pp. 971-976 (1983).
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410. T. Suzuki, I. Kishijima, Y. Ohuch, and K. Anjo,"Parallel Multigap Flashover Probability", IEEE Trans,on Power Appar. Syst., Vol. PAS-88, no. 12,
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411. T. Suzuki and K. Miyake, "Breakdown Process of Long AirGaps with Positive Switching Impulses", IEEE Trans, onPower Appar. Syst., Vol. PAS-94, no. 3, pp. 1021-1029(1975).
412. T. Suzuki and K. Miyake, "Experimental Study ofBreakdown Voltage-Time Characteristics of Large AirGaps with Lightning Impulses", IEEE Trans, on PowerAppar. Syst., Vol. PAS-96, no. 1, pp. 227-233 (1977).
413. T. Takagi, H. Hayashi, T. Higashino, S. Nishihara, andK. Itaka, "Dielectric Strength of SFg Gas and 3-CoreType CGI Cables Under Inter-Phase Switching ImpulseVoltages", IEEE Trans, on Power Appar. Syst.,Vol. PAS-93, no. 1, pp. 354-359 (1974).
414. T. Takuma, "Discharge Mechanism of Gases and ItsApplication to Calculation of Flashover Voltages ofSphere Gaps in Atmospheric Air", Elec. Eng. in Japan,Vol. 91, no. 1, pp. 63-75 (1971).
415. T. Takuma and M. Chiba, "Positive DC Corona and SparkCharacteristics in High Pressure Air", Elec. Eng. inJapan, Vol. 88, no. 9, pp. 10-15 (1968).
416. T. Takuma and T. Watanabe, "Discharge Characteristicsof Long Gaps in High-Pressure SFg Gas", Elec. Eng. inJapan, Vol. 90, no. 3, pp. 166-176 (1970).
417. T. Takuma and T. Watanabe, "Theoretical Analysis ofDischarge Characteristics in High Pressure SFg Gas",Elec. Eng. in Japan, Vol. 90, no. 4, pp. 26-33 (1970).
418. T. Takuma and T. Watanabe, "Comparison between GasInsulation and Atmospheric Air Insulation", Elec. Eng.in Japan, Vol. 90, no. 6, pp. 227-244 (1970).
i
158
419. T. Takuma, T, Watanabe, and K. Kita, "BreakdownCharacteristics of Compressed-Gas Mixtures in NearlyUniform Field", Proc. lEE, Vol. 119, no. 9, pp. 927-928(1972).
420. T. Tatuso, T. Tada, and Y. Watanabe, "Switching SurgeSparkover Characteristics of Air Gaps and InsulatorStrings Under Nonstandard Conditions", IEEE Trans, onPower Appar. Syst. , Vol. PAS-87, no. 2, pp. 361-367(1968).
421. L. C. Thanh, "Distribution of Electric Fields in a Rod-to-Plane Gap at the Onset of Negative Corona", Proc.lEE, Vol. 126, no. 3, pp. 270-275 (1979).
422. L. Thione, "The Dielectric Strength of Large AirInsulation", Surges in High-Voltage Networks , ed. byK. Ragaller, Plenum Press, New York, pp. 165-205(1980).
423. J. Thoris, B. Leon, A. Dubois, and J. C. Bobo,"Dielectric Breakdown of Cold Gaseous Helium in LargeGaps", Cryogenics, Vol. 10, no. 2, pp. 147-149 (1970).
424. N. G. Trinh, F. A. M. Rizk, and C. Vincent,"Electrostatic-Field Optimization of the Profile ofEpoxy Spacers for Compressed SFg-Insulated Cables",IEEE Trans, on Power Appar. Syst., Vol. PAS-99, no. 6,
pp. 2164-2174 (1980).
425. N. G. Trinh and C. Vincent, "Bundled-Conductors for EHVTransmission Systems with Compressed-SFg Insulation",IEEE Trans, on Power Appar. Syst., Vol. PAS-97, no. 6,
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426. I. Tuneyase and M. Akazaki, "Breakdown Processes of aNegative Point-to-Plane Air Gap at Atmospheric Pressureunder Impulse Voltage", Elec. Eng. in Japan, Vol. 93,no. 6, pp. 6-12 (1973).
427. T. Udo, "Sparkover Characteristics of Large Gap Spacesand Long Insulation Strings", IEEE Trans, on PowerAppar. Syst., Vol. PAS-83, no. 5, pp. 471-483 (1964).
428. T. Udo, "Switching Surge and Impulse SparkoverCharacteristics of Large Gap Spacings and LongInsulator Strings", IEEE Trans, on Power Appar. Syst.,Vol. PAS-84, no. 4, pp. 304-309 (1965).
429. T. Udo, "Switching Surge Sparkover Characteristics ofAir Gaps and Insulator Strings Under PracticalConditions", IEEE Trans, on Power Appar. Syst.,Vol. PAS-85, no. 8, pp. 859-864 (1966).
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431. T. Udo, T. Tada, and Y. Watanabe, "Flashover /
Characteristics of Large Gap Spacings Due to Pulse andSwitching Surges", Elec. Eng. in Japan, Vol. 84,no. 12, pp. 69-78 (1964).
432. T. Udo, T. Tada, and Y. Watanabe, "FlashoverCharacteristics of Gaps and Insulators Due to SwitchingSurges", Elec. Eng. in Japan, Vol. 86, no. 5, pp. 22-31(1966).
433. T. Udo and Y. Watanabe, "DC High-Voltage SparkoverCharacteristics of Gaps and Insulator Strings", IEEETrans, on Power Appar. Syst., Vol. PAS-87/ no. 1,
pp. 266-270 (1968).
434. R. J. Van Brunt and M. Misakian, "Mechanisms forInception of DC and 60-Hz AC Corona in SFg", IEEETrans, on Elec. Insul. , Vol. EI-17, no. 2, pp. 106-120(1982).
435. A. K. Vijh, "Correlation Between Electric Strengths andHeats of Atomization of Gaseous Dielectrics", J. Mater.Sci., Vol. 11, pp. 784-785 (1976).
436. A, K. Vijh, "Intermolecular Bonding and the ElectricStrengths of Dielectric Gases", J. Mater. Sci.,Vol. 11, pp. 1374-1375 (1976).
437. A. K. Vijh, "Electric Strength and Molecular Propertiesof Gaseous Dielectrics", IEEE Trans, on Elec. Insul.,Vol. EI-12, no. 4, pp. 313-315 (1977).
438. A. K. Vijh, "On the Relative Strengths and theMolecular Weights of Gases", IEEE Trans, on Elec.Insul., Vol. EI-17, no. 1, pp. 84-87 (1982).
439. O. V. Volkova, A. S. Rejngold, and V. J. Cernysev,"Influence of Humidity on Flashover Voltages of LongAir Gaps", Elektricestvo, no. 3, pp. 49-53 (1968).
440. 0. Vuhuw and R. P. Comsa, "Influence of Gap Length onWire-Plane Corona", IEEE Trans, on Power Appar. Syst.,Vol. PAS-88, no. 10, pp. 1462-1475 (1969).
441. C. F. Wagner and A. R. Hileman, "Mechanism of Breakdownof Laboratory Gaps", AIEE Trans., Vol. 80, Part III,pp. 604-622 (1961).
160
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445. Y. Watanabe, "Switching Surge Flashover Characteristicsof Extremely Long Air Gaps", IEEE Trans, on PowerAppar. Syst., Vol. PAS-86, no. 8, pp. 933-936 (1968).
446. Y. Watanabe, "Switching Impulse FlashoverCharacteristics of Thin Wire Gaps", IEEE Trans, onPower Appar. Syst., Vol. PAS-90, no. 5, pp. 2301-2305(1971).
447. R. T. Waters, "Spark Breakdown in Non-Uniform Fields",Electrical Breakdown of Gases , ed. by J. M. Meek andJ. D. Craggs, John Wiley and Sons, New York,pp. 385-532(1978).
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^
162
465. A. R. M. Zaghloul, R. M. Radwan, and M, S. Abon-Seada,"Characteristic Time of Oxygen: Calculation andTheoretical Study", IEEE Trans, on Elec. Insul.,Vol. EI-11, no. 1, pp. 28-32 (1976).
163
IX. Technical Conference Proceedings
1. International Symposium on Gaseous Dielectrics.Proceedings:
a) Gaseous Dielectrics III, ed. byL. G. Chr istophorou, Pergamon Press, New York(1982).
b) Gaseous Dielectrics II, ed. byL. G. Chr istophorou, Pergamon press. New York(1980).
c) Gaseous Dielectrics, ed. byL. G. Chr istophorou, NTIS, CONF-780301, (1978).
2. Gaseous Electronics Conference.Proceedings:
Abstracts published annually for thirty-sixconferences in the Bulletin of the AmericanPhysical Society.
3. IEEE International Symposium on Electrical Insulation.Proceedings:
Conference records for 1982, -80, -78, -76published by the Institute for Electrical andElectronics Engineers, Inc., New York.
4. Conference on Electrical Insulation and DielectricPhenomena (CEIDP).Proceedings
:
a) Annual reports for 1981-3 CEIDP published byInstitute for Electrical and ElectronicsEngineers, Inc., New York.
b) Annual reports for CEIDP before 1981 publishedby National Academy Press, Washington, DC.
5. International Coference on Gas Discharges and TheirApplications (CGA).Proceedings
:
a) Proceedings of Seventh ICGA, 1982 published byPeter Peregrinus Ltd. , London.
b) Proceedings of Sixth-First ICGA (1980-70)published by Institution of ElectricalEngineers, London.
6. International Symposium on High Voltage Engineering.Proceedings:
Four conferences from 1977-83, papers distributed butproceedings not published.
164
7. International Conferences on Phenomena in IonizedGases.Proceedings:
Sixteen conferences from 1951-1983, proceedingspossibly available from different publishers.
T^U.8. GOVERNMENT PRINTING OFFICE; 198i* kZO 997 70
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4. TITLE AND SUBTITLE
Bibliography of Data on Electrical Breakdown in Gases
5. AUTHOR(S)
R. J. Van Brunt and W. E. Anderson
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This report consists of a bibliography of currently published data on electrical
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lished since 1950, an index indicating the references that give particular types of
data for each gas, an author index, and a list of relevant, regular technicalconferences. The citations given in the bibliography contain experimental ortheoretical data on breakdown which include: 1) sparking potentials; 2) breakdownvoltages; 3) critical fields, or field-to-gas density ratios; 4) corona inceptionvoltages; 5) voltage-time characteristics; 6) relative and absolute dielectricstrengths; and 7) breakdown probabilities. Types of data considered include thosewhich apply to uniform and nonuniform fields; ac, dc, and impulse voltages; andpossible effects of particles, surfaces, interfaces, and corona. This bibliographyis intended to serve as a guide in locating data on breakdown which are most relevantto particular applications.
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bibliography; critical fields; corona onset; discharge inception; electrical
breakdown; gases; sparking potentials
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engaged in scientific and technical work.
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data on the physical and chemical properties of materials, com-piled from the world's literature and critically evaluated.
Developed under a worldwide program coordinated by NBS under
the authority of the National Standard Data Act (Public Law90-396).
NOTE: The principal publication outlet for the foregoing data is
the Journal of Physical and Chemical Reference Data (JPCRD)published quarterly for NBS by the American Chemical Society
(ACS) and the American Institute of Physics (AlP), Subscriptions,
reprints, and supplements available from ACS, 1 155 Sixteenth St.,
NW, Washington, DC 20056.
Building Science Series— Disseminates technical ir formation
developed at the Bureau on building materials, components,
systems, and whole structures. The series presents research results,
test methods, and performance criteria related to the structural and
environmental functions and the durability and safety charac-
teristics of building elements and systems.
Technical Notes—Studies or reports which are complete in them-
selves but restrictive in their treatment of a subject. Analogous to
monographs but not so comprehensive in scope or definitive in
treatment of the subject area. Often serve as a vehicle for final
reports of work performed at NBS under the sponsorship of other
government agencies.
Voluntary Product Standards— Developed under procedures
published by the Department of Commerce in Part 10, Title 15, of
the Code of Federal Regulations. The standards establish
nationally recognized requirements for products, and provide all
concerned interests with a basis for common understanding of the
characteristics of the products, NBS administers this program as a
supplement to the activities of the private sector standardizing
organizations.
Consumer Information Series— Practical information, based on
NBS research and experience, covering areas of interest to the con-
sumer. Easily understandable language and illustrations provide
useful background knowledge for shopping in today's tech-
nological marketplace.
Order the above NBS publications from: Superintendent of Docu-
ments. Government Printing Office. Washington. DC 20402.
Order the following NBS publications^FIPS and NBSIRs—fromthe National Technical Information Service, Springfield. VA 22161
.
Federal Information Processing Standards Publications (FiPS
PUB)— Publications in this series collectively constitute the
Federal Information Processing Standards Register. The Register
serves as the official source of information in the Federal Govern-
ment regarding standards issued by NBS pursuant to the Federal
Property and Administrative Services Act of 1949 as amended.
Public Law 89-306 (79 Stat. 1127), and as implemented by Ex-
ecutive Order 1 1717 (38 FR 12315, dated May II, 1973) and Part 6
of Title 15 CFR (Code of Federal Regulations).
NBS Interagency Reports (NBSIR)—A special series of interim or
final reports on work performed by NBS for outside sponsors
(both government and non-government). In general, initial dis-
tribution is handled by the sponsor; public distribution is by the
National Technical Information Service , Springfield, VA 22161,
in paper copy or microfiche form.
U.S. Department of CommerceNational Bureau of Standards
Washington, DC. 20234Official Business
Penalty for Private Use $300