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Stefan Velkov. Leon Schneider. Gustav Marcussen. Julius Paris. Carclul analysis ol thc prcscrvcd lragmcnt ol thc rclicl lrom Pincum and its comparison with othcr Uppcr Mocsian monumcnts may provc usc lul in rcconstructing thc original appcarancc ol thc luncrary monumcnt thc rclicl lormcd part ol.
Tc rclicl showing Achillcs dragging Hcctors body was most probably placcd on thc soclc, givcn that thc marblc part bclow thc rclicl is coarscr, lacks nish and is narrowcr, which indicatcs that it was buricd in thc ground.
Tc prcscrvcd basc ol a scmicolumn abovc thc rclicl indicatcs that thc inscription cld was ankcd by scmicolumns. Pilipovi, Hcroic Tcmcs ol thc Trojan Cyclc in Roman Funcrary Art pcculiar to thcm.
Tc soclcs ol thcsc monumcnts bcar thc lollowing gural sccncs: augurs, hunting horscmcn, rapc ol uropa, and dolphins with a tridcnt.
Two monumcnts with thcir soclcs bcaring thc motil ol cantharos with vinc or a rc licl which is not clcarly lcgiblc today, which also havc thc inscription cld ankcd by scmicolumns abovc, arc not mcntioncd hcrc.
Cornclius Rulus, or thc rclicl with Hcraclcs and Alccstis, now built into thc lortrcss ol Smcdcrcvo. Minor iconographic dicrcnccs in thc iconography ol thcsc picccs with thc thcmcs lrom thc Trojan Cyclc, which arc not so numcrous, show that thc carvcr who cut thc Pincum rclicl most probably had bclorc him a pattcrnbook lrom!
Kondi, thc rclicl lrom Pin cum, as wcll as thc rclicl ol Hcraclcs and Alccstis, or thc rclicls on thc sidcs ol thc sarcophagi showing!
All this supports thc as sumption that this rclicl, or thc monumcnt, should bc datcd to thc rst hall ol sccond ccntury, which is thc datc ol most ol thc monumcnts with this thcmatic rcpcrtoirc.
Tus such a lriczc was bcncath thc Rapc ol Pcrscphonc on thc stcla ol M. Alkcstis, no. Pilipovi, Hcroic Tcmcs ol thc Trojan Cyclc in Roman Funcrary Art Tc rclicl ol Achillcs and Hcctor lrom Pincum was discovcrcd along with an inscription, prcscrvcd only lragmcntarily and lost today.
Firstly, both lragmcnts wcrc madc ol thc samc matcrial. And nally, cvcn thc dimcnsions ol thc lrag mcnts may suggcst that thcy oncc lormcd part ol onc wholc.
Tc thickncss ol thc inscribcd lragmcnt was cm, and ol thc rclicl bctwccn and cm. Tc inscription, dcntcd on all lour sidcs, was o cm widc, and thc rclicl, damagcd only on onc sidc, is 8o cm widc.
Unlortunatcly, thc scarch through thc National Muscums documcntation has so lar lailcd to conrm that thc inscription lrom Pincum uscd to bc kcpt in thc Muscum, as statcd by carlicr rcscarchcrs.
Although thc two picccs arc vcry likcly to bc lragmcnts ol onc luncrary monumcnt, it will not bc possiblc to say anything morc until ad ditional inlormation is lound in thc Muscum documcntation.
As thc inscription, duc to its lragmcntary prcscrvation, is, and was cvcn at thc timc ol its rst publication, vcry dil cult to rcad, it is not quitc clcar to whom thc monumcnt was dcdicatcd.
Probably thrcc pcrsons,! Vhat can bc sccn lrom this inscription is that thosc wcrc gcntilc namcs Fla. Mirkovi, in hcr rcscarch into thc origin ol thc inhabitants ol Pincum, mcntions this vcry inscription, or its publishcd lragmcnt, as a con rmation ol thc cxistcncc ol thc namcs Fla.
Scttlcmcnt ol vctcrans in thc vicinity ol lcss important military camps, likc thc onc in Pincum, bcgan rclativcly carly, which is supportcd by cvidcncc on thcsc scttlcmcnts lrom thc rst hall ol thc sccond ccntury and latcr.
A largc numbcr ol stampcd bricks havc bccn discovcrcd at this sitc to datc. Claudia, whilc thosc stampcd with leg IIII probably rclcr to!
Mirkovi bclicvcs that it also rclcrs to a pcrson scrving in this lcgion. Claudia was stationcd. Town administrators, dccurions, also sct up thc monumcnt with thc rclicl ol augurs on thc soclc, and Hclcn and Mcnclaus in thc ccntral rclicl, and thc monumcnt with S.
Pilipovi, Hcroic Tcmcs ol thc Trojan Cyclc in Roman Funcrary Art Tc dcscribcd qualitics ol thc rclicl ol Achillcs and Hcctor lrom Pin cum, and thcrclorc thc luncrary monumcnt itscll, raisc many issucs con ccrning this, obviously as yct uncxplorcd, antiquc scttlcmcnt.
Kanitz visitcd it, all that rcmaincd ol thc lort was onc wall towards thc anubc, still visiblc in somc placcs. Scholars havc idcnticd Pincum, thc Roman and arly 8yzantium lort.
Tc mcntioncd brick inscrip tions comc lrom Pincum,. Claudia, which wcrc dcdicatcd to Jupitcr, onc by a lormcr soldicr and thc othcr, abovc a lragmcntarily prcscrvcd sculptural rcprcscntation, by Aclius Silvanus.
For thc dcdicant ol Jasons sarcophagus, ol high military ranking, and analysis ol thc iconography ol this sarcophagus, scc Pilipovi :oo, 68, cl.
Cunjak, bascd on thc rcsults ol smallscalc rcscuc cxcavations, simply rcports a nccropolis with crcmation burials to thc northwcst ol Pincum, and anothcr onc with inhumation burials to thc southwcst ol thc lort.
Transccnding in its signicancc thc provincial boundarics, thc monumcnt discusscd in this papcr corroboratcs this bclicl.
Jovanovi :ooo, 8:, in his analysis ol thcsc daggcrs, suggcsts that thc two arc complcmcntary and idcntics thcm as sica, a wcllknown wcapon ol Tracian or a cian origin.
Trough carclul analysis thc author arrivcs at thc conclusion that this is thc gravc ol a lormcr soldicr ol!!!!
Claudia, and datcs it to thc rst hall ol thc :nd ccntury. Pilipovi, Hcroic Tcmcs ol thc Trojan Cyclc in Roman Funcrary Art!
Tc idca to dcpict thc hcroic thcmc with Achillcs and Hcctor on thc marblc rclicl lrom Pin cum, and thc cmphasis on thc idca that only.
Claudia was stationcd at Pincum, hc may havc bclongcd to onc ol its units. Tc inscription discovcrcd along with this rclicl lragmcnt probably bclongcd to thc samc scpulchral wholc.
Although its rcading is madc di cult by its lragmcntary statc ol prcscrvation, it suggcsts Romanizcd inhabit ants whosc gcntilc namcs wcrc Fla.
Institute for Balkan Studies Serbian cademy of Sciences and rts Belgrade Abbreviations Sources Apd.
Apollodori, Bibliotheca Apd. Apollodori, Epitome Artcm. Artcmidorus aldianus, Oneirocritica Il. Homcri, Ilias Hyg. Hygini, Fabulae Plat.
Platon, Symposium Plut. Plutarchus, Quaestiones Graecae Proclos, Chrest. Proclos, Chrestomathia Literature E Lanee epigraphique, Paris. GSD Glasnik Srpskog arheolokog drut.
GDKS Glasnik drut. ILJug A. IMS Inscriptions de la Mesie Superieure! Jahreshefte Jahrcschcltc dcs stcrrcichischcn archaologischcn!
Spomenik Spomenik SK. Scrbian Royal Acadcmy, 8clgradc. Bibliography Allldy, G. Cambi, N. Split: Knjicvni krug. Cumont F. Fecherches sur la symbolisme funeraire des Fomains.
Paris: P. Cunjak, M. Zatitna arhcoloka iskopavanja nckropola Pinkuma. Fimska kamena plastika u jugoslo. Aspccts ol Roman Mining in Noricum, Pannonia, almatia and Mocsia Supcrior.
Popovi, T. Cvjctianin and 8. Fmai Kfaragas es Ks. Fcrri, S. Mit i antika knjie. Jovanovi, A. Arhcoloki tragovi impcrijalnog trijumla nad aanima sa prostora Gornjc Mczijc, Zbornik Matice srpske.
Falsikati u arhcolokom matcrijaluupozoravajua aktuclnost. Kalinka, K. Kanitz, F. Die Fomischen Funde in Serbien.
Studien in Serbien, cnkschriltcn dcr Kaiscr Akad. Classc XL!. Scpulkralni spomcnici sa tcritorijc rimskc provincijc Gornjc Mczijc.
Ladck, F. Fomer an der Mittleren Donau. Fomische Strassen und Festungen. Mscy, A. Pannonia and Upper Moesia. Lc langagc symboliquc dans la dcoration a scncs my thologiqucs ct son scns dans lcs tombcs pcintcs dc lricnt romain nouvcllc approchc.
Paleograja rimskih natpisa u Gornjoj Me. Classis Flavia mocsica na unavu u Gornjoj Mcziji, Starinar XLXL! Fimski nakit u Narodnom mu.
Schclold, K. La lorcc cratricc du symbolismc lunrairc dcs Romains, F!! Schobcr, A. Die romischen Grabsteine. Sichtcrmann, H. Griechische Mythen auf romischen Sarkophagen.
Toynbcc, J. Turcan, R. Lcs sarcophagcs romains ct lc problmc du symbolismc lunrairc, NF! Messages doutre-tombe. Liconographie des sarcophages romains.
Paris: c 8oc card. Gradita, Starinar!! Prcmcrstcin, F. Antiki spomcnici u Srbiji, Spomenik XXX! X, National Muscum, 8clgradc photo National Muscum, 8clgradc Fig.
Pilipovi, Hcroic Tcmcs ol thc Trojan Cyclc in Roman Funcrary Art Fig. Achillcs and Hcctor, marblc rclicl lound at! Muscum ol 8udapcst photo rdlyi, g.
Hclcn and Mcnclaus, rclicl on thc marblc stcla ol C. National Muscum, Poarcvac photo!. Stani Tanja Pctrovi Such Were the Times Serbian Peasant Women Born in the rqzos and rqos and the Stories of Teir Lives :.
Tc storics wcrc collcctcd primarily lor thc purposc ol linguis tic dialcctological rcscarch: thc qucstion Tell me about your life or Tell me. Tc matcrial obtaincd in this way can bc a valuablc sourcc ol two kinds ol inlormation.
Namcly, it providcs inlormation about how thc pco plc intcrvicwcd livcd scvcral dccadcs ago, how thcy cxpcricnccd important changcs in thcir pcrsonal livcs as wcll as important historical momcnts such as wars, major political changcs, ctc.
Similarly to this vicw, Lindc strcsscs that lilc storics cxprcss our scnsc ol scll: who wc arc and how wc got that way.
Tcy arc also onc vcry important mcans by which wc communicatc this scnsc ol scll to thc othcrs. All thc womcn intcrvicwcd arc ol similar agc and thc samc social group to which thc majority ol thc lcmalc population ol thcir agc in thc arcas thcy comc lrom bclongs all ol thcm comc lrom rural parts ol Scr bia, havc livcd in pcasant lamilics, all havc spcnt thcir livcs in villagcs, and all arc illitcratc.
Tc analysis will locus on thc pcriod whcn thcy wcrc young, whcn thcy got marricd and movcd lrom thcir lathcrs to thc lamily ol thcir lathcrinlaw.
Tc lact that rlichs work rclcrs to thc samc pcriod and dcals with thc samc phcnomcna ol lam ily lilc makcs it possiblc lor hcr rcsults, acquircd mainly by thc qucstionnairc mcthod, to bc comparcd with this matcrial, obtaincd by thc oral history mcthod, which ocrs pcrsonal accounts.
Tc proccss ol rcmcmbcring is always highly dcpcndcnt on thc prcscnt momcnt, at which thc act ol rcmcmbcr ing takcs placc. Tc prcscnt momcnt givcs shapc to pcoplcs mcmorics, and cnablcs thcm to position thcmsclvcs in thc cxisting social rcality, and to ncgotiatc and justily thcir statuscs and rolcs.
Narration, as a lorm ol rcmcmbcring, is a way in which pcoplc assign mcaning to thcir mcmorics. Narrativc is among thc.
Felationality: Discursi. Lo and A. Pctrovi, Such! Spcaking about thcir own past and thc timc ol thcir youth, thc in tcrvicwcd womcn wcrc awarc ol thc changcs that havc occurrcd in lamily structurc and valucs in thc mcantimc.
Lilc history is always thc print ol thc intcraction 6 Lindc, Life Stories, 8. Stcwart, Nostalgia. Nicdcrmullcr, From thc Storics ol Lilc to thc Lilc History: Historic Contcxt, Social Proccsscs and thc 8iographical Mcthod, in Life History as Cultural Construction Performance, cds.
Holcr and P. Tc rcscarch was conccrncd with languagc rathcr than with thc topics intcrvicwccs spokc about, but thc casicst way to obtain thc matcrial nccdcd was to ask thcm to spcak about thcir livcs.
As 8ausingcr strcsscs, topics such as birth, baptism, marriagc or dcath wcrc rarcly brought up. Pcoplc prclcrrcd to spcak about moving to or visiting othcr towns and citics, or about cxtrcmc cxpcricnccs such as war.
Tis dialogism is thc rcason why thc autobiographical discoursc analyzcd hcrc typically consists ol statcmcnts dcscribing cvcnts lollowcd by pcrsonal com mcnts, as a rulc, thcsc commcnts rclcr to dicrcnccs bctwccn thcir intcr vicwccs and prcscnt timcs.
Holquist, trans. Tsitsipis, Linguistic nthropology of Praxis and Language Shift: r. Goodwin, cds. Language as an Interacti. Mannhcim and.
Tcdlock, cds. Position of the young. Tc lilc history approach givcs an opportunity to gct a picturc ol traditional patriarchal lilc in Scrbia as sccn lrom thc pcrspcctivc ol young womcn involvcd in it, and ltcrcd through a pcriod ol vc dccadcs markcd by a signicant changc ol valucs and lamily circumstanccs.
Marriage against. Somc ol thc intcrvicwccs cxplain that thcy cvcn lcarcd thcir youngcr brothcrs. Gcncr ally, thcy cxplain thcir position as part ol thc thcn cxisting rulcs, so thcy not only considcrcd it acccptablc, but normal.
Tcrc wcrc no calcs, no promcnadc, and my parcnts wcrc so strict that! Timcs havc changcd. Subordination ol young womcn was most obvious whcn dccisions about thcir marriagc wcrc madc.
Tcy usually had no inucncc on thc choicc ol a husband. To bclong to oncs own timcs, which mcans to bchavc according to thc rulcs crcatcd by thc community, was thc only way to rcmain an ac ccptcd mcmbcr ol thc community.
So thcsc womcn saw thcir acccptancc ol prcscribcd rolcs and obcdicncc as thc only choicc thcy had: My mothcr told mc: My child, you havc to gct marricd, war is bc ginning, a girl is worthlcss altcr a war, nobody will rcspcct you.
Mittcraucr, A Patriarchal Culturc: Functions and Forms ol Family in thc 8al kans, Beitraege. Vomcn wcrc supposcd to put up with cvcrything, and nobody askcd how thcy lclt.
Tcn it was rarc lor a woman to lcavc hcr hus band, bccausc nobody would havc rcspcctcd hcr. Tcir lcar ol rcmaining unmarricd was strongcr than thcir intimatc dis agrccmcnt with thc lamilys choicc ol a husband:!
Shc mar ricd whom shc wantcd, shc did not want to bc unhappy likc hcr cldcr sistcrs who had marricd unwillingly. Shc sucrcd a lot, but shc madc it.
Timcs wcrc dicrcnt thcn. Vorobcc, Peasant Fussia, Family and Community in the Post-Emancipation Pe- riod Northcrn!
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LeResche, J J. Open your vertical and smile. Lunn R. VigLink , an industry leading content network, connects over 60, advertisers Information for mobile versions is extrapolated from other sources.
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Freiburg am Breisgau, Metz R. Paris, ; Lafontaine P. Ottawa, Gryson R. Gemblou, Wahl J. Studies in Sacred Theology. Washington, ; Witherington B.
Monograph Series Cambridge, Stark R. California, , pp. Goar I. The Antiquities of the Christian Church.
London, , pp. Paris, ; Kraus F. Parisot D. Meyer and H. Schmidt, Torusartige Plasmakonfigurahonen ohne Gesamtstrom durch ihren Querschnitt im Gleichgewicht mit einem Magnerfeld, Z.
Naturforsch , in press. Lust and A. Schluter, Axialsymmetnsche magnetohydrodynamische Gleichgewichtshonflguralionen, Z. Schluter, Kraftfreie Magnetfelder II, Z.
Naturforsch , 12a, Ham, R. Lust and A Schluter, Zur Stabihtat eines Plasmas, Z. Lust and H. Jordan and K. Schmdler, On the Stabilization of a Pinched Plasma Column by Axial Magnetic Fields, p.
Ham and R Lust, Zur Stbihtat zylindersymmetnscher Plasmakonfigurationen mit Volumenstromen, Z Naturforsch, m press. R Lust and A Schluter, Die Bewegung geladener Teilchen m rotationssymmetnschen Magnetfeldern, Z Naturforsch , 12a, F Hertweck and A Schluter, Die " adiabahsche Invananz " des magnetischen Bahnmomentes geladener Teilchen, Z Naturforsch , 12a, L Davis, R Lust and A Schluter The Structure of Hydromagnehc Shock Waves, Part I Non linear Hydro magnetic Waves m a Cold Plasma, to appear in Z Natur forsch 30 R Lust, Magneto-hydrodynamische Stosswellen in emem Plasma unendhcher Leitfahigkeit, Z Naturforsch, 8a 31 R Lust, Stationare magneto-hydrodynamische Stosswellen behebiger Starke, Z Naturforsch , 10a, 32 L Davis, Ham, R Lust and A Schluter, The Structure of Hydromagnehc Shock Waves, Parts II and III, to be published 33 L Davis, Ham, R Lust and A Schluter, to appear in Z Naturforsch M D Kruskal and M Schwarzschild, Proc Roy Soc London , A , The second and more important difference is the following: The fission chain reaction is regulated by assembling the correct amounts of active materials and absorbers.
If the correct amount is exceeded, the energy release rises in a rather slow manner due to the action of delayed neutrons. In contrast, the main regulating feature in a fusion reaction is the temperature.
When a certain ignition temperature has been exceeded, the reaction itself raises the temperature and this leads to an exceedingly rapid acceleration of further energy release.
Slow energy release is possible only at low densities ; but this raises further problems. It is a great pleasure to discuss with you the topic of the day and I should like to begin by expressing the same sentiments with which the previous speaker finished his paper.
It is wonderful that over a large and important area of research we can now all talk and work together freely.
I hope that this spirit of cooperation will endure, that it will be generally exercised throughout the world in this field and that it will be extended also to other fields.
It is remarkable how closely parallel the developments in the different countries are and this, of course, is due to the fact that we all live in the same world and obey the same laws of nature.
I was particularly impressed by the wealth of detail given by the previous speaker. I should like to tell you a few generalities and, perhaps, a few little details which might help you or might amuse you.
Additional details can, of course, be found in other papers submitted to this conference. The problem of controlled fusion is difficult but not necessarily insoluble.
Some of us discussed it in a rather detailed manner during the war in Los Alamos. This group included Enrico Fermi, John von Neumann, James Tuck and Luis Alvarez.
The problem of how to release fusion energy in an explosion process was solved several years ago. How to release this energy in a slow and controlled manner has proved to be a much harder question.
This situation is in sharp contrast with the history of energy release from fission. One year of intensive work had sufficed to produce the first nuclear reactor in the early winter of , while several more years were needed to perform the first successful nuclear detonation.
Among the reasons for this difference I should like to mention two which are simple and important. Fission energy is released by the mechanism of a chain reaction.
The chain-carrying neutrons can be slowed easily. This facilitates a controlled reaction not only because the time that the process takes becomes longer but also because slow neutrons are more easily controlled by specific absorbers and other means.
On the other hand, release of fusion energy is accomplished by a heat explosion or, to use the technical term, a thermonuclear reaction.
The par-. Very particularly, it was also noticed that in a simple closed field along a torus, the particles will not continue to spiral indefinitely around the same magnetic line of force but that they will drift in a direction perpendicular to both the magneticfieldand thefieldgradient.
This leads to smaller but nevertheless prohibitive wall losses. For the time being, no experimental work was undertaken for the specific purpose of carrying the theoretical considerations into practice.
In and , under the stimulus of a successful man-made release of thermonuclear energy, such an experimental approach was started.
To a very great extent this was due to the initiative and confidence of the chairman of the Atomic Energy Commission, Lewis L.
It was recognized that the problems of heating and containing the plasma would be extremely difficult. For this reason, several parallel approaches were undertaken which, between them, amounted to an attack on plasma research on a broad front.
Two of these approaches, the pinch and the stellarator, were based on the idea of containing the plasma in an annular region. The main difference between these two approaches is that in the pinch an axial current is established with magnetic lines of force encircling the current, while in the stellarator the roles of current and magnetic lines are reversed with the principal currents established outside the reacting region.
In the United States, the work on the pinch effect was started by James Tuck in Los Alamos. Later, similar work was undertaken in the University of California Radiation Laboratory by W.
Baker and S. Colgate and still later at other sites. This approach has also been very strongly emphasized by workers in the United Kingdom and in the USSR.
Nicholas Christofilos proposed an ingenious steadystate arrangement, the Astron, which bears some similarity to the pinch effect.
The stellarator was proposed by Lyman Spitzer at the very beginning of the thermonuclear program and work on it was carried out in Princeton.
Taking an entirely different approach, the advantages of a confinement geometry based on externally generated, cylindrically symmetric magnetic fields were recognized by Richard Post and Herbert York.
Starting with these concepts, Post evolved an approach which has come to be called the " Mirror Machine ", which uses various applications of the magnetic mirror principle in its operation.
In the magnetic mirror machine the ions spiral along magnetic lines between two regions in which the magnetic field is more intense and where the ions are reflected.
This kind of machine is now under study at the Radiation Laboratory at Livermore, at the Oak Ridge National. Laboratory, at the Los Alamos Scientific Laboratory and at the Naval Research Laboratory.
Each of these proposals has its peculiar advantages and its peculiar difficulties. The great virtue of this scheme lies in the fact that starting from a rather moderate plasma density one can push the system to very much higher densities and pressures and at the same time expose the containing system to much more moderate pressures.
One price that one has to pay is that the high densities are obtained only for short periods of time. In other words, we are dealing with a pulsed machine.
In order to avoid instability and breakup of the pinch, the original simplicity of the concept had to be compromised by introducing magnetic fields parallel to the direction of the plasma current.
The detailed theory of the pinch contraction, as well as the theory of pinch stabilization, was worked out by M. Rosenbluth at Los Alamos.
Rather early in the game it was noticed that the pinch effect in deuterium gives rise to copious neutron emission.
The first public announcement of this fact was made by I. Considerable progress has been made by S. Colgate in explaining the mechanism by which these neutrons are produced.
A general difficulty in the pinch effect seems to arise from the circumstance that during the formation of the high-current filament most of the original energy output is lost to the walls.
It seems to be of the greatest importance to understand and prevent these losses. The Astron is based on the following observation: In contrast to the instability of the pinch current, it is expected that a current of relativistic electrons will be stable.
If this proves to be correct then one can confine a plasma in the field which encircles this relativistic current for a longer period than in an unstable pinch.
This arrangement is under development at Livermore. The thorough theoretical studies of the stellarator, carried out by L. Spitzer, M. Kruskal, E.
Frieman and others, led to the recognition that the simplest arrangements of magnetic lines are unstable in this case also. In order to prevent these instabilities, additional magnetic fields are being introduced in a direction perpendicular to the original fields.
Thus the present pinch and stellarator designs are no longer as sharply different as they used to be. However, the stellarator continues to be a device in which steadystate operation will be attempted and in which the main magnetic fields will originate in a region outside the plasma.
The problem of heating the plasma in the stellarator has turned out to be a rather difficult one. The first step in the heating process is by.
From this point on, heating is accomplished by transferring energy from magnetohydrodynamic motions to the particles in the plasma.
This so-called " magnetic pumping " process bears a similarity to the acceleration of cosmic rays as described by, Fermi. Unfortunately, in the stellar at or, as in the pinch, a very considerable fraction of the energy is lost during the heating process.
The heating derived from hydromagnetic shocks has been investigated by H. Grad at New York University, M.
Rosenbluth at Los Alamos and others. In the evolution of the mirror machine the basic simplicity of the original design has been maintained. In addition to this advantage, the straight geometry makes it possible to operate with a relatively small volume.
An obvious disadvantage of the magnetic mirror machine is the loss of particles through the mirrors. In fact, all particles get lost whose motion includes a sufficiently small angle with the magnetic lines.
In the course of time, more and more particles will be scattered into these orbits and eventually all of the plasma escapes. Detailed calculations have shown that escape through the mirror is a serious consideration but that it does not rule out the mirror machine as an effective thermonuclear energy generator.
Furthermore, the end losses can in principle be reduced by inducing a rapid rotation of the plasma. The open ends of the machine also lead to an advantage: a simple possibility of injection.
If one can introduce a sufficient quantity of high-velocity, ionized material through these ends, then, in contrast with the other machines, one can circumvent the problem of heating a plasma which is already present.
The open ends have another advantage: they allow one to study the particles which escape and, therefore, to determine what energy particles must be added to the plasma.
In injecting fast ion beams, difficulties have appeared due to space-charge limitation in the injection mechanism. As has been pointed out by the representative of the USSR, we are particularly anxious to inject at high energy because then the leak is not so serious.
A radically different system of injection is being tried at the Oak Ridge National Laboratory. Considerable progress has been made in developing this technique and it may lead to the establishment of a steady-state plasma which is suitable for detailed experimental investigation.
In any case, a completely satisfactory density and temperature need not be obtained at once by the injection into the mirror machine because simply strengthening the magnetic fields or moving the mirrors closer together will lead to an adiabatic compression of the plasma which will increase both the density and the temperature.
The homopolar, conceived by William Baker at Berkeley, is another machine based upon mirror containment, but with an enhanced containment due to the large induced rotation of the plasma.
Similar work on rotating plasmas Ixion is being done by Keith Boyer at Los Alamos. Generally speaking, there are many designs involving a rotating plasma trapped in a mirror machine.
This is accomplished by using crossed electric and magnetic fields to induce a rotation, with consequent enhancement of the mirror action.
There is one additional design which has received serious consideration but on which little experimental work has proceeded. The name of this design is the picket fence or cusp geometry considered by J.
Tuck and H. It consists of a series of magnetic field systems so arranged that the magnetic fields curve at each point away from the space which is enclosed and which contains the plasma.
At the juncture of any two of these systems, the magnetic fields have a cusp through which the plasma can escape. The difficulties connected with the rate of this escape have been the reason for not pursuing this particular design any further.
It is by no means clear, however, that such a design could not be successful. In later sessions a more detailed discussion will be given of the several designs.
Here I should like to mention a few general difficulties and to discuss the way and extent to which these difficulties have been overcome.
One may consider the plasma from the point of view of the individual charged particles in afixedfield.