Pease, R S

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\¥\\ ~ x xg xg x x \ \ x \\\;\ \>¥\\ > \\ \;\\\ \ \\ OCR Output/’/’ $\§§\§\§\§\\<24»?f4W / ’/Q%/22Z%%245.,, %4a /%;E N C 0 E SAZ+ Cx}40%;3*1.. (\ 0 \}g K/# / ISecretarzat : Tel. 2844.A /// {AA J"/ 5. Fusion reactor englneerlng.%"Q’’ ? ‘ 6 / /a/24 Survey of current confmcmcnt experiments. °é. __; E3. Magnetic confmement pr1nc1ples.2. High temperature matter.%%é7/ / ”y••••• 1. The basic poss1b1l1t1es. [ / c/Q/A{ABsr11Acriz/” V5/%?* ’Y >}}vv%zez¢;z<zzx%% %g/X(/%O. . PLACE : Aud1tor1{C ’ s:%e>22‘i</’ TIME : 1 1.00 hours to 12.00 hours,§//y 4/,,., 4 . , /4 ,;/,iff .-wi DATES z June 4, 5, 6, 7, 8 ,1984 E47o;j,,%iii: w;:2»2»TITLE : Fusion reactorsZ/¢·ji.·¢4 ~1» , b tf/<I1*j:2i34<if [Ty.’€>€>2Zi;<’??A SPEAKER : R. S. PEASE / Culham Laboratory9j1ljYf’fZ‘T¥3:3%%/1983 -1984 ACADEMIC TRAINING PROGRAMMETISSL|I’UFSAT00000¤4s4Z4 FK 4Vol.3, No.1 and 2, pp127—352, 1981. OCR OutputO N Jarvis, Eur.Appl.Res.Rept. - Nucl.Sci.Technol.(Crocker et al CLM~P240‘, 1970)n +’Be —> 2He + 2n + e -1.85 MeVNeutron Multiplicatorn +’Li ->‘*H€+ T + n — 2.5 MeVn +1.4 + 118 + T + 4.8 Mev6**Tritium Breedin0.25p +°Li —> "H€ + 3H€ + 3.7 MeV0.8+"B —> 3 '*H,. + 8.7 MeV@-02262+Li + H€ + H€ + 22.4 Mev‘‘*‘*0-8+3He -> "HE + p + 18.3 MeV0.1+ T + "H9 + 21*1 + 11.35.0+ T —> `°H€ + n + 17.6 MeV0.09+D —>’H+p+ 3.75 MeV0.08+ D —>”H_+ n + 3.1 MeVmax (barns)Possible for Practical Tcrrestial Thcrmonuclcar FusionD + H —>‘Hp+ Y + 5.5 MeVH+H -> D+c` +v+0.9McVSolar ReactionsFusion ReactionsTABLE 1(sas own/Aaw) paonpmd Jamcd oggoadgO Q 9 9 9 2 9 " ···· 2 23 m rv ·· Q ca m N `_ b .. ,. .- ,. Q no Ln _,_\\.O FgOCR OutputOCR OutputOCR OutputOCR OutputOCR Output\\\$1.1 OCR OutputY Li .‘t?$’fi',. .:-.-1.. 'TQLZ.1 ‘T`kmw...t jjMof temperature for the D·D and D—T fusion reactions , igvtilig-VProduct of density and energy containment time as a fungionT1 K107 10’°108 1081OiL10‘510iGD·TD·DOCR OutputOCR Output10"`t .ic>OCR Output· .. ·—<; ?$;""” " *Q too small OCR Outputrv - “Be I < 1Q toc snalln; · ug I 0.6 I ·Q I JJQ still smallcat p · 6Li I J I 5 " IOHQ t00_srnallv - "Li | 0.1 I —Q wo smallr · B" | 0.95 { ~neuzrcns Iron D-D reactionNot clean cycle since there aren — an I -· I 6 ¤ mnAviilahility of "lIe7No breedinguz n—u I - I -.2 ¤ 10Mn-¤ No breeding-, I s ¤ 1c"'n-r Tritimn breeding required• I mu - mu\t.¤¤ SEL IConvent:Fuel Cycle Hur Q I "::_£gr_?_:`zTum\.\\emission. OCR OutputCurves 2 and I5 — from the intensity of` the neutronatomsCurve I — from the spectrum of the dwarge exchangeBottom: variation of` ion temperature with timetime.Top: intensity of neutron emission as a iimction of`Ion temperature and neutron emission in Tokomak T—3Lmsec:10 Z0 30 40 50 50 70/00300z' I72,!0200N. pulses fsecOCR OutputOCR OutputOCR Output400\.\•:>Cv? 25+-90c OCR Outputand tritium.FIG. 2. Muon catalysis in a mixture of deuteriumHe + n ·•-Qu»¤u<>§’M\‘°’Sdm3 >* aceHep + nOCR OutputOCR OutputOCR OutputOCR OutputXacdA cnct xo \ IDecayFIG. 1. Resonant production of efxsu m0I1<—2cu}le2s.• d • d)~¤m—¤dlpgd O I\ .7,0Awseaa Haw'! !A5EE¥§E ru. 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Fusion reactors

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