Rezultati sastava vodonicno-helijumske plazme pri razlicitim
vrednostima pritiska (, , ) i razlicitim
vrednostima procentnog sastava su predstavljeni u tabelama
5.16, 5.17,
5.18 strana .
U kolonama su predstavljene koncentracije elektrona,
atoma, jona vodonika i atoma,
jona helijuma.
Sa grafika 5.11, 5.12, 5.13, strana se moze videti da je pri temperaturama do koncentracija dvostruko jonizovanih atoma helijuma zanemarljiva. Tako oni nisu predstavljeni u tabelama 5.16, 5.17, 5.18 i nisu uzeti u razmatranje transportnih osobina guste i neidealne plazme. Pri niskim temperaturama plazme preovladjuju neutralne komponente. Odnos koncentracije atoma vodonika u odnosu na atome helijuma pre svega zavise od njihovog procentnog sastava u posmatranoj plazmi. Takodje pri procentnom sastavu videti grafik 5.12 strana moze se primetiti da su koncentracije atoma helijuma primetne do temperature , za razliku od atoma vodonika koji su prisutni do temperature , što je razumljivo jer energija jonizacije atoma helijuma je veca od energije jonizacije vodonika. Pri višim temperaturama preovladjuju jonske komponente plazme i to u medjusobnom odnosu zavisnom od procentnog sastava.
T(K) | ||||
.856733E+16 | .111257E+17 | .132070E+17 | ||
.209081E+18 | .350343E+18 | .491386E+18 | ||
10000 | .856710E+16 | .111256E+17 | .132069E+17 | |
.507846E+18 | .361468E+18 | .216254E+18 | ||
.237904E+12 | .130802E+12 | .660735E+11 | ||
.102326E+18 | .126652E+18 | .148435E+18 | ||
.458152E+16 | .841812E+16 | .116582E+17 | ||
20000 | .748301E+17 | .111771E+18 | .141359E+18 | |
.157798E+18 | .105309E+18 | .585031E+17 | ||
.274959E+17 | .148810E+17 | .707576E+16 | ||
.119870E+18 | .120191E+18 | .120511E+18 | ||
.811740E+15 | .135290E+16 | .189403E+16 | ||
30000 | .366334E+17 | .608956E+17 | .850297E+17 | |
.414149E+16 | .295807E+16 | .177473E+16 | ||
.832240E+17 | .592858E+17 | .354755E+17 |
T(K) | ||||
.196607E+17 | .255335E+17 | .303297E+17 | ||
.107553E+19 | .179686E+19 | .251760E+19 | ||
10000 | .196601E+17 | .255332E+17 | .303296E+17 | |
.255545E+19 | .182239E+19 | .109197E+19 | ||
.527708E+12 | .291147E+12 | .147378E+12 | ||
.405732E+18 | .545059E+18 | .659751E+18 | ||
.664338E+17 | .121204E+18 | .172731E+18 | ||
20000 | .362393E+18 | .523844E+18 | .650053E+18 | |
.957258E+18 | .623834E+18 | .342923E+18 | ||
.433391E+17 | .212148E+17 | .969824E+16 | ||
.574188E+18 | .581468E+18 | .588738E+18 | ||
.726372E+16 | .121113E+17 | .169582E+17 | ||
30000 | .187511E+18 | .308874E+18 | .427332E+18 | |
.678044E+17 | .483951E+17 | .290071E+17 | ||
.386664E+18 | .272585E+18 | .161400E+18 |
T(K) | ||||
.280852E+17 | .364964E+17 | .433770E+17 | ||
.216558E+19 | .361555E+19 | .506469E+19 | ||
10000 | .280844E+17 | .364960E+17 | .433768E+17 | |
.511856E+19 | .365204E+19 | .218917E+19 | ||
.744856E+12 | .411295E+12 | .208305E+12 | ||
.732823E+18 | .996746E+18 | .120481E+19 | ||
.199665E+18 | .364995E+18 | .532602E+18 | ||
20000 | .681582E+18 | .971789E+18 | .119325E+19 | |
.200500E+19 | .131183E+19 | .728094E+18 | ||
.512412E+17 | .249568E+17 | .115573E+17 | ||
.110176E+19 | .112744E+19 | .115303E+19 | ||
.193758E+17 | .323437E+17 | .453122E+17 | ||
30000 | .384160E+18 | .627372E+18 | .860377E+18 | |
.223996E+18 | .159646E+18 | .954970E+17 | ||
.717582E+18 | .500065E+18 | .292653E+18 |