Postupak racunanja sastava plazme vodonika je detaljno opisan u dodatak
(C) strana .
Rezultati izracunavanja sastava su predstavljeni u tabelama (5.1),
(5.2), (5.3) za razlicite vrednosti
pritiska plazme. U odgovarajucim kolonama su prikazane, temperatura,
koncentracija elektrona , koncentracija atoma i jona .
5000.0 | .493176E+13 | .146874E+19 | .493176E+13 |
10000.0 | .158323E+17 | .702396E+18 | .158323E+17 |
15000.0 | .153093E+18 | .183188E+18 | .153093E+18 |
20000.0 | .175496E+18 | .160392E+17 | .175496E+18 |
25000.0 | .144562E+18 | .450200E+16 | .144562E+18 |
30000.0 | .120991E+18 | .270563E+16 | .120991E+18 |
35000.0 | .103984E+18 | .176461E+16 | .103984E+18 |
40000.0 | .911258E+17 | .126404E+16 | .911258E+17 |
5000.0 | .110443E+14 | .735462E+19 | .110443E+14 |
10000.0 | .364027E+17 | .359749E+19 | .364027E+17 |
15000.0 | .462443E+18 | .152199E+19 | .462443E+18 |
20000.0 | .792714E+18 | .249729E+18 | .792714E+18 |
25000.0 | .707231E+18 | .536626E+17 | .707231E+18 |
30000.0 | .599610E+18 | .242183E+17 | .599610E+18 |
35000.0 | .516581E+18 | .154983E+17 | .516581E+18 |
40000.0 | .454072E+18 | .943375E+16 | .454072E+18 |
5000.0 | .156430E+14 | .147416E+20 | .156430E+14 |
10000.0 | .521019E+17 | .723642E+19 | .521019E+17 |
15000.0 | .714182E+18 | .346539E+19 | .714182E+18 |
20000.0 | .145934E+19 | .751643E+18 | .145934E+19 |
25000.0 | .138921E+19 | .157833E+18 | .138921E+19 |
30000.0 | .119109E+19 | .646938E+17 | .119109E+19 |
35000.0 | .103235E+19 | .326214E+17 | .103235E+19 |
40000.0 | .905548E+18 | .240597E+17 | .905548E+18 |
Na grafiku (5.1) je predstavljen odnos elektronske,
jonske i atomske komponente plazme u odnosu na ukupan
broj cestica
u funkciji temperature ,
pri datom pritisku.
Primecuje se da atomska komponenta preovladjuje do temperature priblizno . Pri temperaturi od u plazmi vodonika skoro potpuno preovladjuju elektronska tj. jonska komponenta u odnosu na atomsku. Plazma je skoro potpuno jonizovana.