wang jin-shan, zhu yu-qun, jiang chao. Fuel components in ICF targets at vapor-liquid equilibrium phase[J]. High Power Laser and Particle Beams, 2005, 17.
Citation:
wang jin-shan, zhu yu-qun, jiang chao. Fuel components in ICF targets at vapor-liquid equilibrium phase[J]. High Power Laser and Particle Beams, 2005, 17.
wang jin-shan, zhu yu-qun, jiang chao. Fuel components in ICF targets at vapor-liquid equilibrium phase[J]. High Power Laser and Particle Beams, 2005, 17.
Citation:
wang jin-shan, zhu yu-qun, jiang chao. Fuel components in ICF targets at vapor-liquid equilibrium phase[J]. High Power Laser and Particle Beams, 2005, 17.
According to Raoult's law and Dalton's partial-pressure laws, the mixture of D2, T2 and DT fuel components in the proportion of 3∶3∶4 in an ICF target is analyzed on the basis of mass conservation, under the vapor-liquid equilibrium phase at several work temperatures (22, 24, 26, 28 and 30 K).The result is that at 22 K, with filling pressure increasing from 1 MPa to 5 MPa, the mole fraction of D2 increases from 0.251 to 0.290, the mole fraction of T2 decreases from 0.350 to 0.310 in the liquid fuel, and the mole fraction of D2 increases from 0.322 to 0.365, the mole fraction of T2 decreases from 0.278 to 0.241 in the gas fuel. When filling pressure is 5 MPa, with work temperature increasing from 22 K to 30 K, the mole fraction of D2 decreases from 0.290 to 0.261, the mole fraction of T2