The power balance of a thermonuclear plasma in the DD fusion reactor is discussed by taking account of the losses of 1) the thermal conduction and 2) the bremsstrahlung. The spatial dependence of the plasma temperature in the “Pure DD” and “Catalyzed DD” fusion reactors are obtained.
The power balance of a thermonuclear cylindrical plasma is discussed by taking account of the losses of the thermal conduction and the bremsstrahlung under the assumptions that 1) the number density is constant (n=const.) and 2) the number density is proportional to the temperature (n-T). The temperature profile is obtained in the case that the temperature at the center of the plasma is equal to 100 keV and the strength of the magnetic field 100kG.
The power balance of a thermonuclear plasma is discussed by taking into account of the losses of the thermal conduction and the bremsstrahlung under the assumption that the pressure of the plasma is constant (nT=const.). The temperature profile is obtained in the case that the temperature at the center of the plasma is equal to 100 keV and the strength of the magnetic field 100kG.
In order to describe a steady state of a thermonuclear cylindrical plasma, the two-component theory is used. The spatial dependence of the plasma temperature, the number density, the plasma pressure and the strength of the magnetic field are obtained.