diff --git a/plasmaExpansion.f90 b/plasmaExpansion.f90 index f715510..896629d 100644 --- a/plasmaExpansion.f90 +++ b/plasmaExpansion.f90 @@ -35,7 +35,7 @@ program plasmaExpansion real(dp), parameter:: m_i = 1.9712258e-25_dp ! Tin atom mass in kg real(dp), parameter:: gamma_i = 1.0_dp ! Adiabatic coefficient for ions real(dp), parameter:: m_e = 9.1093837e-31_dp ! Electron mass in kg - real(dp), parameter:: gamma_e = 2.0_dp ! Adiabatic coefficient for electrons + real(dp), parameter:: gamma_e = 4.0_dp / 3.0_dp ! Adiabatic coefficient for electrons real(dp):: r0, rf real(dp), allocatable, dimension(:):: r @@ -285,9 +285,9 @@ program plasmaExpansion phi_old = phi ! Diagonal matrix for Newton integration scheme - db_dphi = n_e / T_e ! Isotropic - ! db_dphi = Zave(1) * n_i(1) / (gamma_e * T_e) * & - ! (1.0_dp + ((gamma_e - 1.0_dp)/gamma_e*(phi_old-phi0)/T_e)**((2.0_dp - gamma_e)/(gamma_e - 1.0_dp))) ! Polytropic + ! db_dphi = n_e / T_e ! Isotropic + db_dphi = Zave(1) * n_i(1) / (gamma_e * T_e) * & + (1.0_dp + (gamma_e - 1.0_dp)/gamma_e*(phi_old-phi0)/T_e)**((2.0_dp - gamma_e)/(gamma_e - 1.0_dp)) ! Polytropic diag = -2.0_dp / dr**2 - db_dphi diag_low = 1.0_dp / dr**2 - 1.0_dp / (r(2:nr) * dr) diag_high = 1.0_dp / dr**2 + 1.0_dp / (r(1:nr-1) * dr) @@ -314,8 +314,8 @@ program plasmaExpansion ! phi0=phi(1) ! Neumann ! Calculate distribution of electrons - n_e = Zave(1) * n_i(1) * exp((phi- phi0) / T_e) ! Isothermal (Boltzmann) - ! n_e = Zave(1) * n_i(1) * (1.0_dp + ((gamma_e - 1.0_dp)/gamma_e*(phi-phi0)/T_e)**(1.0_dp/(gamma_e - 1.0_dp))) ! Polytropic + ! n_e = Zave(1) * n_i(1) * exp((phi- phi0) / T_e) ! Isothermal (Boltzmann) + n_e = Zave(1) * n_i(1) * (1.0_dp + (gamma_e - 1.0_dp)/gamma_e*(phi-phi0)/T_e)**(1.0_dp/(gamma_e - 1.0_dp)) ! Polytropic ! Check if the solution has converged phiConv = maxval(abs(Res),1)