altitudes = 150:10:800; % km dens_jb = zeros(size(altitudes)); dens_msis = zeros(size(altitudes)); for i = 1:length(altitudes) dens_jb(i) = jb2008(altitudes(i), 0, 0, 80, 43200, 180, 170, 15, -20); dens_msis(i) = atmosnrlmsise00(altitudes(i)*1000, 0, 0, 80, 43200, 180, 170, 15); end
– Compare your MATLAB outputs against the official CIRA-2012 reference tables. Off-by errors in the exospheric temperature equation are common in amateur translations. Beyond JB2008: What Comes Next? JB2008 remains the gold standard for operational drag modeling, but it is empirical—it fits historical data rather than simulating physics. Newer models like HASDM (High Accuracy Satellite Drag Model) and TIEGCM (thermosphere-ionosphere GCM) offer higher fidelity, but they require supercomputing resources. jb2008 matlab
– The full JB2008 includes iterative temperature solutions. For Monte Carlo simulations (thousands of orbits), precompute lookup tables or use a polynomial surrogate model. JB2008 remains the gold standard for operational drag
% Date: March 23, 2024 (geomagnetic storm day) doy = 83; ut_sec = 14*3600; % 14:00 UTC lat = 35; lon = -120; alt = 450e3; % Over California % Solar & geomagnetic indices (real values from SWPC) f10 = 158.2; % Daily solar flux f10b = 145.3; % 81-day mean ap = 48; % Active geomagnetic dst = -78; % Moderate storm ut_sec = 14*3600
semilogy(altitudes, dens_jb, 'b-', 'LineWidth', 2); hold on; semilogy(altitudes, dens_msis, 'r--', 'LineWidth', 2); xlabel('Altitude (km)'); ylabel('Density (kg/m³)'); title('JB2008 vs. MSISE-00: Solar Maximum Conditions'); legend('JB2008', 'MSISE-00'); grid on;