function result = Mie_rain5(fGHz, R, nrain) % Extinction, scattering, absorption, backscattering and % asymmetric scattering coefficients in 1/km versus Temperature, % for Marshall-Palmer (MP) drop-size distribution % see Sauvageot et al. (1992), % using Mie Theory, Input: % fGHz: frequency in GHz, TK: Temp. in K, % nrain: Number of temperatrures % C. Mätzler, June 2002. Tmin=270; nsteps=501; N0=0.08/10000; % original MP N0 in 1/mm^4 TK=Tmin; nx=(1:nsteps)'; c0=299.793; for jr = 1:nrain TK=TK+1; m=sqrt(epswater(fGHz, TK)); dD=0.01*R^(1/6)/fGHz^0.05; D=(nx-1)*dD; x=pi*D*fGHz/c0; sigmag=pi*D.*D/4; LA=4.1/R^0.21; NMP=N0*exp(-LA*D); sn=sigmag.*NMP*1000000; for j = 1:nsteps a(j,:)=Mie(m,x(j)); end; b(:,1)=D; b(:,2)=a(:,1).*sn; b(:,3)=a(:,2).*sn; b(:,4)=a(:,3).*sn; b(:,5)=a(:,4).*sn; b(:,6)=a(:,2).*a(:,5).*sn; gext= sum(b(:,2))*dD; gsca= sum(b(:,3))*dD; gabs= sum(b(:,4))*dD; gb= sum(b(:,5))*dD; gteta=sum(b(:,6))*dD; res(jr,:)=[TK gext gsca gabs gb gteta]; end; output_parameters='Gext, Gsca, Gabs, Gb, Gsca*' plot(res(:,1),res(:,2:6)) legend('Gext','Gsca','Gabs','Gb','Gsca*') title(sprintf(' Propagation Coef. vs. Temperature at f=%gGHz, R=%gmm/h',fGHz,R)) xlabel('T (K)'); ylabel('Gi(1/km)') result=res;