rho=200^(1/32);
bins(:,1) = 1.25*rho.^([0:31]); %lower limit for type B
bins(:,2) = 1.25*rho.^([1:32]); % upper limit for type B
bins(:,3) = sqrt(bins(:,1).*bins(:,2));%mid-point for type B

bins(:,4) = 2.5*rho.^([0:31]); %lower limit for type C
bins(:,5) = 2.5*rho.^([1:32]); % upper limit for type C
bins(:,6) = sqrt(bins(:,4).*bins(:,5));%mid-point for type C

bins(:,7) = 7.5*rho.^([0:31]); %lower limit for type FLOC
bins(:,8) = 7.5*rho.^([1:32]); %upper limit for type FLOC
bins(:,9) = sqrt(bins(:,7).*bins(:,8));%mid-point for type FLOC

rho=100^(1/32);
bins(:,10) = 5*rho.^([0:31]); %lower limit for type A
bins(:,11) = 5*rho.^([1:32]); % upper limit for type A
bins(:,12) = sqrt(bins(:,10).*bins(:,11));%mid-point for type A

rhoST=200^(1/8);

binST(:,1) = 1.25*rhoST.^([0:7]); %lower limit for LISST-ST type B
binST(:,2) = 1.25*rhoST.^([1:8]); %upper limit for LISST-ST type B
binST(:,3) = sqrt(binST(:,1).*binST(:,2));%mid-point for LISST-ST type B

binST(:,4) = 2.5*rhoST.^([0:7]); %lower limit for LISST-ST type C
binST(:,5) = 2.5*rhoST.^([1:8]); %upper limit for LISST-ST type C
binST(:,6) = sqrt(binST(:,4).*binST(:,5));%mid-point for LISST-ST type C

The tables below tabulate the values computed using the script above. NOTE: The table below is ONLY valid for inversions that have used the matrices based on scattering off of spherical particles. For inversions based on scattering from randomly shaped particles, use the table in this article.

If you are looking for the LISST-100X scattering angles, click here for the angles IN AIR or click here for the angles in WATER.