163
.
10 .
10
2
10
0
10
10
-,
-,
10
-.
10 -.
10
1 0 - 6 U_ .-1llJLlllL~_ ,ilJjlllL_L.WlJJJLUlJWllL--"-1JJlllILlJiLWJL~Wllll--:-LLW""-;~WllL--:-'~, 0 •
1 0
1 0
1 0
Figure 7. A) Side Scatter (SS) and near-forward scatter (FS) for spherical particles with increasing size
parameter a (abcissae) and for two values of the refraction index (real, 1.01 and 1.07 respectively). The
units for SS and FS are m·! sr·! (but see remark in the legend of Fig. 4); B) SS plotted versus FS for
various a values, as indicated. Each rod corresponds to a given a-value and a varying index of
refraction (between 1.03 and 1.06). Note that the diameter d (in J.(m) is numerically equal to a if A is
supposed to be 0.421 /Lm.
.
10 .
10
2
10
0
10
10
-,
-,
10
-.
10 -.
10
1 0 - 6 U_ .-1llJLlllL~_ ,ilJjlllL_L.WlJJJLUlJWllL--"-1JJlllILlJiLWJL~Wllll--:-LLW""-;~WllL--:-'~, 0 •
1 0
1 0
1 0
Figure 7. A) Side Scatter (SS) and near-forward scatter (FS) for spherical particles with increasing size
parameter a (abcissae) and for two values of the refraction index (real, 1.01 and 1.07 respectively). The
units for SS and FS are m·! sr·! (but see remark in the legend of Fig. 4); B) SS plotted versus FS for
various a values, as indicated. Each rod corresponds to a given a-value and a varying index of
refraction (between 1.03 and 1.06). Note that the diameter d (in J.(m) is numerically equal to a if A is
supposed to be 0.421 /Lm.