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. Author manuscript; available in PMC: 2009 Feb 9.
Published in final edited form as: J Biomed Opt. 2008;13(2):024018. doi: 10.1117/1.2904952

Table 1.

Diffusion efficiencies (%) of the 1-mm-diam, 3-cm-long diffusers over axial distances of 1, 2, and 3 cm (values separated by commas)a for various nozzle-to-sample distances (D=1,2, and 3 cm), nozzle translation speeds (S=1,2, and 3 mm/s), and blasting pressures (P=10, 30, and 50 psi).

D=1 cm D=2 cm D=3 cm
S=1 mm/s
P=10 psi 39, 71, 91 (9) 12, 31, 60 (40) 5, 10, 18 (82)
P=30 psi 75, 94, 98 (2) 70, 91, 97 (3) 13, 29, 47 (53)
P=50 psi 54, 81, 90 (10) 77, 90, 94 (6) 63, 89, 96 (4)
S=2 mm/s
P=10 psi 10, 29, 62 (38) 13, 26, 41 (59) 6, 13, 23 (77)
P=30 psi 25, 55, 79 (21) 45, 73, 90 (10) 40, 68, 86 (14)
P=50 psi 39, 74, 91 (9) 67, 91, 96 (4) 61, 87, 96 (4)
S=3 mm/s
P=10 psi 17, 32, 51 (49) 13, 31, 49 (51) 1, 6, 12 (88)
P=30 psi 25, 45, 65 (35) 32, 63, 81 (19) 17, 31, 47 (53)
P=50 psi 43, 69, 82 (18) 58, 89, 98 (2) 55, 83, 94 (6)
a

The first three values represent the percentage of incident light emitted over the first 1 cm of diffuser length, the first 2 cm of diffuser length, and the entire 3 cm, respectively. The fourth value (in parentheses) represents the percentage of incident light exiting the distal end of the diffuser and is equal to the difference between the diffusion efficiency over 3 cm and 100%. For example, a perfectly uniform diffuser with a diffusion efficiency of 90% over 3 cm would have values of 30, 60, and 90% with 10% exiting the distal end.