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The power-law form of PSD (see Power-law PSD) is preserved if the latter is expressed at the logarithmic scale, i.e. as nln(D). The concentration factor, t, remains the same, but the slope changes from s to sln = s - 1. Indeed, by using Eq. 4 in Particle size distribution, we have:
| nln(D) | = n(D) D | |
| = tD -s D | ||
| = tD -(s - 1) | (2) |
If the frequency size distribution, n(D), follows a power law with a slope s, then the cumulative size distribution (see Particle size distribution), N(D), also follows a power law but with a slope S = s -1, and a concentration constant, T = t / (s - 1). Indeed, we have:
| N(D) | = ∫D∞ n(x) dx | |
| = ∫D∞ tx -s dx | ||
| = t / ( -s + 1) x -s + 1 |D∞ | ||
| = t / (s -1) D -(s - 1) | ||
| = T D -S | (3) |
Note that s must exceed 1 for the power-law approximation to the cumulative PSD to exist. This condition is easily met for natural PSDs (for example, Jonasz 1983). Also note that a power-law PSD with a slope, s > 1 must, by definition, apply to a range of the particle size that is finite at the small-size end, otherwise the total number of particles in a sample would be infinite.
| CITATION: Jonasz M. 2006. Power-law PSD: Alternate forms (www.tpdsci.com/Tpc/PsdPwLwAlt.php). In: Top. Part. Disp. Sci. (www.tpdsci.com). |
HISTORY: Published: 6-Jan-2006 Modified: 18-Jul-2006 Reviewed: PENDING |
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