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298 Chapter 6
where the subscripts refer to heavy (H), light (L), and continuous phase (C).
The drop diameter, d, for use in Equation 6.16 is difficult to determine.
There is not a single drop size but a distribution of drop sizes. Jacobs and Penny
[17] recommend a drop diameter of 150 micrometers, which is conservative and
compensates somewhat for the other assumptions in Equation 6.16.
Once the drop terminal velocity is found, the time taken for the dispersed
phase to reach the interface is given by Equation 6.15.8 in Table 6.15, and the
decanter length required for the droplets to settle is given by Equation 6.15.9. The
maximum distance that the disperse phase droplets have to travel to reach the in-
terface, which is located at the center of the separator, is D/2. The distance varies
from zero to D/2. Also, the path of the droplets is not straight down or up but will
curve because of the motion of the phases.
The length of the coalescing zone of the decanter is determined by the time
required for the dispersed phase to coalesce. Coalescence could occur by drop to
drop coalescence and drop to interface coalescence. There is no relationship that
can predict the time required for coalescence, which according to Drown and
Thomson [18] could vary from seconds to many hours. Coalescence is enhanced
when the continuous phase viscosity is small, the density difference between
phases large, the interfacial tension large, and the temperature high. Because of the
time it takes for coalescence, the dispersed phase drops accumulate near the inter-
face to form a dispersion zone. Jacobs and Penny [17] recommend that the disper-
sion zone thickness be kept to less than or equal to 10% of the decanter diameter
as given by Equation 6.15.10. Also, the drops occupy about half of the volume of
the dispersion zone volume. Neglecting the curvature of the separator, the disper-
sion zone volume is equal to H A], where H is the thickness of the dispersion
D D
zone, and AI is the area of the interface. Therefore, the residence time, IR, of the
drops in the dispersion zone is given by Equation 6.15.11. The residence time is
specified by experience, and the interfacial area required for coalescence is calcu-
lated. If it is assumed that the interface will be located at the center of the de-
canter, then the length of the coalescing zone, L D, is calculated from Equation
6.15.12. The total length of the decanter is the sum of the lengths required for set-
tling and coalescence. The procedure for calculating the dimensions of a decanter
is given in Table 6.16, and Example 6.4 illustrates the procedure.
Table 6.16 Calculation Procedure for Sizing Liquid-Liquid Separators
1. Calculate 6 to determine the dispersed phase from Equation 6.15.1 using Table
6.13.
2. Solve Equations 6.15.14, 6.15.16, 6.15.18, 6.15.20 and 6.15.22 for D L, the in-
side diameter of the decanter, assuming that the light phase determines the diame-
ter.
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