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Air velocity profiles as those shown in Fig. 3(c) were specified at the nozzle orifice, which corresponds to an internal boundary. Along the x-direction these profiles were uniform over the length lx’ of the flat hollow portion of the flanged orifice, in the rest of the orifice the profiles decreased to zero varying in angle from 0 dig to dig at the edge; the distributions were the same throughout the whole thickness (y-)direction of the orifice.
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These velocity profiles were suggested by the geometry of the flanged orifice and are supported by the results presented in Section 4. The expressions describing the profiles are listed in Table 1, together with the expressions for the turbulence kinetic energy and the dissipation rate of turbulence kinetic energy at this boundary, ko and o, respectively.
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To do this, the orifice was simulated as a grid of ports, k, releasing drops satisfying the diameter distribution measured at z= as (according with the assumption indicated in Section 3.1) for the particular set of nozzle operating conditions under consideration. For deciding the number of ports assigned to each drop size category situations there may be no mode in a simple series where no value occurs more than once.
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The modal size of all clothing is the size which the businessman must stock in the greatest quantity and variety in comparison with other sizes. Indeed, in most inventory (stock level) problems, one needs the mode more often than any other measure of central tendency.
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