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<br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br />I <br /> <br />35 <br /> <br />should serve to form an embryo or droplet. Also, only one embryo or <br /> <br />droplet should form an ioe orystal. The ooourrence of ioe <br /> <br />multiplication, where one ice nucleus may produoe more than one ice <br /> <br />orystal, is not considered beoause laboratory oloud chamber conditions <br /> <br />in this stUdy are not conducive to such processes. Equations 3.2.3 and <br /> <br />3.2.4 can now be written as, <br /> <br />dC <br />::Ii _ -k'C <br />dt 1 N <br /> <br />dC <br />~ - kiCR -k2CAE <br /> <br /><3.2.6) <br /> <br />de <br />~ - k2CAE -k3C1E <br /> <br />~ <br />dt - k3CIE <br /> <br />and <br /> <br />de <br />::Ii _ -k'C <br />dt 4 H <br /> <br />dCDSD <br />dt - k.CN -k5CDSD <br /> <br /><3.2.7) <br /> <br />de <br />~ III k5CDSD -k,CFD <br /> <br />dele <br />III k'C~-- <br />dt 6 FD <br />In the experiments that follow, a final step, common to both <br /> <br />meohanisms of eq. 3.2.1 and 3.2.2, must be included. Ice nucleation is <br /> <br />monitored in this research when ice crystals have fallen to the bottom <br />of the 1 m3 ohamber. The process of fallout of the ioe crystals after <br /> <br />growth is a kinetio process that must be included in the net process. <br /> <br />This step can be expressed as <br /> <br />