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<br />. <br /> <br />28 <br /> <br />. <br /> <br />tends to generate more crystals in the jug, and, thus, enhances the <br />competition at lower temperatures. This effectively stops the crystal growth <br />associated with the seeding technique and competition before injecting the <br />crystals into the suspension chamber, but the crystal size is not necessarily the <br />same every time although uncertainty arising from this factor may not be <br />large. However, the importance of this uncertainty rapidly decreases as the <br />growth time increases. Thus, time as well as temperature can be factors that <br />affect the starting time to some extent. <br />The sensitivity of temperature on the measured quantities, mass, <br />dimensions and fall velocity, has significant implications on the certainty of <br />the results. Mass and axial ratio can have a particularly large variation with <br />small temperature changes; temperature changes as small as lOC can double <br />the magnitude of these quantities, which will be shown in temperature plots <br />later in this thesis. Thus, temperature sensitivity can account for a large part <br />of the differences between the results from. each experimental study. <br />In summary, the chronological order of the performed experiments, the <br />time after seeding, the ambient or fog temperature and temperature <br />sensitivity are important factors in estimating the experimental uncertainties <br />and reliability of each data set to be used in this thesis. These factors in <br />addition to those discussed in the first part of this chapter can help resolve <br />some of the internal and external inconsistencies of each data set. Thus, <br />despite some drawbacks, these data sets will be useful in this thesis. <br /> <br />. <br /> <br />. <br /> <br />. <br /> <br />. <br /> <br />. <br /> <br />. <br /> <br />. <br /> <br />. <br /> <br />. <br />