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<br />----------,--------- <br /> <br />X <br />::J <br />u... <br /> <br />Q) <br />() <br />+:i <br />..... <br />o <br />Q.. <br /> <br />Q) <br />() <br /> <br />'"0 <br />Q) <br />N <br />o <br />E <br />..... <br />o <br />z <br /> <br />50 <br /> <br />40 <br /> <br />30 <br /> <br />20 <br /> <br />10 <br /> <br /> <br />.... .f <br />.. .: <br /> <br />\.... <br /> <br />o <br />o <br /> <br /> <br />W <br />I-' <br /> <br />100 <br /> <br />120 <br /> <br />40 <br /> <br />60 80 <br />Time (5) <br /> <br />20 <br /> <br />140 <br /> <br />Figure 3.4 Plot of the shape of the unit transfer function formulated <br />for the required deconvolution of ice data (see text). Also <br />shown are ice crystal numbers measured versus time <br />following one of the instantaneous nucleation ~xperiments <br />(using liquid CO in the dynamic cloud chamber) used to <br />define it. 2 <br />