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<br />--( <br />, <br />-~ <br />-----, <br />-----.i <br />-, <br /> <br /> '\ <br />@ \ <br /> ~ <br /> S <br /> (I) 1 (3) tI <br /> - <br /> ~ G- <br /> Lob Rob 'tI <br /> ~ 0 <br /> 'tI 0 <br /> - <br /> 0 ... <br /> 0 ~ ... <br /> - <br /> .. 0 <br /> ... 1 = <br /> 0 E <br /> .. ~ <br /> ... ..J <br /> ~ <br /> -.J <br /> L3 <br /> n3 <br />CD <br /> <br /> <br />@ <br /> <br /> <br />CD <br /> <br />5.02 Distribution of reach lenllthl and n-values <br /> <br />The strips subdivide the cross sections into portions called <br />subsections. These subsections form the basic framework from which <br /> <br />distributed properties are converted to averages for use in the energy <br /> <br /> <br />equation. In the general case, three strips or subsections are not <br /> <br />5.05 <br />