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8

Segment response tex2html_wrap_inline729 (Eq. ) -

There are two ways of looking at this equation. First, it basically just states Newton's law, tex2html_wrap_inline1157 : on each segment two tension forces pull along y in opposite directions (hence the derivative), tex2html_wrap_inline861 measures the mass of the segment and tex2html_wrap_inline1163 is the acceleration. Another way is to rewrite it as tex2html_wrap_inline1165 , which says that the acceleration of each segment is in direct proportion to the rate of change in the y-component of the tension and in inverse proportion to the mass per unit length tex2html_wrap_inline861 . The inverse proportion to tex2html_wrap_inline861 comes directly from Newton's law F=ma. The smaller the mass of each segment the more acceleration tex2html_wrap_inline1163 we expect. The proportionality to the derivative tex2html_wrap_inline915 comes from the fact that tension pulls in opposite directions on the ends of each segment (Figure 2). If the tension in the y-direction were constant, then the two tensions would cancel and the segment would not accelerate. The greater the rate of change of the tension tex2html_wrap_inline915 , the greater the difference in tension on the two sides of a segment and the greater its acceleration. Thus, we do expect the acceleration tex2html_wrap_inline1163 to be in direct proportion to tex2html_wrap_inline915 .



Tomas Arias
Mon Oct 15 16:15:07 EDT 2001