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Page Title: Integrals and Summations in Physical Systems
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Application  of  Derivatives  to  Physical  Systems
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Mathematics Volume 2 of 2
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Integrals  and  Summations  in  Physical  Systems

Higher Concepts of Mathematics CALCULUS Integrals  and  Summations  in  Physical  Systems Differentials and derivatives arose in physical systems when small changes in one quantity were considered.   For example, the relationship between position and time for a moving object led to the definition of the instantaneous velocity, as the derivative of the distance traveled with respect to  time,  ds/dt.    In  many  physical  systems,  rates  of  change  are  measured  directly.    Solving problems, when this is the case, involves another aspect of the mathematics of dynamic systems; namely integral and summations. Figure 7 is a graph of the instantaneous velocity of an object as a function of elapsed time.  This is the type of graph which could be generated if the reading of the speedometer of a car were recorded as a function of time. At any given instant of time, the velocity Figure 7    Graph of Velocity vs. Time of   the   object   can   be   determined   by referring  to  Figure  7.     However,  if  the distance  traveled  in  a  certain  interval  of time   is   to   be   determined,   some   new techniques  must  be  used.    Consider  the velocity  versus  time  curve  of  Figure  7. Let's     consider     the     velocity     changes between   times   tA   and   tB. The   first approach is to divide the time interval into three short intervals , and to (t1,t2,t3) assume that the velocity is constant during each   of   these   intervals. During   time interval    Dt1,    the    velocity    is    assumed constant at an average velocity v1; during the  interval  Dt2,  the  velocity  is  assumed constant at an average velocity v2; during time  interval  Dt3,  the velocity  is  assumed constant  at  an  average velocity  v3.   Then the  total  distance  traveled  is  approximately  the  sum  of  the  products  of  the  velocity  and  the elapsed time over each of the three intervals.   Equation 5-10 approximates the distance traveled during the time interval from ta to tb and represents the approximate area under the velocity curve during this same time interval. s = v1Dt1 + v2Dt2 + v3Dt3 (5-10) Rev. 0 Page 41 MA-05

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