{VERSION 3 0 "APPLE_68K_MAC" "3.0" } {USTYLETAB {CSTYLE "Maple Input" -1 0 "Courier" 0 1 255 0 0 1 0 1 0 0 1 0 0 0 0 }{CSTYLE "2D Math" -1 2 "Times" 0 1 0 0 0 0 0 0 2 0 0 0 0 0 0 }{CSTYLE "2D Output" 2 20 "" 0 1 0 0 255 1 0 0 0 0 0 0 0 0 0 } {CSTYLE "" -1 256 "" 0 1 0 0 0 0 0 1 0 0 0 0 0 0 0 }{PSTYLE "Normal" -1 0 1 {CSTYLE "" -1 -1 "" 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 }0 0 0 -1 -1 -1 0 0 0 0 0 0 -1 0 }{PSTYLE "Maple Output" 0 11 1 {CSTYLE "" -1 -1 " " 0 1 0 0 0 0 0 0 0 0 0 0 0 0 0 }3 3 0 -1 -1 -1 0 0 0 0 0 0 -1 0 }} {SECT 0 {EXCHG {PARA 0 "" 0 "" {TEXT -1 41 "Eric & Steven \+ Feb 24, 2000" }}{PARA 0 "" 0 "" {TEXT -1 11 "PP. 97, #12" }}{PARA 0 "" 0 "" {TEXT -1 0 "" }}}{EXCHG {PARA 0 "> " 0 "" {MPLTEXT 1 0 8 "re start:" }}}{EXCHG {PARA 0 "" 0 "" {TEXT -1 435 "A shell of mass m = 2 \+ kg is shot straight up at initial velocity v = 200 m/s from the groun d. Our task is to determine the time this shell reaches it's maximum \+ height, and what that height may be. We assigned ground level as x = \+ 0, and upwards as the postive x direction. Two forces act in the oppo site direction, the force due to air resistance and gravity. Since we are only concerned with the trip up, we my consider the force " }} {PARA 0 "" 0 "" {TEXT -1 199 "m * dv/dt (or dp/dt) to be positive, and air resistance k * v and gravity m * g to be negative. As we know t he shell will lose velocity, that dp/dt will be negative, this intuiti vely makes sense. " }}{PARA 0 "" 0 "" {TEXT -1 82 " \+ m * dv/dt = -k * v - mg" }} {PARA 0 "" 0 "" {TEXT -1 43 "Plugging the known constants, this become s:" }}{PARA 0 "" 0 "" {TEXT -1 90 " \+ 2 * dv/dt = -.05 * v - 2 * 9.81" }}{PARA 0 "" 0 "" {TEXT -1 124 "Recognizing this as a seperable equation, and using the initial condition v = 200 at time t = 0, we arrived at the equati on:" }}{PARA 0 "" 0 "" {TEXT -1 100 " \+ v(t) = 20 * (29.62 * e ^ (-t/40) - 19.62)" } }{PARA 0 "" 0 "" {TEXT -1 72 "To check on Maple we isolate the dv/dt b y dividing through by 2 and get:" }}}{EXCHG {PARA 0 "> " 0 "" {MPLTEXT 1 0 70 "v:=unapply(rhs(dsolve(\{diff(v(t),t)=-9.81-v(t)/40,v( 0)=200\},v(t))),t);" }}{PARA 11 "" 1 "" {XPPMATH 20 "6#>%\"vGR6#%\"tG6 \"6$%)operatorG%&arrowGF(,&$!++++CR!\"(\"\"\"-%$expG6#,$9$#!\"\"\"#S$ \"++++CfF/F(F(F(" }}}{EXCHG {PARA 0 "" 0 "" {TEXT -1 94 "This is the s ame answer with the 20 distributed. Next we ask Maple when the veloci ty is zero." }}}{EXCHG {PARA 0 "> " 0 "" {MPLTEXT 1 0 16 "solve(v(t)=0 ,t);" }}{PARA 11 "" 1 "" {XPPMATH 20 "6#$\"+>9gZ;!\")" }}}{EXCHG {PARA 0 "" 0 "" {TEXT -1 113 "To find the height at this point, we mus t integrate the velocity function to get a function in terms of distan ce." }}}{EXCHG {PARA 0 "> " 0 "" {MPLTEXT 1 0 37 "x:=unapply(\{int(v(t ),t)+c,x(0)=0\},t);" }}{PARA 11 "" 1 "" {XPPMATH 20 "6#>%\"xGR6#%\"tG6 \"6$%)operatorG%&arrowGF(<$,(9$$!++++CR!\"(-%$expG6#,$F.$!+++++D!#6$!& 'pB\"\"!%\"cG\"\"\"/-F$6#F;F;F(F(F(" }}}{EXCHG {PARA 0 "" 0 "" {TEXT -1 79 "We know that at time t = 0, x(t) = 0, so c = 23696. This match es our solution." }}}{EXCHG {PARA 0 "" 0 "" {TEXT -1 59 "To complete t he problem, we must find x when t = 16.48 sec." }}}{EXCHG {PARA 0 "> \+ " 0 "" {MPLTEXT 1 0 38 "x1:=t->23696-392.4*t-23696*exp(-t/40);" }} {PARA 11 "" 1 "" {XPPMATH 20 "6#>%#x1GR6#%\"tG6\"6$%)operatorG%&arrowG F(,(\"&'pB\"\"\"9$$!%CR!\"\"-%$expG6#,$F/#F2\"#S!&'pBF(F(F(" }}} {EXCHG {PARA 0 "> " 0 "" {MPLTEXT 1 0 10 "x1(16.48);" }}{PARA 11 "" 1 "" {XPPMATH 20 "6#$\"*&>\"[`\"!\"&" }}}{EXCHG {PARA 0 "" 0 "" {TEXT -1 213 "Sadly, in over an hour of Maple expirimentation, we could not \+ figure out how to get Maple to give us the x value for t = 16.48 sec. \+ On a calculator, this simple plugging in of numbers gives x(16.48) = 1534.8m." }{TEXT 256 62 "Dr. Sarah's comment - I put in x1(16.48) w hich does the trick!" }}}{EXCHG {PARA 0 "> " 0 "" {MPLTEXT 1 0 0 "" }} }}{MARK "0 1 0" 11 }{VIEWOPTS 1 1 0 1 1 1803 }