{VERSION 2 3 "IBM INTEL NT" "2.3" } {USTYLETAB {CSTYLE "Maple Input" -1 0 "Courier" 0 1 255 0 0 1 0 1 0 0 1 0 0 0 0 }{PSTYLE "Normal" -1 0 1 {CSTYLE "" -1 -1 "Times" 1 12 0 0 0 1 2 2 2 0 0 0 0 0 0 }0 0 0 -1 -1 -1 0 0 0 0 0 0 -1 0 }{PSTYLE "R3 Fo nt 0" -1 256 1 {CSTYLE "" -1 -1 "Helvetica" 1 10 255 0 0 1 2 1 2 0 0 0 0 0 0 }0 0 0 -1 -1 -1 0 0 0 0 0 0 -1 0 }{PSTYLE "R3 Font 2" -1 257 1 {CSTYLE "" -1 -1 "Courier" 1 8 0 0 0 1 2 2 2 0 0 0 0 0 0 }0 0 0 -1 -1 -1 0 0 0 0 0 0 -1 0 }} {SECT 0 {EXCHG {PARA 0 "" 0 "" {TEXT -1 18 "piano.mws 8/24/95" }} {PARA 0 "" 0 "" {TEXT -1 336 "This is a problem of dispersion of sound waves on a piano wire.The dispersion relation of the piano wire is: ( omega)^2/(k)^2=T/mu+alpha*(k^2), where omega is the angular frequency, k the wave vector, T the tension of the string, and alpha a small con stant value. Let us take several individual waves and observe the wave group behavior." }}{PARA 0 "" 0 "" {TEXT -1 0 "" }}{PARA 0 "" 0 "" {TEXT -1 84 "The small individual 'phase' peaks move forward through t he envelope or 'group peak." }}{PARA 0 "" 0 "" {TEXT -1 0 "" }}{PARA 0 "> " 0 "" {MPLTEXT 1 0 8 "restart;" }}}{EXCHG {PARA 0 "> " 0 "" {MPLTEXT 1 0 12 "with(plots):" }}}{EXCHG {PARA 0 "> " 0 "" {MPLTEXT 1 0 32 "d:=omega^2/k^2=T/(mu)+alpha*k^2;" }}}{EXCHG {PARA 0 "> " 0 "" {MPLTEXT 1 0 18 "for n from 0 to 10" }}{PARA 0 "> " 0 "" {MPLTEXT 1 0 2 "do" }}{PARA 0 "> " 0 "" {MPLTEXT 1 0 40 "y.n:=sin((k+n*k1)*x-(omega +n*omega1)*t);" }}{PARA 0 "> " 0 "" {MPLTEXT 1 0 3 "od;" }}}{EXCHG {PARA 0 "> " 0 "" {MPLTEXT 1 0 45 "psi:=simplify(convert(\{y.(0..10)\} ,`+`),trig);" }}}{EXCHG {PARA 0 "> " 0 "" {MPLTEXT 1 0 20 "sol:=solve( d,omega);" }}}{EXCHG {PARA 0 "> " 0 "" {MPLTEXT 1 0 25 "v[p]:=simplify (sol[1]/k);" }}}{EXCHG {PARA 0 "> " 0 "" {MPLTEXT 1 0 27 "vg:=diff(v[p ],k)=omega1/k1;" }}}{EXCHG {PARA 0 "> " 0 "" {MPLTEXT 1 0 22 "vgr:=sol ve(vg,omega1);" }}}{EXCHG {PARA 0 "> " 0 "" {MPLTEXT 1 0 29 "vphase_ov er_vgroup:=v[p]/vgr;" }}}{EXCHG {PARA 0 "> " 0 "" {MPLTEXT 1 0 57 "psi fin:=subs(\{omega1=solve(vg,omega1),omega=sol[1]\},psi);" }}}{EXCHG {PARA 0 "> " 0 "" {MPLTEXT 1 0 46 "values:=\{k=5,k1=5/10,alpha=2/10,T= 3,mu=1/100\};" }}}{EXCHG {PARA 0 "> " 0 "" {MPLTEXT 1 0 23 "m:=subs(va lues,psifin);" }}}{EXCHG {PARA 0 "> " 0 "" {MPLTEXT 1 0 113 "animate(m ,x=10..20,t=0..0.2,color=blue,frames=20,numpoints=100); # the small pe aks move forward thru the envelope" }}}{EXCHG {PARA 0 "" 0 "" {TEXT -1 99 "The individual peaks come up and move through the 'envelope' or 'group' peak, showing vphase>vgroup" }}{PARA 0 "> " 0 "" {MPLTEXT 1 0 35 "vgval:=evalf(subs(values,lhs(vg)));" }}}{EXCHG {PARA 0 "> " 0 " " {MPLTEXT 1 0 32 "vpval:=evalf(subs(values,v[p]));" }}}{EXCHG {PARA 0 "> " 0 "" {MPLTEXT 1 0 19 "ratio:=vpval/vgval;" }}}}{MARK "0 0 0" 18 }{VIEWOPTS 1 1 0 1 1 1803 }