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0 0 0 0 0 0 -1 0 }{PSTYLE "" 0 317 1 {CSTYLE " " -1 -1 "" 1 14 0 0 0 0 0 0 0 0 0 0 0 0 0 1 }0 0 0 -1 -1 -1 0 0 0 0 0 0 -1 0 }{PSTYLE "" 0 318 1 {CSTYLE "" -1 -1 "" 1 14 0 0 0 0 0 0 0 0 0 0 0 0 0 1 }0 0 0 -1 -1 -1 0 0 0 0 0 0 -1 0 }{PSTYLE "" 0 319 1 {CSTYLE "" -1 -1 "" 1 14 0 0 0 0 0 0 0 0 0 0 0 0 0 1 }0 0 0 -1 -1 -1 0 0 0 0 0 0 -1 0 }{PSTYLE "" 0 320 1 {CSTYLE "" -1 -1 "" 1 14 0 0 0 0 0 0 0 0 0 0 0 0 0 1 }0 0 0 -1 -1 -1 0 0 0 0 0 0 -1 0 }{PSTYLE "" 0 321 1 {CSTYLE "" -1 -1 "" 1 14 0 0 0 0 0 0 0 0 0 0 0 0 0 1 }0 0 0 -1 -1 -1 0 0 0 0 0 0 -1 0 }{PSTYLE "" 0 322 1 {CSTYLE "" -1 -1 "" 1 14 0 0 0 0 0 0 0 0 0 0 0 0 0 1 }0 0 0 -1 -1 -1 0 0 0 0 0 0 -1 0 }{PSTYLE " " 0 323 1 {CSTYLE "" -1 -1 "" 1 14 0 0 0 0 0 0 0 0 0 0 0 0 0 1 }0 0 0 -1 -1 -1 0 0 0 0 0 0 -1 0 }{PSTYLE "" 0 324 1 {CSTYLE "" -1 -1 "" 1 14 0 0 0 0 0 0 0 0 0 0 0 0 0 1 }0 0 0 -1 -1 -1 0 0 0 0 0 0 -1 0 } {PSTYLE "" 0 325 1 {CSTYLE "" -1 -1 "" 1 14 0 0 0 0 0 0 0 0 0 0 0 0 0 1 }0 0 0 -1 -1 -1 0 0 0 0 0 0 -1 0 }{PSTYLE "" 0 326 1 {CSTYLE "" -1 -1 "" 1 14 0 0 0 0 0 0 0 0 0 0 0 0 0 1 }0 0 0 -1 -1 -1 0 0 0 0 0 0 -1 0 }{PSTYLE "" 0 327 1 {CSTYLE "" -1 -1 "" 1 14 0 0 0 0 0 0 0 0 0 0 0 0 0 1 }0 0 0 -1 -1 -1 0 0 0 0 0 0 -1 0 }} {SECT 0 {PARA 17 "" 0 "" {TEXT -1 39 " Paradigms in Physics: Oscil lations" }}{PARA 17 "" 0 "" {TEXT -1 0 "" }}{PARA 17 "" 0 "" {TEXT -1 77 "© 2000 Oregon State University version Oct 1 6, 2000 DMc" }}{PARA 17 "" 0 "" {TEXT -1 0 "" }}{PARA 17 "" 0 "" {TEXT -1 6 " " }}{PARA 18 "" 0 "" {TEXT -1 29 "Choosing Fourier C oefficients" }}{PARA 18 "" 0 "" {TEXT -1 20 "for Triangular Waves" }} {PARA 19 "" 0 "" {TEXT 264 75 "by Jason Janesky, Catherine Meyer, Cori nne A. Manogue and Philip J. Siemens" }}{PARA 19 "" 0 "" {TEXT -1 43 " Physics Department, Oregon State University" }}{PARA 0 "" 0 "" {TEXT -1 0 "" }}{PARA 0 "" 0 "" {TEXT -1 0 "" }}{SECT 1 {PARA 256 "" 0 "" {TEXT 258 22 "Worksheet Introduction" }}{PARA 257 "" 0 "" {TEXT -1 78 "This worksheet is designed as a first experience in the use of Fourie r series." }}{PARA 258 "" 0 "" {TEXT -1 0 "" }}{PARA 259 "" 0 "" {TEXT -1 0 "" }}{PARA 260 "" 0 "" {TEXT -1 53 "A Fourier series can be used to represent a function " }{XPPEDIT 18 0 "g(t) " "6#-%\"gG6#%\"t G" }{TEXT -1 48 "which is defined on a finite interval of length " } {XPPEDIT 18 0 "T" "6#%\"TG" }{TEXT 263 3 ", " }{TEXT -1 22 "or a peri odic function" }{TEXT 265 8 " g(t) =" }{TEXT -1 3 " g(" }{TEXT 262 3 "t+T" }{TEXT -1 61 "). The fundamental angular frequency of such a f unction is " }{XPPEDIT 18 0 "omega = 2*Pi/T" "6#/%&omegaG*(\"\"#\"\"\" %#PiGF'%\"TG!\"\"" }{TEXT -1 172 " , Fourier series analysis involve s the approximation of such a function as an infinite sum of terms who se frequencies are integer multiples of the fundamental frequency " } {XPPEDIT 18 0 "omega" "6#%&omegaG" }{TEXT -1 1 "." }}{PARA 261 "" 0 " " {TEXT -1 1 " " }}{PARA 262 "" 0 "" {TEXT -1 90 "In the worksheet \"F ourier Series Approximation\" we introduced the Sine and Cosine Serie s:" }}{PARA 263 "" 0 "" {XPPEDIT 18 0 "g(t)=a[0]/2 +a[1]*cos(omega t)+ a[2]*cos(2omega t)+a[3]*cos(3omega t)" "6#/-%\"gG6#%\"tG,**&&%\"aG6#\" \"!\"\"\"\"\"#!\"\"F.*&&F+6#F.F.-%$cosG6#*&%&omegaGF.F'F.F.F.*&&F+6#F/ F.-F56#*(F/F.F8F.F'F.F.F.*&&F+6#\"\"$F.-F56#*(FBF.F8F.F'F.F.F." } {TEXT -1 3 " + " }{TEXT 257 3 "..." }}{PARA 263 "" 0 "" {TEXT -1 5 ".. .+ " }{XPPEDIT 18 0 "+ b[1]*sin(omega t)+b[2]*sin(2omega t)+b[3]*sin(3 omega t) " "6#,(*&&%\"bG6#\"\"\"F(-%$sinG6#*&%&omegaGF(%\"tGF(F(F(*&&F &6#\"\"#F(-F*6#*(F2F(F-F(F.F(F(F(*&&F&6#\"\"$F(-F*6#*(F9F(F-F(F.F(F(F( " }{TEXT -1 6 " + ..." }}{PARA 264 "" 0 "" {TEXT -1 0 "" }}{PARA 265 " " 0 "" {TEXT -1 37 "The coefficients in the series - the " }{XPPEDIT 18 0 "a[n]" "6#&%\"aG6#%\"nG" }{TEXT -1 7 "'s and " }{XPPEDIT 18 0 "b[ n]" "6#&%\"bG6#%\"nG" }{TEXT -1 79 "'s - can be chosen to provide the best approximation to the original function " }{XPPEDIT 18 0 "g(t)" " 6#-%\"gG6#%\"tG" }{TEXT -1 90 ". We can often obtain a useful approxi mation by keeping only a few terms of the series. " }}{PARA 266 "" 0 "" {TEXT -1 0 "" }}{PARA 0 "" 0 "" {TEXT 260 243 "The present workshee t begins with a Fourier series approximation of a sawtooth waveform wh ere you guess the most useful coefficients. Finally, for homework, yo u will use a systematic method to find the best possible values of the coefficients" }{TEXT -1 1 "." }}{PARA 0 "" 0 "" {TEXT -1 2 " " }}} {SECT 1 {PARA 3 "" 0 "" {TEXT 259 12 "Triangle Wav" }{TEXT 261 1 "e" } }{PARA 0 "" 0 "" {TEXT -1 0 "" }}{PARA 267 "" 0 "" {TEXT -1 329 "Now i t's your turn to try to fit a given function with sines and cosines. \+ There is a mathematical way to arrive at the coefficients which will b e presented to you shortly. However using intuition and educated gues ses will provide you with a lot of insight into the underlying princip les. Try to fit the sawtooth pattern below:" }}{PARA 0 "" 0 "" {TEXT -1 0 "" }}{SECT 1 {PARA 4 "" 0 "" {TEXT -1 17 "The Sawtooth wave" }} {EXCHG {PARA 268 "> " 0 "" {MPLTEXT 1 0 20 "restart:with(plots):" }}} {EXCHG {PARA 269 "> " 0 "" {MPLTEXT 1 0 86 "f(t):=piecewise(t<=-Pi,-3/ Pi*t-9/2,t<0,3/Pi*t+3/2,t<=Pi,-3/Pi*t+3/2, t>Pi,3/Pi*t-9/2);" }}} {EXCHG {PARA 270 "> " 0 "" {MPLTEXT 1 0 35 "plot(f(t),t=-2*Pi..2*Pi,-1 .5..1.5);" }}}{PARA 271 "" 0 "" {TEXT -1 0 "" }}{PARA 272 "" 0 "" {TEXT -1 48 "What is the fundamental period of this waveform?" }} {PARA 273 "" 0 "" {TEXT -1 0 "" }}{EXCHG {PARA 274 "> " 0 "" {MPLTEXT 1 0 12 "Period := ;" }}}{PARA 275 "" 0 "" {TEXT -1 0 "" }}{PARA 276 " " 0 "" {TEXT -1 45 "this defines the fundamental frequency to be:" }} {PARA 277 "" 0 "" {TEXT -1 0 "" }}{EXCHG {PARA 278 "> " 0 "" {MPLTEXT 1 0 21 "omega := 2*Pi/Period;" }}}{PARA 0 "" 0 "" {TEXT -1 0 "" }}} {SECT 1 {PARA 4 "" 0 "" {TEXT -1 24 "The constant term (n=0):" }} {PARA 279 "" 0 "" {TEXT -1 27 "This is the constant term, " }{XPPEDIT 18 0 "a[0]" "6#&%\"aG6#\"\"!" }{TEXT -1 141 ". It does not depend on \+ sine or cosine. Remember this guess should get you as close to as man y points as possible. Enter your guess below:" }}{PARA 280 "" 0 "" {TEXT -1 0 "" }}{EXCHG {PARA 281 "> " 0 "" {MPLTEXT 1 0 11 "a[0] := 1 \+ ;" }}}{PARA 282 "" 0 "" {TEXT -1 0 "" }}{PARA 283 "" 0 "" {TEXT -1 36 "Your Fourier series so far is then:" }}{PARA 284 "" 0 "" {TEXT -1 0 "" }}{EXCHG {PARA 285 "> " 0 "" {MPLTEXT 1 0 15 "g(t) := a[0]/2;" }}} {PARA 286 "" 0 "" {TEXT -1 0 "" }}{PARA 287 "" 0 "" {TEXT -1 45 "And p lotting that against the sawtooth gives:" }}{PARA 288 "" 0 "" {TEXT -1 0 "" }}{EXCHG {PARA 289 "> " 0 "" {MPLTEXT 1 0 44 "plot([f(t),g(t)] , t=-2*Pi..2*Pi, -1.5..1.5);" }}}{PARA 290 "" 0 "" {TEXT -1 0 "" }} {PARA 291 "" 0 "" {TEXT -1 67 "You can plot the difference if you woul d like using the line below:" }}{PARA 292 "" 0 "" {TEXT -1 0 "" }} {EXCHG {PARA 293 "> " 0 "" {MPLTEXT 1 0 44 "plot([f(t)-g(t)], t=-2*Pi. .2*Pi, -1.5..1.5);" }}}{PARA 0 "" 0 "" {TEXT -1 0 "" }}}{SECT 1 {PARA 4 "" 0 "" {TEXT -1 27 "The fundamental term (n=1):" }}{PARA 294 "" 0 " " {TEXT -1 37 "Now determine what the coefficients, " }{XPPEDIT 18 0 " a[1]" "6#&%\"aG6#\"\"\"" }{TEXT -1 5 " and " }{XPPEDIT 18 0 "b[1]" "6# &%\"bG6#\"\"\"" }{TEXT -1 260 ", should be. A hint is to first determ ine if the sawtooth is even or odd. There should be a match between t his (even or odd) and the choice of sine or cosine terms. An odd func tion can't be used to describe an even function. WHY? Enter your cho ices below:" }}{PARA 295 "" 0 "" {TEXT -1 0 "" }}{EXCHG {PARA 296 "> \+ " 0 "" {MPLTEXT 1 0 11 "a[1] := ;" }}}{PARA 297 "" 0 "" {TEXT -1 0 " " }}{EXCHG {PARA 298 "> " 0 "" {MPLTEXT 1 0 11 "b[1] := ;" }}}{PARA 299 "" 0 "" {TEXT -1 0 "" }}{PARA 300 "" 0 "" {TEXT -1 19 "The series \+ is then:" }}{PARA 301 "" 0 "" {TEXT -1 0 "" }}{EXCHG {PARA 302 "> " 0 "" {MPLTEXT 1 0 59 "g(t) := a[0]/2 + a[1]*cos(1*omega*t) + b[1]*sin(1* omega*t);" }}}{PARA 303 "" 0 "" {TEXT -1 0 "" }}{PARA 304 "" 0 "" {TEXT -1 43 "Plotting your guess and the waveform gives:" }}{PARA 305 "" 0 "" {TEXT -1 0 "" }}{EXCHG {PARA 306 "> " 0 "" {MPLTEXT 1 0 44 "pl ot([f(t),g(t)], t=-2*Pi..2*Pi, -1.5..1.5);" }}}{PARA 307 "" 0 "" {TEXT -1 0 "" }}{PARA 308 "" 0 "" {TEXT -1 99 "Adjust your parameters \+ until you are satisfied that you are as close to as many points as pos sible." }}{PARA 309 "" 0 "" {TEXT -1 98 "You can subtract the two wave forms to give you clues about the next terms using the command below: " }}{PARA 310 "" 0 "" {TEXT -1 0 "" }}{EXCHG {PARA 311 "> " 0 "" {MPLTEXT 1 0 44 "plot([f(t)-g(t)], t=-2*Pi..2*Pi, -1.5..1.5);" }}} {PARA 0 "" 0 "" {TEXT -1 0 "" }}}{SECT 1 {PARA 4 "" 0 "" {TEXT -1 19 " Higher order terms:" }}{PARA 312 "" 0 "" {TEXT -1 221 "Keep going incl uding as many terms as you can. Adjusting them to give as good a fit as possible. You will have to cut and paste the commands you need or create them yourself. Call an instructor over for any questions." }} {PARA 313 "" 0 "" {TEXT -1 0 "" }}{PARA 314 "" 0 "" {TEXT -1 0 "" }} {EXCHG {PARA 315 "> " 0 "" {MPLTEXT 1 0 11 "a[0] := ;" }}}{EXCHG {PARA 316 "> " 0 "" {MPLTEXT 1 0 11 "a[1] := ;" }}}{EXCHG {PARA 317 "> " 0 "" {MPLTEXT 1 0 11 "b[1] := ;" }}}{EXCHG {PARA 318 "> " 0 "" {MPLTEXT 1 0 11 "a[2] := ;" }}}{EXCHG {PARA 319 "> " 0 "" {MPLTEXT 1 0 11 "b[2] := ;" }}}{EXCHG {PARA 320 "> " 0 "" {MPLTEXT 1 0 103 "g (t) := a[0]/2 + a[1]*cos(1*omega*t) + b[1]*sin(1*omega*t) + a[2]*cos(2 *omega*t) + b[2]*sin(2*omega*t);" }}{PARA 0 "> " 0 "" {MPLTEXT 1 0 0 " " }}}{EXCHG {PARA 321 "> " 0 "" {MPLTEXT 1 0 44 "plot([f(t),g(t)], t=- 2*Pi..2*Pi, -1.5..1.5);" }}}{EXCHG {PARA 0 "> " 0 "" {MPLTEXT 1 0 0 " " }}}}{PARA 322 "" 0 "" {TEXT -1 0 "" }}{PARA 323 "" 0 "" {TEXT -1 74 "For homework you will mathematically calculate the correct coefficien ts. " }}{PARA 324 "" 0 "" {TEXT -1 0 "" }}{PARA 325 "" 0 "" {TEXT -1 111 "Compare these calculated results to your guesses, and then use th em in the program to see how well they work. " }}{PARA 0 "" 0 "" {TEXT -1 0 "" }}{PARA 0 "" 0 "" {TEXT 266 100 "WHEN YOU ARE TRYING OUT YOUR RESULTS, BE SURE TO CHOOSE INLINE PLOTS IN ORDER TO DOCUMENT YOU R WORK." }}{PARA 326 "" 0 "" {TEXT -1 0 "" }}{PARA 327 "" 0 "" {TEXT -1 98 "After you substitute your homework results, print out the works heet to document your achievement. " }}{PARA 0 "" 0 "" {TEXT -1 0 "" } }}{PARA 3 "" 0 "" {TEXT -1 0 "" }}}{MARK "12" 0 }{VIEWOPTS 1 1 0 1 1 1803 1 1 1 1 }{PAGENUMBERS 0 1 2 33 1 1 }