# Solutions HW #5 PHYS 160 Fall # Travis Hoppe restart: with(plots): signal := (N1,N2,t) -> sum(term(2*k-1,t),k=N1..N2); term := (n,t) -> a(n)*sin(2*Pi*n*t/TP); a := (n) -> 4/(Pi*n); TP := 1.125: Zio2JUkjTjFHNiJJI04yR0YlSSJ0R0YlRiU2JEkpb3BlcmF0b3JHRiVJJmFycm93R0YlRiUtSSRzdW1HRiU2JC1JJXRlcm1HRiU2JCwmSSJrR0YlIiIjISIiIiIiOSYvRjI7OSQ5JUYlRiVGJQ== Zio2JEkibkc2IkkidEdGJUYlNiRJKW9wZXJhdG9yR0YlSSZhcnJvd0dGJUYlKiYtSSJhR0YlNiM5JCIiIi1JJHNpbkdGJTYjLCQqKkkjUGlHJSpwcm90ZWN0ZWRHRi9GLkYvOSVGL0kjVFBHRiUhIiIiIiNGL0YlRiVGJQ== Zio2I0kibkc2IkYlNiRJKW9wZXJhdG9yR0YlSSZhcnJvd0dGJUYlLCQqJkkjUGlHJSpwcm90ZWN0ZWRHISIiOSRGLSIiJUYlRiVGJQ== plot( signal(1,50,t), t=0..2*TP, title="Two full cycles of the signal"); 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filter := (n) -> (1+exp(n-9))**(-1); filtered_signal := (N1,N2,t) -> sum(term(2*k-1,t)*filter(2*k-1),k=N1..N2); Zio2I0kibkc2IkYlNiRJKW9wZXJhdG9yR0YlSSZhcnJvd0dGJUYlKiQsJiIiIkYrLUkkZXhwR0YlNiMsJjkkRishIipGK0YrISIiRiVGJUYl Zio2JUkjTjFHNiJJI04yR0YlSSJ0R0YlRiU2JEkpb3BlcmF0b3JHRiVJJmFycm93R0YlRiUtSSRzdW1HNiQlKnByb3RlY3RlZEdJKF9zeXNsaWJHRiU2JComLUkldGVybUdGJTYkLCZJImtHRiUiIiMhIiIiIiI5JkY5LUknZmlsdGVyR0YlNiNGNUY5L0Y2OzkkOSVGJUYlRiU= plot( filtered_signal(1,15,t), t=0..TP, title="One full cycle of the filtered signal"); 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 slope := (t) -> diff( filtered_signal(1,15,t), t); slope(t); Zio2I0kidEc2IkYlNiRJKW9wZXJhdG9yR0YlSSZhcnJvd0dGJUYlLUklZGlmZkclKnByb3RlY3RlZEc2JC1JMGZpbHRlcmVkX3NpZ25hbEdGJTYlIiIiIiM6OSRGMkYlRiVGJQ== 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 plot( slope(t), t=0..TP, title="Slope of filtered_signal" ); 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 # Zeros of the slopes == maxima and minima of the orginal function Z := seq(fsolve( slope(t)=0, t=x ),x=0..TP/2, 0.01): Z := [seq(x, x in {Z})]; Ny0kISt0RCkqXDchIzUkIitXbTJdaSEjNiQiK3REKSpcN0YlJCIrKCkqSF0oPUYlJCIrJDRmKipcI0YlJCIrXytdN0dGJSQiKy40L0RKRiUkIistKygqXFBGJSQiK0B1LHZWRiUkIitNQioqKipcRiUkIisqM2ZcNylGJQ== # Plug these values back into the orginal function Y_Z := [seq(filtered_signal(1,15,t), t in Z)]; Ny0kISsiSEpbYiohIzUkIitveVVTNiEiKiQiKyJISltiKkYlJCIrPGQtOTVGKCQiK2kpUl8nKipGJSQiK3c+PnkqKkYlJCIrZClSXycqKkYlJCIrPWQtOTVGKCQiKyNISltiKkYlJCIrbnlVUzZGKCQhK2UpUl8nKipGJQ== # Visually, I like to see the solutions mapped back onto the orginal function (as a check!) P_Z := [seq( [Z[i],Y_Z[i]], i=1..nops(Z) )]: P1 := plot( filtered_signal(1,15,t), t=0..TP/2 ): P2 := plot( P_Z,t=0..TP/2,style=point,symbolsize=20,symbol="circle" ): display([P1,P2]); 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 # The second half of the period is clearly a reflection of the first TP/2, thus the solution can be mapped back onto itself if one desired the other zeros.