= 0 for we showed that Length-N (i.e., h[n] Vn N-1) real-valued causal FIR filters...

 

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= 0 for we showed that Length-N (i.e., h[n] Vn<0 and Vn > N-1) real-valued causal FIR filters with even symmetry (i.e., h[n] = h[N-1-n]) and odd N (i.e., N = 2M+1) had frequency response that could be represented as M-1 H(e) = ) = e¯jwM | h[M] +2Σh[n] cos(w[n-M]) MI)), n=0 and thus posseses generalized linear phase (GLP). Derive a similar GLP representation for length-N real-valued causal FIR filters with odd symmetry (i.e., h[n] = -h[N-1 - n]) and even N (i.e., N = 2M). = 0 for we showed that Length-N (i.e., h[n] Vn<0 and Vn > N-1) real-valued causal FIR filters with even symmetry (i.e., h[n] = h[N-1-n]) and odd N (i.e., N = 2M+1) had frequency response that could be represented as M-1 H(e) = ) = e¯jwM | h[M] +2Σh[n] cos(w[n-M]) MI)), n=0 and thus posseses generalized linear phase (GLP). Derive a similar GLP representation for length-N real-valued causal FIR filters with odd symmetry (i.e., h[n] = -h[N-1 - n]) and even N (i.e., N = 2M).

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To derive a generalized linear phase GLP representation for length N realvalued causal FIR filters w... View the full answer