The transfer function is identified as G(s) = (s² + 2ζωn + ωn²)/((s + p1)(s + p2), indicating a relationship between the zeros and poles. The analysis suggests that both ωn is less than p1 and p2, leading to the conclusion that the system behaves like a high-pass filter due to the magnitude amplification at higher frequencies. The proximity of the imaginary part of the zeros and the real parts of the poles complicates the determination of their frequency responses. Despite some uncertainty about the exact frequency behavior, the conclusion about the filter type is supported. Overall, the discussion emphasizes the importance of analyzing pole-zero plots and Bode plots in filter classification.