Summary

This document introduces second-order systems, focusing on their transfer functions and characteristics, such as natural frequency (ωn) and damping ratio (ζ). It provides examples demonstrating calculations of these parameters. The document also covers various classifications of the response, including underdamped and overdamped systems.

Full Transcript

Introduction A general second-order system is characterized by the following transfer function. C( s )  n2  2 R( s ) s  2 n s   n2 Introduction C( s )  n2...

Introduction A general second-order system is characterized by the following transfer function. C( s )  n2  2 R( s ) s  2 n s   n2 Introduction C( s )  n2  2 R( s ) s  2 n s   n2 n un-damped natural frequency of the second order system, which is the frequency of oscillation of the system without damping.  damping ratio of the second order system, which is a measure of the degree of resistance to change in the system output. Example#1 Determine the un-damped natural frequency and damping ratio of the following second order system. C( s ) 4  2 R( s ) s  2s  4 Compare the numerator and denominator of the given transfer function with the general 2nd order transfer function. C( s )  n2  2 R( s ) s  2 n s   n2 n2  4  n  2 rad / sec  2 n s  2s   n  1 s 2  2 n s  n2  s 2  2s  4    0.5 Introduction C( s )  n2  2 R( s ) s  2 n s   n2 Two poles of the system are   n   n  2  1   n   n  2  1 Introduction   n   n  2  1   n   n  2  1 According the value of  , a second-order system can be set into one of the four categories: 1. Overdamped - when the system has two real distinct poles (  >1). jω δ -c -b -a Introduction   n   n  2  1   n   n  2  1 According the value of  , a second-order system can be set into one of the four categories: 2. Underdamped - when the system has two complex conjugate poles (0

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