EEE 302 Electrical Networks II Dr. Keith E. Holbert Summer 2001 Lecture 20 Sinusoidal Frequency Analysis • The transfer function is composed of both magnitude and.
Download ReportTranscript EEE 302 Electrical Networks II Dr. Keith E. Holbert Summer 2001 Lecture 20 Sinusoidal Frequency Analysis • The transfer function is composed of both magnitude and.
EEE 302 Electrical Networks II Dr. Keith E. Holbert Summer 2001 Lecture 20 1 Sinusoidal Frequency Analysis • The transfer function is composed of both magnitude and phase information as a function of frequency H( j) H ( j) e j ( ) where |H(jω)| is the magnitude and φ(ω) is the phase angle • Plots of the magnitude and phase characteristics are used to fully describe the frequency response Lecture 20 2 Bode Plots • A Bode plot is a semilog plot of transfer function's magnitude and phase as a function frequency • The gain magnitude is many times expressed in terms of decibels (dB) dB = 20 log10 A where A is the amplitude or gain – a decade is defined as any 10-to-1 frequency range – an octave is any 2-to-1 frequency range 20 dB/decade = 6 dB/octave Lecture 20 3 Bode Plots • Straight-line approximations of the Bode plot may be drawn quickly from knowing the poles and zeros – response approaches a minimum near the zeros – response approaches a maximum near the poles • The overall effect of constant, zero and pole terms Term Magnitude Break Constant (K) N/A Zero Pole Asymptotic Magnitude Slope Asymptotic Phase Shift 0 0 upward +20 dB/decade + 90 downward –20 dB/decade – 90 Lecture 20 4 Bode Plots • Express the transfer function in standard form K j (1 j1 ) 1 2 2 ( j 2 ) ( j 2 ) 2 H( j ) (1 j a ) 1 2 b ( j b ) ( j b ) 2 N • There are four different factors: 1. 2. 3. 4. Constant gain term, K Poles or zeros at the origin, (j)±N Poles or zeros of the form (1+ j) Quadratic poles or zeros of the form 1+2(j)+(j)2 Lecture 20 5 Bode Plots • We can combine the constant gain term and the poles/zeros at the origin such that the magnitude crosses 0dB at K Pole : ( j ) N 0 dB K 1 / N Zero : K ( j ) N 0 dB (1 / K )1 / N • Define the break frequency to be at ω=1/τ with magnitude at ±3dB and phase at ±45° Lecture 20 6 Bode Plots Magnitude Behavior Factor Constant Low Freq Break Asymptotic Phase Behavior Low Freq Break Asymptotic 20 log10(K) for all frequencies 0 for all frequencies Poles or zeros at origin ±20N dB/decade for all frequencies with a crossover of 0 dB at ω=1 ±90(N) for all frequencies First order (simple) poles or zeros 0 dB ±3N dB at ω=1/τ ±20N dB/decade 0 ±45(N) with slope ±45 per decade ±90(N) Quadratic poles or zeros 0 dB see ζ at ω=1/τ ±40N dB/decade 0 ±90(N) ±180(N) where N is the number of roots of value τ Lecture 20 7 Class Examples • Extension Exercise E12.3 • Extension Exercise E12.4 • Extension Exercise E12.5 Lecture 20 8 MATLAB Exercise • Here we will use MATLAB to create Bode plots for Extension Exercise E12.3 • Start MATLAB and open the file BodePlt.m from the class webpage Lecture 20 9