Define `H(s)=C\frac{N(s)}{D(s)}`





We start with the transfer function (note: the process here follows that on the second page of the file BodeRules.pdf):

H(s)=Cs2+5s+6s5+4s4+7s3+6s2+2s

We rewrite it by factoring into real poles & zeros, complex poles & zeros and poles & zeros at the origin.

H(s)=C(1s)(s+ωz1)(s+ωz2)(s+ωp1)2(s2+2ζp1ω0p1s+ω0p12)

With:

  • Constant: C=10
  • A real pole at s=-1.00, of muliplicity 2.
    This is the (s+ωp1)2 term in the denominator, with ωp1=1.
  • A real zero at s=-2.00.
    This is the (s+ωz1) term in the numerator, with ωz1=2.
  • A real zero at s=-3.00.
    This is the (s+ωz2) term in the numerator, with ωz2=3.
  • Complex poles, at s = -1.00 ± 1.00j.
    This is the (s2+2ζp1ω0p1s+ω0p12) term in the denominator, with ω0p1=1.41, ζp1=0.707.
  • A pole at the origin.

Next we write all the poles and zeros is our standard form.

H(s)=Cωz1ωz2ωp12ω0p12(1s)(1+s/ωz1)(1+s/ωz2)(1+s/ωp1)2(1+2ζp1(s/ω0p1)+(s/ω0p12))

Rewrite the constant:

K=Cωz1ωz2ωp12ω0p12=30.0=29.6dB

So

H(s)=K(1s)(1+s/ωz1)(1+s/ωz2)(1+s/ωp1)2(1+2ζp1(s/ω0p1)+(s/ω0p12))

Now the transfer function is in the form we need to apply our rules to draw the Bode plot.

Putting It All Together


Magnitude
Phase

Calculate Sinusoid


Input sinusoid of form cos(ω rad/S · t + φ°)



1.0 · cos(1.0 rad/S · t + 1.0°)

cos(ω rad/S · t + φ° + θ°)

The dotted lines are straight-line approximations of the exact plots, which are solid.
The red dots show the location of the input frequency on the overal chart.

References

© Copyright 2005 to 2020 Erik Cheever    This page may be freely used for educational purposes.














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Erik Cheever       Department of Engineering         Swarthmore College