1 / 38

Frequency Resp. method

Frequency Resp. method. Given: G ( j ω ) as a function of ω is called the freq. resp. For each ω , G ( jω ) = x ( ω ) + jy ( ω ) is a point in the complex plane As ω varies from 0 to ∞, the plot of G ( jω ) is called the Nyquist plot. Can rewrite in Polar Form:

pavel
Download Presentation

Frequency Resp. method

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript


  1. Frequency Resp. method Given: • G(jω) as a function of ω is called the freq. resp. • For each ω, G(jω) = x(ω) + jy(ω) is a point in the complex plane • As ω varies from 0 to ∞, the plot of G(jω) is called the Nyquist plot

  2. Can rewrite in Polar Form: • |G(jω)| as a function of ω is called the amplitude resp. • as a function of ω is called the phase resp. • The two plots: With log scale-ω, are Bode plot

  3. To obtain freq. Resp from G(s): • Select • Evaluate G(jω) at those to get • Plot Imag(G) vs Real(G): Nyquist • or plot With log scale ω • Matlab command to explore: nyquist, bode

  4. To obtain freq. resp. experimentally: • Select • Given input to system as: • Adjust A1 so that the output is not saturated or distorted. • Measure amp B1 and phase φ1 ofoutput:

  5. Then is the freq. resp. of the system at freq ω • Repeat for all ωK • Either plot or plot

  6. Product of T.F.

  7. System type, steady state tracking, & Bode plot C(s) Gp(s) R(s) Y(s)

  8. As ω → 0 Therefore: gain plot slope = –20N dB/dec. phase plot value = –90N deg

  9. If Bode gain plot is flat at low freq, system is “type zero” Confirmed by phase plot flat and  0° at low freq Then: Kv = 0, Ka = 0 Kp = Bode gain as ω→0 = DC gain (convert dB to values)

  10. Example

  11. Steady state tracking error Suppose the closed-loop system is stable: If the input signal is a step, ess would be = If the input signal is a ramp, ess would be = If the input signal is a unit acceleration, ess would be =

  12. N = 1, type = 1 Bode mag. plot has –20 dB/dec slope at low freq. (ω→0) (straight line with slope = –20 as ω→0) Bode phase plot becomes flat at –90° when ω→0 Kp= DC gain → ∞ Kv = K = value of asymptotic straight line at ω = 1 =ws0dB =asymptotic straight line’s 0 dB crossing frequency Ka = 0

  13. Example Asymptotic straight line ws0dB ~14

  14. The matching phase plot at lowfreq. must be → –90° type = 1 Kp= ∞ ← position error const. Kv = value of low freq. straight line at ω = 1 = 23 dB ≈ 14 ← velocity error const. Ka = 0 ← acc. error const.

  15. Steady state tracking error Suppose the closed-loop system is stable: If the input signal is a step, ess would be = If the input signal is a ramp, ess would be = If the input signal is a unit acceleration, ess would be =

  16. N = 2, type = 2 Bode gain plot has –40 dB/dec slope at low freq. Bode phase plot becomes flat at –180° at low freq. Kp= DC gain → ∞ Kv = ∞ also Ka = value of straight line at ω = 1 = ws0dB^2

  17. Example Ka ws0dB=Sqrt(Ka) How should the phase plot look like?

  18. Steady state tracking error Suppose the closed-loop system is stable: If the input signal is a step, ess would be = If the input signal is a ramp, ess would be = If the input signal is a unit acceleration, ess would be =

  19. System type, steady state tracking, & Nyquist plot C(s) Gp(s) As ω → 0

  20. Type 0 system, N=0 Kp=lims0 G(s) =G(0)=K Kp w0+ G(jw)

  21. Type 1 system, N=1 Kv=lims0sG(s) cannot be determined easily from Nyquist plot winfinity w0+ G(jw)  -j∞

  22. Type 2 system, N=2 Ka=lims0 s2G(s) cannot be determined easily from Nyquist plot winfinity w0+ G(jw)  -∞

  23. Margins on Bode plots In most cases, stability of this closed-loop can be determined from the Bode plot of G: • Phase margin > 0 • Gain margin > 0 G(s)

  24. If never cross 0 dB line (always below 0 dB line), then PM = ∞. If never cross –180° line (always above –180°), then GM = ∞. If cross –180° several times, then there are several GM’s. If cross 0 dB several times, then there are several PM’s.

  25. Example: Bode plot on next page.

  26. Example: Bode plot on next page.

  27. Where does cross the –180° lineAnswer: __________at ωpc, how much is • Closed-loop stability: __________

  28. crosses 0 dB at __________at this freq, • Does cross –180° line? ________ • Closed-loop stability: __________

  29. Margins on Nyquist plot Suppose: • Draw Nyquist plot G(jω) & unit circle • They intersect at point A • Nyquist plot cross neg. real axis at –k

More Related