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23-Mechatronics-A1 Systems Dynamics and Controls · Undated paper

Question 5 of 6: Bode Diagrams of Two Open-Loop Transfer Functions

Nivaar worked solution (AI-drafted; not reviewed by a licensed engineer)

Notes on this paper

Paper format. 16-Mex-A1, System Analysis and Control, a three-hour closed-book National Examination for which candidates may use an approved Casio or Sharp calculator. The cover page states that any four (4) of the printed questions constitute a complete paper, all of equal value; all six printed questions are worked here.

Reference texts. N.S. Nise, Control Systems Engineering, 8th ed. (Ch. 4 second-order time response; Ch. 6 stability & the Routh-Hurwitz criterion; Ch. 8 root locus; Ch. 10 frequency-response methods); K. Ogata, Modern Control Engineering, 5th ed. (Ch. 3 Laplace transform; Ch. 5 stability analysis; Ch. 6 root-locus method; Ch. 7 frequency-response analysis).

Question 5: Bode Diagrams of Two Open-Loop Transfer Functions

Question text not reproduced: the examination questions are © Engineers and Geoscientists BC. Open the official past paper (linked at the top of this page) to read the question, then follow the worked solution below.

Given. Two open-loop transfer functions: (a) one integrator plus an underdamped quadratic factor; (b) a double integrator plus one real pole at $s=-10$.

Find. The asymptotic and corrected (actual) Bode magnitude and phase plots for each.

Approach. Rewrite each transfer function in Bode (time-constant) form to read off the DC gain and break frequencies, draw the straight-line magnitude asymptote, then correct near each break using the exact quadratic/first-order corrections and plot the running phase.

  1. Part (a) — Bode form. $$G(s)H(s)=\frac{150}{s(s^2+2s+9)}=\frac{K}{s\!\left(\dfrac{s^2}{\omega_n^2} +\dfrac{2\zeta s}{\omega_n}+1\right)},\qquad K=\frac{150}{9}=16.7,\ \ \omega_n=3\ \text{rad/s},\ \ \zeta=\tfrac13=0.333$$
  2. Part (a) — asymptote. $-20$ dB/decade line through $20\log_{10} 16.7=24.4$ dB at $\omega=1$ rad/s (the integrator alone), breaking to $-60$ dB/decade at $\omega_n=3$ rad/s (integrator's $-20$ plus the quadratic's additional $-40$).
  3. Part (a) — correction near the break. Since $\zeta=0.333< 0.707$ the quadratic factor peaks: the correction at $\omega=\omega_n$ is $-20\log_{10}(2\zeta)=+3.5$ dB above the asymptote, and the true resonant peak $M_r=1/(2\zeta\sqrt{1-\zeta^2})=1.59$ ($+4.0$ dB) occurs slightly below $\omega_n$ at $\omega_r=\omega_n\sqrt{1-2\zeta^2}=2.65$ rad/s. Phase runs from $-90^\circ$ ($\omega\ll \omega_n$, integrator alone) through exactly $-180^\circ$ at $\omega=\omega_n$, toward $-270^\circ$ as $\omega\to\infty$. $$\boxed{K=16.7,\ \omega_n=3\ \text{rad/s},\ \zeta=0.333,\ M_r\approx+4.0\ \text{dB at}\ \omega_r=2.65\ \text{rad/s}}$$
  4. Part (b) — Bode form. $$G(s)H(s)=\frac{50}{s^2(s+10)}=\frac{K}{s^2(s/10+1)},\qquad K=\frac{50}{10}=5,\quad \text{break at}\ \omega=10\ \text{rad/s}$$
  5. Part (b) — asymptote and correction. $-40$ dB/decade line (double integrator) through $20\log_{10}5=14.0$ dB at $\omega=1$ rad/s, breaking to $-60$ dB/decade at $\omega=10$ rad/s. A simple real pole has no resonance: the standard correction is $-3$ dB exactly at the break and $\mp1$ dB at half/double the break frequency. Phase starts at $-180^\circ$ (double integrator, constant for $\omega\ll10$), runs through $-225^\circ$ at the break, and approaches $-270^\circ$ as $\omega\to\infty$. $$\boxed{K=5,\ \text{break at}\ \omega=10\ \text{rad/s (monotonic, no resonance)}}$$
Q5(a) — Bode DiagramG(s)H(s) = 150 / [s(s²+2s+9)]0.1110100|G(jω)| dB0.1110100Phase (deg)ω (rad/s, log scale)-270-180-900ωn=3, ζ=0.333 | break -20→-60 dB/decasymptoticactual
Figure Q5(a) — asymptotic (dashed) vs. actual (solid) Bode magnitude and phase for $150/[s(s^2+2s+9)]$.
Q5(b) — Bode DiagramG(s)H(s) = 50 / [s²(s+10)]0.1110100|G(jω)| dB0.1110100Phase (deg)ω (rad/s, log scale)-270-180-90double integrator | break -40→-60 dB/dec at ω=10asymptoticactual
Figure Q5(b) — asymptotic (dashed) vs. actual (solid) Bode magnitude and phase for $50/[s^2(s+10)]$.
$K$Break(s)Asymptotic slopesPhase range
(a)16.7$\omega_n=3$$-20\to-60$ dB/dec$-90^\circ\to-270^\circ$
(b)5$\omega=10$$-40\to-60$ dB/dec$-180^\circ\to-270^\circ$