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
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.
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 $-40$).
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 $\omega\to\infty$.
$$\boxed{K=16.7,\ \omega_n=3\ \text{rad/s},\ \zeta=0.333,\ M_r\approx+4.0\ \text{dB at}\
\omega_r=2.65\ \text{rad/s}}$$
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 $\omega\to\infty$.
$$\boxed{K=5,\ \text{break at}\ \omega=10\ \text{rad/s (monotonic, no resonance)}}$$
Figure Q5(a) — asymptotic (dashed) vs. actual (solid) Bode
magnitude and phase for $150/[s(s^2+2s+9)]$.
Figure Q5(b) — asymptotic (dashed) vs. actual (solid) Bode
magnitude and phase for $50/[s^2(s+10)]$.