Power Electronics

Chapter 8
Dynamic Modeling and Control of Converters

Post Graduate Program in Electrical Engineering
Power Electronics   •   Post Graduate

Dynamic Modeling and Control of Converters

Introduction

Power converters are nonlinear, switched systems whose operating states change within every switching period. Their semiconductor devices impose discrete circuit topologies, while inductors and capacitors generate continuous dynamic states. A useful control model must therefore preserve the dominant energy-storage dynamics while suppressing unnecessary switching detail.

Dynamic modeling answers three central questions:

  1. How do input voltage, duty ratio and load disturbances affect converter states and output voltage?
  2. What poles, zeros, delays and nonlinearities constrain achievable control bandwidth?
  3. How should analog or digital controllers be designed to ensure stability, robustness and acceptable transient performance?

This chapter develops averaged and sampled-data models for buck, boost and inverting buck–boost converters operating in continuous-conduction mode (CCM). Particular attention is given to right-half-plane zeros, output impedance, current-mode instability, digital implementation and model validation.

Learning Objectives

After studying this chapter, the reader should be able to:

  • derive nonlinear averaged converter models;
  • linearize a converter about a steady operating point;
  • obtain control-to-output, line-to-output and output-impedance transfer functions;
  • explain the dynamic differences among buck, boost and buck–boost converters;
  • define converter natural frequency and quality factor;
  • design and assess voltage-mode and current-mode feedback loops;
  • quantify sampled-data delay and slope-compensation requirements;
  • evaluate stability margins, bandwidth limitations and model uncertainty; and
  • implement a structured modeling, control-design and validation workflow.

1. Modeling Hierarchy and Assumptions

A converter may be represented at several levels.

ModelSwitching represented?Principal use
Detailed switching modelYesDevice stress, switching loss, EMI and waveform validation
Sampled-data modelThrough cycle mapsSubharmonic oscillation and digital control
State-space averaged modelNoLow-frequency dynamics and control design
Small-signal modelNo; locally linearTransfer functions, poles, zeros and loop shaping
Reduced-order modelNoReal-time implementation and system-level studies

Unless otherwise stated, the derivations below assume:

  • ideal semiconductor switches;
  • fixed switching frequency fs;
  • CCM;
  • negligible inductor and capacitor parasitics;
  • a resistive nominal load R;
  • perturbation frequencies well below fs; and
  • sufficiently small perturbations that operation remains near one equilibrium.

These assumptions must not be extended uncritically to discontinuous conduction, pulse-skipping operation, saturation, current limiting or large-signal startup.

2. State-Space Averaging and Linearization

Let the state vector be x, the input vector be u, the duty ratio be d, and the output be y. For two switching configurations,

\dot{x}=A1x+B1u \quad \text{and} \quad \dot{x}=A2x+B2u.

If configuration 1 occupies fraction d of each switching period, first-order state-space averaging gives

\dot{x}=d(A1x+B1u)+(1-d)(A2x+B2u).

The model is nonlinear whenever duty ratio multiplies a state or input. Write each quantity as its equilibrium value plus a perturbation:

x=X+\hat{x},\qquad d=D+\hat{d},\qquad u=U+\hat{u}.

Terms containing products of perturbations, such as \hat{d}\hat{x}, are second order and are neglected in a local small-signal model. The result has the form

\dot{\hat{x}}=A\hat{x}+Bu\hat{u}+Bd\hat{d},\qquad
\hat{y}=C\hat{x}+Du\hat{u}+Dd\hat{d}.

The corresponding transfer matrix is

G(s)=C(sI-A)-1B+D.

Here s is the Laplace variable in s⁻¹. The eigenvalues of A are the local poles.

Converter dynamic modeling workflow Switchingcircuits Nonlinearaverage model Operating-pointlinearization Loop designand robustness Switched-modelvalidation If validation fails, revise parasitics, delays, operating point or model order.
Converter dynamic modeling workflow
Figure: Converter dynamic modeling workflow

Figure: A control model is useful only after validation against the switched converter and relevant operating range.

3. Buck Converter Model

Let i be inductor current, v output voltage, vg input voltage and iload an independent disturbance current drawn from the output. Averaging the CCM switching states gives

L\frac{di}{dt}=dvg-v,
C\frac{dv}{dt}=i-\frac{v}{R}-iload.

At equilibrium, with no independent load disturbance,

V=DVg,\qquad I=\frac{V}{R}.

Linearization produces

Ls\hat{i}=Vg\hat{d}+D\hat{v}g-\hat{v},
Cs\hat{v}=\hat{i}-\frac{\hat{v}}{R}-\hat{i}load.

Define the characteristic polynomial

\Deltab(s)=LCs2+\frac{L}{R}s+1.

The control-to-output and line-to-output transfer functions are

Gvd(s)=\frac{\hat{v}}{\hat{d}}=\frac{Vg}{\Deltab(s)},
Gvg(s)=\frac{\hat{v}}{\hat{v}g}=\frac{D}{\Deltab(s)}.

For an incremental current drawn from the output, define output impedance by Zo=-\hat{v}/\hat{i}load. Direct substitution gives

Zo(s)=-\frac{\hat{v}}{\hat{i}load}
=\frac{Ls}{LCs2+(L/R)s+1}.

The minus sign in the definition makes Zo positive in the usual engineering sense: an increase in current drawn tends to reduce output voltage. The ideal fixed-duty model has zero DC output impedance; winding resistance, switch resistance and control limitations make practical DC impedance nonzero.

The undamped natural frequency and quality factor are

\omega0=\frac{1}{\sqrt{LC}},\qquad Q=R\sqrt{\frac{C}{L}}.

These expressions apply to the ideal buck model with a resistive load and no capacitor ESR. Capacitor ESR introduces a left-half-plane zero, approximately \omegaz,ESR=1/(rCC), when other parasitics are negligible.

4. Boost Converter: Derivation and the Right-Half-Plane Zero

For a boost converter, let D'=1-D. During the on interval the inductor charges from the source and the diode is blocked. During the off interval the inductor transfers energy to the output. The averaged equations are

L\frac{di}{dt}=vg-(1-d)v,
C\frac{dv}{dt}=(1-d)i-\frac{v}{R}.

The CCM equilibrium is

V=\frac{Vg}{D'},\qquad I=\frac{V}{RD'}=\frac{Vg}{R{D'}2}.

Linearization gives

Ls\hat{i}=\hat{v}g-D'\hat{v}+V\hat{d},
Cs\hat{v}=D'\hat{i}-I\hat{d}-\frac{\hat{v}}{R}.

Eliminating \hat{i} yields

\left(LCs2+\frac{L}{R}s+{D'}2\right)\hat{v}
=D'\hat{v}g+(D'V-LIs)\hat{d}.

Therefore,

Gvd(s)=\frac{V}{D'}
\frac{1-s/\omegaz}{1+s/(Q\omega0)+(s/\omega0)2},

where

\omega0=\frac{D'}{\sqrt{LC}},\qquad
Q=RD'\sqrt{\frac{C}{L}},\qquad
\omegaz=\frac{R{D'}2}{L}.

The line-to-output transfer function is

Gvg(s)=\frac{1}{D'}
\frac{1}{1+s/(Q\omega0)+(s/\omega0)2}.

The zero at s=+\omegaz lies in the right half-plane (RHP). Immediately after duty ratio increases, the diode conducts for less time, so output current initially falls even though the eventual output voltage rises. This inverse response contributes phase lag without the magnitude attenuation associated with a left-half-plane zero. Consequently, the voltage-loop crossover is normally kept well below the RHP-zero frequency; a factor of three to ten is common, but it is a design guideline rather than a theorem.

5. Inverting Buck–Boost Converter

Let v>0 denote the magnitude of the negative physical output, so the terminal output is vo=-v. The CCM average equations are

L\frac{di}{dt}=dvg-(1-d)v,
C\frac{dv}{dt}=(1-d)i-\frac{v}{R}.

At equilibrium,

V=\frac{D}{D'}Vg,
\qquad I=\frac{V}{RD'}=\frac{DVg}{R{D'}2}.

Linearization gives

Ls\hat{i}=D\hat{v}g-D'\hat{v}+(Vg+V)\hat{d},
Cs\hat{v}=D'\hat{i}-I\hat{d}-\frac{\hat{v}}{R}.

After elimination,

\left(LCs2+\frac{L}{R}s+{D'}2\right)\hat{v}
=DD'\hat{v}g+(Vg-LIs)\hat{d}.

For output magnitude,

Gvd(s)=\frac{Vg}{{D'}2}
\frac{1-s/\omegaz}{1+s/(Q\omega0)+(s/\omega0)2},

with

\omega0=\frac{D'}{\sqrt{LC}},\qquad
Q=RD'\sqrt{\frac{C}{L}},\qquad
\omegaz=\frac{R{D'}2}{LD}.

For the signed terminal voltage vo=-v, the transfer functions acquire an additional minus sign. As in the boost converter, the RHP zero restricts voltage-loop bandwidth.

6. Feedback Structure and Loop Gain

For a negative-feedback voltage loop, let C(s) be the compensator, Fm(s) the PWM modulator, Gvd(s) the power stage and H(s) the sensor. The loop gain is

T(s)=C(s)Fm(s)Gvd(s)H(s).

For a ramp of peak-to-peak amplitude Vm, the low-frequency modulator gain is approximately Fm=1/Vm duty per volt, provided the command remains within the ramp limits.

Negative feedback control structure for a power converter +− C(s) PWMFₘ(s) ConverterGᵥd(s) H(s) vref v
Negative feedback control structure for a power converter
Figure: Negative feedback control structure for a power converter

Figure: Standard negative-feedback voltage-control loop.

If the open-loop plant has no unstable poles, adequate gain and phase margins provide useful—but not absolute—robustness indicators. For systems with RHP poles, Nyquist encirclement conditions must explicitly be checked. Typical nominal targets are phase margin of 45°–70° and gain margin above 6–10 dB, followed by tolerance and delay analysis.

7. Compensator Structures

A Type-II compensator may be written as

CII(s)=\frac{Kc}{s}\frac{1+s/\omegaz}{1+s/\omegap}.

It contains integral action, one zero and one high-frequency pole. It is commonly suitable for a dominant-pole plant or for a buck converter with crossover well below its LC resonance.

A Type-III compensator contains two zeros and two finite high-frequency poles in addition to the integrator:

CIII(s)=\frac{Kc}{s}
\frac{(1+s/\omegaz1)(1+s/\omegaz2)}
{(1+s/\omegap1)(1+s/\omegap2)}.

It can provide substantial phase boost around an LC resonance. It cannot cancel an RHP zero because stable cancellation would require an unstable controller pole. Attempting such cancellation is structurally unsafe.

Worked Example: Type-II Design and Verified Phase Margin

Consider an ideal buck converter with

  • Vg=48\ V, V=12\ V;
  • L=20\ \mu H, C=100\ \mu F, R=3\ \Omega;
  • sensor gain H=0.1;
  • PWM ramp amplitude Vm=3.02\ V; and
  • desired crossover fc=1\ kHz.

The LC natural frequency is

f0=\frac{1}{2\pi\sqrt{LC}}
=\frac{1}{2\pi\sqrt{(20\times10-6)(100\times10-6)}}
\approx3.56\ \text{kHz}.

Thus the selected crossover is below, not above, resonance.

At \omegac=2\pi(1000)=6283\ rad/s,

|\Deltab(j\omegac)|
=\sqrt{(1-LC\omegac2)2+(L\omegac/R)2}
\approx0.9220.

Hence

|Gvd(j\omegac)|=\frac{48}{0.9220}\approx52.06\ \text{V/duty}.

The combined power-stage, modulator and sensor magnitude is

|FmGvdH|=\frac{52.06(0.1)}{3.02}\approx1.724.

Choose fz=1\ kHz and fp=20\ kHz. Excluding Kc, the compensator magnitude at crossover is

\left|\frac{1}{j\omegac}
\frac{1+j\omegac/\omegaz}{1+j\omegac/\omegap}\right|
=\frac{\sqrt{2}}{6283\sqrt{1+0.052}}
\approx2.25\times10-4\ \text{s}.

The unity-gain condition gives

Kc=\frac{1}{(1.724)(2.247\times10-4)}
\approx2.58\times103\ \text{s}-1.

The plant phase is approximately

\angle Gvd\approx-\tan-1\left(\frac{0.04189}{0.92104}\right)=-2.60^\circ.

The compensator phase is

\angle CII=-90^\circ+45^\circ-\tan-1(0.05)
\approx-47.86^\circ.

Neglecting switching, computation and sensing delays, the loop phase is about -50.46^\circ, giving

PM\approx180^\circ-50.46^\circ=129.5^\circ.

The design therefore greatly exceeds a minimum 60° target; it does not produce a 60° margin. Such a high nominal margin results from choosing crossover well below resonance. Practical delay and parasitic models reduce it, but a substantially faster response would require a deliberately redesigned crossover and usually a Type-III compensator.

8. Current-Mode Control and Sampled-Data Instability

Current-mode control places a fast inductor-current loop inside a slower voltage loop. Its benefits include cycle-by-cycle current limiting, improved line rejection and an outer plant that is often closer to first order. Peak current-mode control is nevertheless a sampled-data system because the switch decision occurs once per cycle.

For a buck converter, let:

  • m1=(Vg-V)/L be the positive on-state current slope;
  • m2=V/L be the magnitude of the negative off-state slope; and
  • ma be the externally added compensation-ramp slope.

A small perturbation in the beginning-of-cycle current follows the approximate cycle map

\hat{i}n+1=\lambda\hat{i}n,
\qquad
\lambda=\frac{ma-m2}{m1+ma}.

Local sampled-data stability requires |\lambda|<1, which gives

ma>\frac{m2-m1}{2}.

When ma=0, \lambda=-m2/m1=-D/(1-D). The familiar instability therefore occurs for D>0.5. Equality is marginal in the ideal model.

Numerical Slope-Compensation Example

For Vg=24\ V, V=18\ V, L=20\ \mu H and fs=200\ kHz,

m1=\frac{6}{20\ \mu H}=0.30\ \text{A}/\mu\text{s},
\qquad
m2=\frac{18}{20\ \mu H}=0.90\ \text{A}/\mu\text{s}.

The minimum ideal compensation slope is greater than 0.30\ A/\mu s. Selecting ma=0.45\ A/\mu s gives

\lambda=\frac{0.45-0.90}{0.30+0.45}=-0.60,

which is stable. Since the switching period is 5\ \mu s, the added current-ramp excursion is 0.45\times5=2.25\ A per cycle.

9. Digital and Sampled-Data Models

For a continuous linearized model

\dot{x}=Ax+Bu,

sampled every Ts seconds with a zero-order-held input, the exact discrete model is

x[k+1]=\Phi x[k]+\Gamma u[k],
\Phi=eATs,\qquad
\Gamma=\int0TseA\tauB\,d\tau.

The approximation \Gamma\approx BTs is valid only when state evolution over one sample is small. Exact matrix-exponential discretization is preferable for high-bandwidth control.

A one-sample computational delay contributes z-1, corresponding on the unit circle to phase lag -\omega Ts. A zero-order hold contributes approximately half-sample delay at frequencies well below Nyquist, in addition to its sinc-shaped magnitude response. These effects can materially reduce phase margin.

A crossover below one-tenth of the sampling frequency is a common conservative starting point, not a universal stability condition. Multirate sampling, predictive duty updates and computation synchronized to PWM edges can permit different trade-offs.

Quantization introduces limit cycles when the duty or measured-voltage resolution is coarse. Anti-windup is required when duty saturation conflicts with integral action. Digital models should also represent ADC delay, PWM update timing, sensor filtering and timer resolution.

Averaged models cannot predict period-doubling or switching-frequency sidebands. Exact sampled-data analysis instead constructs a one-cycle map from the switched state-transition matrices. Its Jacobian, sometimes called the monodromy matrix, determines orbital stability: every nontrivial eigenvalue must lie inside the unit circle.

10. Impedance-Based and Multiloop Stability

Converters are often connected through EMI filters, cables, batteries or other regulated converters. A subsystem can be internally stable yet become unstable after interconnection.

For a source converter with output impedance Zs feeding a load with input impedance Zl, the minor-loop gain is commonly formed as

Tm(s)=\frac{Zs(s)}{Zl(s)}.

Stability must be assessed using Nyquist analysis with the applicable source and load terminations. The informal condition |Zs|<|Zl| over interaction frequencies is a useful sufficient design objective under restricted conditions, but it is not a general theorem.

A tightly regulated constant-power load has incremental resistance

rin=\frac{dV}{dI}=-\frac{V2}{P},

because I=P/V. Its negative incremental impedance can reduce damping. Multivariable converters and grid-connected systems may require impedance matrices, sequence-domain models or generalized Nyquist criteria.

11. Illustrative Case: 2 kW Digital Boost Converter

Background

An engineering team must regulate a fictional 2 kW DC bus from 200 V to 400 V using a CCM boost converter. The switching frequency is 100 kHz, with L=500\ \mu H and C=470\ \mu F. The case is illustrative rather than a product specification.

Problem

The controller must reject input disturbances while avoiding instability caused by the LC dynamics, the boost RHP zero and digital delay.

Analysis

At rated power,

R=\frac{V2}{P}=\frac{4002}{2000}=80\ \Omega,
\qquad D=1-\frac{200}{400}=0.5.

The output current is 5 A and the average inductor current is

I=\frac{V}{RD'}=10\ \text{A}.

The ideal dynamic parameters are

\omega0=\frac{0.5}{\sqrt{(500\times10-6)(470\times10-6)}}
\approx1031\ \text{rad/s},

so f0\approx164\ Hz. Also,

Q=80(0.5)\sqrt{\frac{470}{500}}\approx38.8.

This unusually high ideal value indicates weak damping; practical losses reduce it. The RHP zero is

\omegaz=\frac{80(0.5)2}{500\times10-6}
=40000\ \text{rad/s},

or fz\approx6.37\ kHz.

Approach

A cascaded architecture is selected:

  1. an inner average-current loop with a proposed crossover near 2 kHz;
  2. an outer voltage loop near 100 Hz;
  3. synchronized ADC sampling and PWM updating;
  4. anti-windup, soft start and hardware overcurrent protection; and
  5. validation over input voltage, load, temperature and component tolerances.

The 2 kHz current-loop target is below approximately one-third of the RHP-zero frequency and far below the 100 kHz sampling frequency. The outer voltage loop is much slower than the current loop, supporting approximate loop separation. Exact margins must nevertheless be computed from the complete digital model.

At the nominal operating point, the boost current slopes have equal magnitude:

m1=\frac{200}{500\ \mu H}=0.40\ \text{A}/\mu\text{s},
\qquad
m2=\frac{400-200}{500\ \mu H}=0.40\ \text{A}/\mu\text{s}.

If peak current programming is used, zero artificial ramp is marginal in the ideal sampled-data model. Choosing ma=0.20\ A/\mu s gives \lambda=-1/3, providing damping against period-doubling.

Outcome

The analysis prevents selection of an outer voltage-loop bandwidth close to the RHP zero and identifies the need to include parasitic damping and digital delay. Hardware validation should include line steps, load steps, startup, current limiting, output short circuit and impedance interaction with the source filter.

Learning Points

  • DC conversion ratio alone provides no information about dynamic limitations.
  • The RHP zero is determined by operating point, load and inductance.
  • Cascaded current and voltage loops can separate fast protection from bus regulation.
  • Averaged, sampled-data and switching models answer different questions and should be used together.

12. Model Limitations, Validation and Contemporary Practice

Nonidealities

Inductor resistance, capacitor ESR, semiconductor voltage drops and dead time alter both equilibrium and dynamics. Magnetic saturation makes inductance current-dependent. Thermal drift changes resistance and sensor gain. A credible design includes these effects when they influence crossover, damping or protection.

Large-signal behavior

Small-signal models do not predict startup, mode transitions or saturation recovery. Large-signal averaged models, phase-plane analysis and time-domain switching simulation are required. Controllers should include reference ramps, duty limits, current limits and anti-windup.

Identification and AI-assisted design

Frequency-response analyzers can identify control-to-output and loop-gain responses directly on hardware. Recursive estimation can track parameter drift. Machine-learning models may assist anomaly detection or surrogate modeling, but stability-critical control should retain verifiable constraints, bounded operating domains and deterministic fallback protection. Training data alone do not establish closed-loop stability.

Safety, governance and regulation

High-power converter control is safety-critical. Designs should address isolation, creepage and clearance, fault containment, electromagnetic compatibility, cybersecurity of update interfaces and traceable firmware configuration. Applicable standards depend on the sector—for example, IEC 62477-1 for power electronic converter safety and IEC 61000-series requirements for electromagnetic compatibility. Compliance does not replace engineering risk assessment.

Recommended professional workflow

  1. Define operating range, modes, loads and protection states.
  2. Derive the nonlinear averaged model and verify its equilibrium.
  3. Linearize at multiple worst-case operating points.
  4. include parasitics, sensor dynamics, modulator gain and delays.
  5. Select crossover below nonminimum-phase and sampling constraints.
  6. assess gain, phase, sensitivity and complementary sensitivity.
  7. perform tolerance and impedance-interaction studies.
  8. validate using nonlinear switching simulation and hardware measurements.
  9. test saturation, startup, faults and mode transitions.
  10. document assumptions, model versions and safety limits.

Chapter Summary

Dynamic converter models connect circuit operation to control-system design. State-space averaging produces a nonlinear low-frequency representation, while perturbation and linearization yield transfer functions around a specified operating point. The buck converter has a minimum-phase duty-to-output response under ideal CCM assumptions, and its open-loop output impedance for current drawn from the output is Ls/[LCs2+(L/R)s+1].

Boost and inverting buck–boost converters possess RHP zeros because an increase in duty ratio initially reduces energy delivery to the output. Their natural frequency, quality factor and RHP-zero frequency depend strongly on duty ratio and load. These features impose fundamental bandwidth constraints.

Voltage-mode compensators shape loop gain, whereas current-mode control introduces a fast current loop and cycle-by-cycle protection. Peak current-mode control requires sampled-data analysis; adequate slope compensation prevents period-doubling. Digital implementation further introduces zero-order hold, computation delay, quantization and PWM update effects. Robust converter design therefore combines averaged, sampled-data and switching models with experimental validation, tolerance analysis and safety-conscious implementation.

Key Terms

State-space averaging: Replacement of switching subinterval dynamics by their duty-weighted average.

Operating point: Steady-state values about which a nonlinear model is linearized.

Small-signal model: Local linear approximation relating incremental variables.

Control-to-output transfer function: Ratio of output perturbation to duty-ratio perturbation.

Line-to-output transfer function: Ratio of output perturbation to input-voltage perturbation.

Output impedance: Incremental relationship between output-voltage change and load-current disturbance.

Continuous-conduction mode: Operation in which inductor current does not reach zero during a switching cycle.

Right-half-plane zero: Nonminimum-phase zero that causes inverse response and additional phase lag.

Natural frequency: Characteristic frequency associated with an energy-storage pole pair.

Quality factor: Dimensionless measure of damping or resonant peaking.

Loop gain: Product of gains around a feedback loop when opened at a defined point.

Phase margin: Additional phase lag required at gain crossover to reach the instability boundary.

Type-II compensator: Integral compensator with one finite zero and one finite pole.

Type-III compensator: Integral compensator with two finite zeros and two finite poles.

Slope compensation: Artificial ramp added to stabilize peak current-mode control.

Sampled-data model: Model describing state evolution from one sampling or switching instant to the next.

Monodromy matrix: Jacobian of a one-period state-transition map used to assess orbital stability.

Zero-order hold: Reconstruction that holds each digital control value constant between updates.

Constant-power load: Load whose regulation produces negative incremental input resistance.

Anti-windup: Mechanism that prevents excessive integrator accumulation during actuator saturation.

Review Questions

Short Answer Questions

  1. Why is a converter averaged model generally nonlinear even when all passive components are linear?
  2. Define the control-to-output transfer function.
  3. What physical mechanism creates the boost converter's RHP zero?
  4. Why does computational delay reduce phase margin?
  5. What is the purpose of slope compensation in peak current-mode control?

Long Answer Questions

  1. Derive the ideal CCM buck converter's duty-to-output and load-current-to-output transfer functions.
  2. Starting from its two switching states, derive the boost converter's averaged model and define \omega0, Q and \omegaz.
  3. Compare voltage-mode, peak current-mode and average current-mode control in terms of dynamics, implementation and protection.
  4. Explain how parasitics, sampling delay and component tolerances should be incorporated into a robust control design.
  5. Discuss why gain and phase margins alone may be insufficient for converters interconnected through input filters and regulated loads.

Analytical / Application Questions

  1. A 36 V-to-12 V buck converter has L=30\ \mu H, C=220\ \mu F and R=2\ \Omega. Derive its ideal control-to-output transfer function and calculate its natural frequency and quality factor.
  2. For a boost converter operating at D=0.6, determine how its RHP-zero frequency changes when the load resistance doubles while all other parameters remain fixed. Explain the control implication.
  3. Design a slope-compensation ramp for a peak current-mode buck converter with specified Vg, V, L and fs. Verify stability using the sampled-data eigenvalue and calculate the ramp excursion per switching period.

Multiple Choice Questions with Answers

Question 1

For the ideal CCM buck model, with load-disturbance current defined as positive when drawn from the output, which expression is the output impedance Zo=-\hat{v}/\hat{i}load?

A. \frac{Ls}{LCs2+(L/R)s+1}

B. \frac{Ls+R}{LCs2+(L/R)s+1}

C. \frac{R}{LCs2+(L/R)s+1}

D. \frac{1}{LCs2+(L/R)s+1}

Correct Answer: A. \frac{Ls}{LCs2+(L/R)s+1}

Question 2

For an ideal CCM boost converter, the control-to-output RHP-zero frequency is:

A. \omegaz=1/\sqrt{LC}

B. \omegaz=RD'/L

C. \omegaz=R{D'}2/L

D. \omegaz=L/(R{D'}2)

Correct Answer: C. \omegaz=R{D'}2/L

Question 3

What is the ideal boost converter's natural frequency under the assumptions used in the chapter?

A. \omega0=D'/\sqrt{LC}

B. \omega0=1/(D'\sqrt{LC})

C. \omega0=D'/LC

D. \omega0=R{D'}2/L

Correct Answer: A. \omega0=D'/\sqrt{LC}

Question 4

Which phenomenon generally cannot be predicted by a conventional low-frequency state-space averaged model?

A. Steady-state conversion ratio

B. Low-frequency load-step response

C. Period-doubling oscillation

D. LC resonant frequency

Correct Answer: C. Period-doubling oscillation

Question 5

A peak current-mode buck converter has m1=0.30\ A/\mu s, m2=0.90\ A/\mu s and ma=0.45\ A/\mu s. What is its approximate sampled-data eigenvalue?

A. −0.60

B. −0.33

C. +0.60

D. +1.80

Correct Answer: A. −0.60

Question 6

At fc=fz=1\ kHz and fp=20\ kHz, what is the magnitude of (1/j\omegac)(1+j\omegac/\omegaz)/(1+j\omegac/\omegap)?

A. 2.25\times10-4\ s

B. 1.59\times10-4\ s

C. 2.25\times10-3\ s

D. 6.28\times103\ s

Correct Answer: A. 2.25\times10-4\ s

Question 7

In the worked buck-compensator example, neglecting delays and parasitics, the nominal phase margin is approximately:

A. 30°

B. 60°

C. 90°

D. 129.5°

Correct Answer: D. 129.5°

Question 8

For exact zero-order-hold discretization of \dot{x}=Ax+Bu, which expression defines the discrete state matrix?

A. \Phi=I+ATs in all cases

B. \Phi=eATs

C. \Phi=A/Ts

D. \Phi=(sI-A)-1

Correct Answer: B. \Phi=eATs

Question 9

For L=20\ \mu H and C=100\ \mu F, the ideal LC natural frequency is approximately:

A. 356 Hz

B. 1.00 kHz

C. 3.56 kHz

D. 35.6 kHz

Correct Answer: C. 3.56 kHz

Question 10

In the 2 kW illustrative boost-converter case, what is the nominal RHP-zero frequency?

A. 164 Hz

B. 1.03 kHz

C. 6.37 kHz

D. 40.0 kHz

Correct Answer: C. 6.37 kHz

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