Unit 5: Three-Phase Inverters, Space Vector PWM (SVPWM), and Harmonic Minimization

Unit 5: Resonant and soft-switching conversion

Engineering situation

Resonant networks trade frequency-dependent impedance against switching transitions and circulating current. In a resonant inverter, the impedance near resonance can amplify current even when useful load power is modest. Zero-voltage switching and zero-current switching refer to transitions at particular instants; neither proves zero overall loss.

Shared numerical scenario

A normalized series RLC example anchors this unit. Starting from L=10 µH and C=100 nF, we calculate a resonance frequency and explore detuning, quality factor and sensitivity. The simulator stays linear and sinusoidal; it does not pretend to solve every nonlinear LLC operating mode.

Intended competence

Learners will locate resonance, distinguish series resonance from LLC magnetizing behavior, reason about soft-switching boundaries and compare a loss reduction with the added magnetics and control complexity.

Assumptions and model boundary

This unit uses specific equations at specific operating points; a model must not be extended merely because it produces a number outside the stated range. In particular, the switching network may be averaged over a PWM period for a slow state calculation, while magnetic reset, terminal-voltage stress and semiconductor switching energy demand individual switching intervals. Keep the mechanical, magnetic and electrical energy variables separate where appropriate. Every diagram should identify a reference node, current direction and whether the axes show peak, average, or RMS quantities. Where an external network or motor is discussed, the waveform is software-generated for learning and does not authorize connection to an energized system.

Unit reading route

Read Lessons 5.1 through 5.4 in sequence, then use the [unit simulation](../simulations/model-05.html). Complete the unit project before the assessment. Preserve the original scenario as a baseline so parameter changes are attributable; do not change source, loading and control law simultaneously. When citing a numerical result, write the values, units and limit cases, then label it as ideal analytical, simplified dynamic model, computed simulation or actual measurement. No measurement claims are made here.

Technical review checkpoint

Resonant gain is a function of frequency and loading rather than a single fixed transformer turns ratio. A soft-switching assumption can be true at one operating point and false at another. The most dangerous regions may be startup and light load, not maximum delivered power.

Plot voltage gain or current magnitude on a frequency axis using fixed, documented component values; repeat with at least two load values. Locate the resonant peak, mark the chosen command range, and explain what a linear model cannot tell you about switch-node commutation.

A good explanation specifies the assumptions under which a relation is true and names an experiment or simulation capable of detecting when it fails. A numerical waveform can agree with its own programmed equations and still be incapable of predicting a real apparatus. Use the following assessment to distinguish those two forms of evidence.

Lesson 5.1: Series resonance and normalized impedance

Position: Unit 5, Resonant and soft-switching conversion. Reading level: undergraduate circuit analysis, switching converters and elementary calculus. Learning claim: distinguish the mathematical approximation from the physical device-level consequences. Status: unreviewed teaching chapter.

Physical picture and mechanism

A series RLC circuit reaches zero net reactance when inductive and capacitive reactances cancel at one frequency. At that point its impedance is resistive and its current can peak. An actual resonant power converter adds switching harmonics, nonlinear rectifier loading and a control-dependent operating point.

The practical boundary of the system matters. Draw where energy enters, where useful energy leaves, what storage changes within the process and where heat or field energy is likely to be lost. Define all voltage polarities before changing reference frames; a reported sign is physically meaningful only relative to a declared node or direction. The natural interval for averaging must also be stated: a switching-period equation, a line-frequency RMS result and a slowly varying thermal estimate describe different aspects of the same apparatus. One cannot simply average all three over an arbitrary interval and call the result a design guarantee.

Governing mathematical relation

Resonance frequency for an ideal series LC is fr=1/(2π√(LC)). For sinusoidal excitation, |Z|=√(R²+(ωL−1/(ωC))²), and I_rms=V_rms/|Z|. A dimensionless quality factor can be written Q=ωr L/R for the series model.

Write the baseline relation symbolically first, then test it against a dimensional check and an elementary limiting case. For a variable expressed as a rate, verify what time base is implicit: per switching period, per electrical cycle, per unit mechanical rotation or per second. If the equation assumes continuous conduction, a linear magnetic inductance, an ideal waveform or a balanced three-phase input, say so before substituting numerical values. For a measured value, specify sensor position and measurement bandwidth; for a computed value, identify the exact source equation.

Worked numerical example with interpretation

Using L=10 µH, C=100 nF gives fr≈159.15 kHz. If R=2 Ω, the ideal series reactance at resonance cancels and a 10 V RMS sinusoid produces 5 A RMS. Q≈(2π×159155×10e−6)/2≈5.

A credible numerical answer includes both a displayed number and its physical meaning. If a computed voltage is a peak, it cannot be directly used as an RMS rating. If a frequency is a natural resonance, it cannot be presented as a measured closed-loop bandwidth. If a result is an ideal output voltage, it cannot be equated with the real part's dielectric withstand requirement. Use at least three significant digits in the intermediate steps and round the final display to the precision actually supported by input parameters. A second independent check, such as energy conservation, a complementary voltage, or the expected response as one variable approaches zero, should be written beside the arithmetic.

Derivation workflow

Start from a physical definition and then introduce any simplification. Before calculating, sketch or describe the states that make the claimed equation meaningful. A derived relation is usually an operating-point statement, not a guarantee across startup, overload and faulted conditions. Distinguish independent inputs from outputs: a duty ratio may be commanded by the regulator, but a peak current is determined jointly by source voltage, load, storage and event timing.

Check dimensions at every substitution. In particular, microseconds and nanoseconds differ by a factor of one thousand; degrees and radians require explicit conversion before inserting a frequency; and a quantity in electrical radians per second is not a shaft speed in revolutions per minute. The direction of energy flow should be consistent with the current-arrow convention shown beside the circuit or graph.

Important failure modes and nonideal boundaries

This RLC relation assumes an explicit real series resistance, not an uncontrolled switching bridge. A rectifier with variable loading is not accurately represented by the same constant R at all frequencies.

These limitations are not a minor footnote: they are the conditions under which this chapter's conclusion could reverse. Separate the design intent from the semiconductor's transient stress, and the requested controller action from the physical switching state. A controller display can be numerically smooth while its switching node is overshooting; a motor speed command can be well behaved while the DC bus is absorbing excessive regenerative energy. A waveform generated by a hand-written program is only as complete as the modeled parasitics and fault behavior.

Engineering judgment

Plot magnitude and phase versus normalized frequency for at least three resistance values. Explain why a high-Q frequency response is more sensitive to manufacturing tolerance.

An engineering comparison should use a common reference case and explicitly report one metric that improves and one that could worsen. For example, increasing switching frequency may reduce some storage ripple yet increase switching heat and radiated emissions; adding capacitance may smooth a voltage while raising surge energy and discharge requirements; increasing control bandwidth may improve tracking while reducing delay tolerance. The tradeoff depends on this lesson's topology and assumptions. Where the text omits a datasheet value, test configuration or certification criterion, the correct output is 'not established' rather than an invented margin.

Focused exercise set

Exercise A — reconstruct. Rewrite the governing relation above using named inputs and outputs. Draw or describe the source, load, storage or reference frame that makes it valid. Mark whether the calculated result is a switching-period average, fundamental value, transient peak, energy, current, power, frequency or loss.

Exercise B — parameter sensitivity. Reproduce the numerical case but change the most influential stated input by +10% while keeping all other inputs fixed. Show the substituted equation and the new number. Explain whether the response is expected to be linear, reciprocal, quadratic or nonlinear, and whether the modified point remains inside the same assumed operating regime.

Exercise C — challenge the assumption. Identify one concrete event, such as a load step, missing feedback signal, frequency detuning, angle-estimation error, current sign reversal or temperature change, that makes the basic calculation incomplete. State which extra measurement or model parameter would be necessary to proceed.

Exercise D — compare choices. Evaluate a second solution concept, not simply a different numerical parameter. Compare source-current stress, controllability, complexity and validation burden. Give a reason the choice could change at light load or at a different source voltage.

Exercise E — audit someone else's answer. A classmate reports a precise 'safe and efficient' result after using only the simplified equation in this lesson. Write a six-line technical review identifying one valid quantitative conclusion, one ignored uncertainty, one protection concern, one proposed simulation, one missing empirical test and the exact boundary of the claim.

Answer guidance and grading rubric

For Exercise A, the key is a consistent sign convention and correct categorization of the calculated quantity. In Exercise B the arithmetic must start from the same stated units, and a legitimate answer must note when a changed parameter would require a new operating regime. In Exercise C the missing variable must materially affect the behavior, rather than being a vague appeal to 'more data'. Exercise D earns full credit only when the alternate architecture changes an engineering tradeoff; merely changing a plotted color is not a design option. Exercise E must not describe software results as measurements or claim an external safety approval. Partial credit is appropriate for an otherwise correct derivation with an explicit, honest limitation; no credit for physically inconsistent units or an unstated phase-voltage reference.

Bridge to the unit model

Operating points across resonance: Resonant gain is a function of frequency and loading rather than a single fixed transformer turns ratio. A soft-switching assumption can be true at one operating point and false at another. The most dangerous regions may be startup and light load, not maximum delivered power.

Plot voltage gain or current magnitude on a frequency axis using fixed, documented component values; repeat with at least two load values. Locate the resonant peak, mark the chosen command range, and explain what a linear model cannot tell you about switch-node commutation.

The companion simulation uses deterministic, intentionally simplified equations. Preserve input settings and screenshot or export the computed parameters together with any graph. A successful interactive plot demonstrates software operation and internal mathematical consistency for the declared formulas; it does not prove real component compatibility. Return to the central question of this chapter: what is calculated, what is assumed, and what is still unknown?

Lesson 5.2: LLC tank and magnetizing branch

Position: Unit 5, Resonant and soft-switching conversion. Reading level: undergraduate circuit analysis, switching converters and elementary calculus. Learning claim: distinguish the mathematical approximation from the physical device-level consequences. Status: unreviewed teaching chapter.

Physical picture and mechanism

The LLC converter adds magnetizing inductance to a series resonant inductance and capacitance. Its frequency-dependent gain can be shaped by the ratio Lm/Lr and the load reflected through the transformer. This extra branch enables different gain and soft-switching characteristics from a simple series RLC circuit.

The practical boundary of the system matters. Draw where energy enters, where useful energy leaves, what storage changes within the process and where heat or field energy is likely to be lost. Define all voltage polarities before changing reference frames; a reported sign is physically meaningful only relative to a declared node or direction. The natural interval for averaging must also be stated: a switching-period equation, a line-frequency RMS result and a slowly varying thermal estimate describe different aspects of the same apparatus. One cannot simply average all three over an arbitrary interval and call the result a design guarantee.

Governing mathematical relation

Two characteristic frequencies often appear in elementary tank analysis: fr=1/(2π√(Lr Cr)) and a lower idealized frequency fm=1/(2π√((Lr+Lm)Cr)). A full gain curve additionally requires an appropriate fundamental-harmonic model and reflected load definition.

Write the baseline relation symbolically first, then test it against a dimensional check and an elementary limiting case. For a variable expressed as a rate, verify what time base is implicit: per switching period, per electrical cycle, per unit mechanical rotation or per second. If the equation assumes continuous conduction, a linear magnetic inductance, an ideal waveform or a balanced three-phase input, say so before substituting numerical values. For a measured value, specify sensor position and measurement bandwidth; for a computed value, identify the exact source equation.

Worked numerical example with interpretation

For Lr=10 µH, Lm=50 µH and Cr=100 nF, fr≈159.15 kHz and fm≈64.97 kHz. Their separation quantifies the available resonant range but does not determine the exact DC output gain or switch stress.

A credible numerical answer includes both a displayed number and its physical meaning. If a computed voltage is a peak, it cannot be directly used as an RMS rating. If a frequency is a natural resonance, it cannot be presented as a measured closed-loop bandwidth. If a result is an ideal output voltage, it cannot be equated with the real part's dielectric withstand requirement. Use at least three significant digits in the intermediate steps and round the final display to the precision actually supported by input parameters. A second independent check, such as energy conservation, a complementary voltage, or the expected response as one variable approaches zero, should be written beside the arithmetic.

Model comparison workflow

A second model is useful only if it changes an identifiable assumption. Compare an ideal lossless expression with a bounded nonideal version, or a fixed load with a changed load; do not modify several unrelated quantities and attribute the entire difference to a single mechanism. Make a table showing which equations survive the changed operating regime and which must be derived again.

Include the neglected process in plain language even when it cannot be computed: leakage inductance, dead time, load-angle error, winding temperature or non-sinusoidal current can change a conclusion. Giving an uncalibrated guessed correction factor to hide that omission is less useful than stating that the quantity remains unknown.

Important failure modes and nonideal boundaries

Do not infer safe soft-switching operation merely by selecting a switching frequency between these values. Actual gain depends on load, transformer ratio, rectifier mode and parasitic capacitances.

These limitations are not a minor footnote: they are the conditions under which this chapter's conclusion could reverse. Separate the design intent from the semiconductor's transient stress, and the requested controller action from the physical switching state. A controller display can be numerically smooth while its switching node is overshooting; a motor speed command can be well behaved while the DC bus is absorbing excessive regenerative energy. A waveform generated by a hand-written program is only as complete as the modeled parasitics and fault behavior.

Engineering judgment

Construct an assumptions table before using an LLC gain curve. State whether the transformer magnetizing branch is linear and which harmonics are ignored in the chosen approximation.

An engineering comparison should use a common reference case and explicitly report one metric that improves and one that could worsen. For example, increasing switching frequency may reduce some storage ripple yet increase switching heat and radiated emissions; adding capacitance may smooth a voltage while raising surge energy and discharge requirements; increasing control bandwidth may improve tracking while reducing delay tolerance. The tradeoff depends on this lesson's topology and assumptions. Where the text omits a datasheet value, test configuration or certification criterion, the correct output is 'not established' rather than an invented margin.

Focused exercise set

Exercise A — reconstruct. Rewrite the governing relation above using named inputs and outputs. Draw or describe the source, load, storage or reference frame that makes it valid. Mark whether the calculated result is a switching-period average, fundamental value, transient peak, energy, current, power, frequency or loss.

Exercise B — parameter sensitivity. Reproduce the numerical case but change the most influential stated input by +10% while keeping all other inputs fixed. Show the substituted equation and the new number. Explain whether the response is expected to be linear, reciprocal, quadratic or nonlinear, and whether the modified point remains inside the same assumed operating regime.

Exercise C — challenge the assumption. Identify one concrete event, such as a load step, missing feedback signal, frequency detuning, angle-estimation error, current sign reversal or temperature change, that makes the basic calculation incomplete. State which extra measurement or model parameter would be necessary to proceed.

Exercise D — compare choices. Evaluate a second solution concept, not simply a different numerical parameter. Compare source-current stress, controllability, complexity and validation burden. Give a reason the choice could change at light load or at a different source voltage.

Exercise E — audit someone else's answer. A classmate reports a precise 'safe and efficient' result after using only the simplified equation in this lesson. Write a six-line technical review identifying one valid quantitative conclusion, one ignored uncertainty, one protection concern, one proposed simulation, one missing empirical test and the exact boundary of the claim.

Answer guidance and grading rubric

For Exercise A, the key is a consistent sign convention and correct categorization of the calculated quantity. In Exercise B the arithmetic must start from the same stated units, and a legitimate answer must note when a changed parameter would require a new operating regime. In Exercise C the missing variable must materially affect the behavior, rather than being a vague appeal to 'more data'. Exercise D earns full credit only when the alternate architecture changes an engineering tradeoff; merely changing a plotted color is not a design option. Exercise E must not describe software results as measurements or claim an external safety approval. Partial credit is appropriate for an otherwise correct derivation with an explicit, honest limitation; no credit for physically inconsistent units or an unstated phase-voltage reference.

Bridge to the unit model

Operating points across resonance: Resonant gain is a function of frequency and loading rather than a single fixed transformer turns ratio. A soft-switching assumption can be true at one operating point and false at another. The most dangerous regions may be startup and light load, not maximum delivered power.

Plot voltage gain or current magnitude on a frequency axis using fixed, documented component values; repeat with at least two load values. Locate the resonant peak, mark the chosen command range, and explain what a linear model cannot tell you about switch-node commutation.

The companion simulation uses deterministic, intentionally simplified equations. Preserve input settings and screenshot or export the computed parameters together with any graph. A successful interactive plot demonstrates software operation and internal mathematical consistency for the declared formulas; it does not prove real component compatibility. Return to the central question of this chapter: what is calculated, what is assumed, and what is still unknown?

Lesson 5.3: Zero-voltage and zero-current transitions

Position: Unit 5, Resonant and soft-switching conversion. Reading level: undergraduate circuit analysis, switching converters and elementary calculus. Learning claim: distinguish the mathematical approximation from the physical device-level consequences. Status: unreviewed teaching chapter.

Physical picture and mechanism

Switching loss arises when current and voltage overlap during transitions. ZVS turns on a device when its voltage is near zero; ZCS turns it on or off with near-zero current. Both depend on stored resonant energy, device capacitances, current direction and actual gate timing.

The practical boundary of the system matters. Draw where energy enters, where useful energy leaves, what storage changes within the process and where heat or field energy is likely to be lost. Define all voltage polarities before changing reference frames; a reported sign is physically meaningful only relative to a declared node or direction. The natural interval for averaging must also be stated: a switching-period equation, a line-frequency RMS result and a slowly varying thermal estimate describe different aspects of the same apparatus. One cannot simply average all three over an arbitrary interval and call the result a design guarantee.

Governing mathematical relation

A first estimate for energy held in a device output capacitance is Eoss≈½Coss V² if Coss is treated as constant. Because actual Coss is voltage-dependent, device-specific integrated Eoss(V) data are preferred. A simple per-cycle switching-energy term gives P≈Esw fs.

Write the baseline relation symbolically first, then test it against a dimensional check and an elementary limiting case. For a variable expressed as a rate, verify what time base is implicit: per switching period, per electrical cycle, per unit mechanical rotation or per second. If the equation assumes continuous conduction, a linear magnetic inductance, an ideal waveform or a balanced three-phase input, say so before substituting numerical values. For a measured value, specify sensor position and measurement bandwidth; for a computed value, identify the exact source equation.

Worked numerical example with interpretation

At Coss=200 pF and 400 V, a constant-capacitance approximation gives Eoss=0.5×200e−12×160000=16 µJ. At 100 kHz that corresponds to 1.6 W if the full energy is dissipated each event. Actual energy recovery and device nonlinearities change this estimate.

A credible numerical answer includes both a displayed number and its physical meaning. If a computed voltage is a peak, it cannot be directly used as an RMS rating. If a frequency is a natural resonance, it cannot be presented as a measured closed-loop bandwidth. If a result is an ideal output voltage, it cannot be equated with the real part's dielectric withstand requirement. Use at least three significant digits in the intermediate steps and round the final display to the precision actually supported by input parameters. A second independent check, such as energy conservation, a complementary voltage, or the expected response as one variable approaches zero, should be written beside the arithmetic.

Measurement and inference workflow

Define what an instrument would actually observe, even though this exercise is software only. A spectrum analyzer reports a frequency-domain estimate, a current sensor reports a bandwidth-limited sample, and a thermal measurement reports temperature at a location and time. None directly measures every term in an analytical state equation. Design an independent cross-check using conservation of energy or symmetry before trusting a displayed result.

Record the intended sample rate, window, triggering event and reference node. For transient switching analyses distinguish a 10 ns peak from a 1 ms average and identify whether the probe itself could perturb the observed circuit. If a claim needs actual bench data, mark it explicitly as not yet established.

Important failure modes and nonideal boundaries

Fast transitions do not guarantee soft switching. A small resonant current at light load may be insufficient to charge and discharge device output capacitances before the command edge.

These limitations are not a minor footnote: they are the conditions under which this chapter's conclusion could reverse. Separate the design intent from the semiconductor's transient stress, and the requested controller action from the physical switching state. A controller display can be numerically smooth while its switching node is overshooting; a motor speed command can be well behaved while the DC bus is absorbing excessive regenerative energy. A waveform generated by a hand-written program is only as complete as the modeled parasitics and fault behavior.

Engineering judgment

For each claimed ZVS event, identify the energy source, the capacitor-charge route, its required time interval and a measurement criterion. Avoid the unqualified claim that soft switching eliminates all losses.

An engineering comparison should use a common reference case and explicitly report one metric that improves and one that could worsen. For example, increasing switching frequency may reduce some storage ripple yet increase switching heat and radiated emissions; adding capacitance may smooth a voltage while raising surge energy and discharge requirements; increasing control bandwidth may improve tracking while reducing delay tolerance. The tradeoff depends on this lesson's topology and assumptions. Where the text omits a datasheet value, test configuration or certification criterion, the correct output is 'not established' rather than an invented margin.

Focused exercise set

Exercise A — reconstruct. Rewrite the governing relation above using named inputs and outputs. Draw or describe the source, load, storage or reference frame that makes it valid. Mark whether the calculated result is a switching-period average, fundamental value, transient peak, energy, current, power, frequency or loss.

Exercise B — parameter sensitivity. Reproduce the numerical case but change the most influential stated input by +10% while keeping all other inputs fixed. Show the substituted equation and the new number. Explain whether the response is expected to be linear, reciprocal, quadratic or nonlinear, and whether the modified point remains inside the same assumed operating regime.

Exercise C — challenge the assumption. Identify one concrete event, such as a load step, missing feedback signal, frequency detuning, angle-estimation error, current sign reversal or temperature change, that makes the basic calculation incomplete. State which extra measurement or model parameter would be necessary to proceed.

Exercise D — compare choices. Evaluate a second solution concept, not simply a different numerical parameter. Compare source-current stress, controllability, complexity and validation burden. Give a reason the choice could change at light load or at a different source voltage.

Exercise E — audit someone else's answer. A classmate reports a precise 'safe and efficient' result after using only the simplified equation in this lesson. Write a six-line technical review identifying one valid quantitative conclusion, one ignored uncertainty, one protection concern, one proposed simulation, one missing empirical test and the exact boundary of the claim.

Answer guidance and grading rubric

For Exercise A, the key is a consistent sign convention and correct categorization of the calculated quantity. In Exercise B the arithmetic must start from the same stated units, and a legitimate answer must note when a changed parameter would require a new operating regime. In Exercise C the missing variable must materially affect the behavior, rather than being a vague appeal to 'more data'. Exercise D earns full credit only when the alternate architecture changes an engineering tradeoff; merely changing a plotted color is not a design option. Exercise E must not describe software results as measurements or claim an external safety approval. Partial credit is appropriate for an otherwise correct derivation with an explicit, honest limitation; no credit for physically inconsistent units or an unstated phase-voltage reference.

Bridge to the unit model

Operating points across resonance: Resonant gain is a function of frequency and loading rather than a single fixed transformer turns ratio. A soft-switching assumption can be true at one operating point and false at another. The most dangerous regions may be startup and light load, not maximum delivered power.

Plot voltage gain or current magnitude on a frequency axis using fixed, documented component values; repeat with at least two load values. Locate the resonant peak, mark the chosen command range, and explain what a linear model cannot tell you about switch-node commutation.

The companion simulation uses deterministic, intentionally simplified equations. Preserve input settings and screenshot or export the computed parameters together with any graph. A successful interactive plot demonstrates software operation and internal mathematical consistency for the declared formulas; it does not prove real component compatibility. Return to the central question of this chapter: what is calculated, what is assumed, and what is still unknown?

Lesson 5.4: Frequency control, load changes and protection

Position: Unit 5, Resonant and soft-switching conversion. Reading level: undergraduate circuit analysis, switching converters and elementary calculus. Learning claim: distinguish the mathematical approximation from the physical device-level consequences. Status: unreviewed teaching chapter.

Physical picture and mechanism

Frequency-controlled resonant converters operate over a range in which gain, current stress and soft-switching boundaries all move with load. A controller that simply tracks output error may accidentally command an unfavorable region during startup, a short circuit or lost feedback.

The practical boundary of the system matters. Draw where energy enters, where useful energy leaves, what storage changes within the process and where heat or field energy is likely to be lost. Define all voltage polarities before changing reference frames; a reported sign is physically meaningful only relative to a declared node or direction. The natural interval for averaging must also be stated: a switching-period equation, a line-frequency RMS result and a slowly varying thermal estimate describe different aspects of the same apparatus. One cannot simply average all three over an arbitrary interval and call the result a design guarantee.

Governing mathematical relation

The tank impedance magnitude depends on frequency, and the phase of impedance changes sign across resonance. A frequency loop also has finite update rate and measurement delay; stable tuning must consider more than the static gain slope.

Write the baseline relation symbolically first, then test it against a dimensional check and an elementary limiting case. For a variable expressed as a rate, verify what time base is implicit: per switching period, per electrical cycle, per unit mechanical rotation or per second. If the equation assumes continuous conduction, a linear magnetic inductance, an ideal waveform or a balanced three-phase input, say so before substituting numerical values. For a measured value, specify sensor position and measurement bandwidth; for a computed value, identify the exact source equation.

Worked numerical example with interpretation

For the simple series tank L=10 µH, C=100 nF and R=2 Ω, calculate |Z| at 100 kHz: XL≈6.28 Ω, XC≈15.92 Ω, difference ≈−9.64 Ω, total |Z|≈9.85 Ω. A 10 V RMS sinusoid therefore produces about 1.02 A RMS, much below the 5 A at resonance.

A credible numerical answer includes both a displayed number and its physical meaning. If a computed voltage is a peak, it cannot be directly used as an RMS rating. If a frequency is a natural resonance, it cannot be presented as a measured closed-loop bandwidth. If a result is an ideal output voltage, it cannot be equated with the real part's dielectric withstand requirement. Use at least three significant digits in the intermediate steps and round the final display to the precision actually supported by input parameters. A second independent check, such as energy conservation, a complementary voltage, or the expected response as one variable approaches zero, should be written beside the arithmetic.

Design-release workflow

A mathematical design is complete only relative to its declared requirements. Produce a decision matrix connecting efficiency, voltage stress, current stress, temperature, dynamics, isolation where applicable, EMC and fault response. Each column has a different pass criterion; a high numerical efficiency cannot compensate for a failed voltage rating or missing fault isolation.

Audit the design under the worst credible input, the largest and smallest loads, startup, shutdown and a sensor fault. State which cases have been derived, which have only been simulated, and which demand independent qualified testing. A student solution can be rigorous while acknowledging that specific manufacturers' datasheets and safety standards have not been checked.

Important failure modes and nonideal boundaries

A load-dependent resonance shift or abnormal operating region can invalidate a fixed frequency guardband. Control saturation and frequency limits need explicitly documented fault paths.

These limitations are not a minor footnote: they are the conditions under which this chapter's conclusion could reverse. Separate the design intent from the semiconductor's transient stress, and the requested controller action from the physical switching state. A controller display can be numerically smooth while its switching node is overshooting; a motor speed command can be well behaved while the DC bus is absorbing excessive regenerative energy. A waveform generated by a hand-written program is only as complete as the modeled parasitics and fault behavior.

Engineering judgment

Draft an operating-state diagram: disabled, startup sweep, regulated operation, limited operation and fault latch. Show how a missing feedback signal leads to a safe state in a simulated controller.

An engineering comparison should use a common reference case and explicitly report one metric that improves and one that could worsen. For example, increasing switching frequency may reduce some storage ripple yet increase switching heat and radiated emissions; adding capacitance may smooth a voltage while raising surge energy and discharge requirements; increasing control bandwidth may improve tracking while reducing delay tolerance. The tradeoff depends on this lesson's topology and assumptions. Where the text omits a datasheet value, test configuration or certification criterion, the correct output is 'not established' rather than an invented margin.

Focused exercise set

Exercise A — reconstruct. Rewrite the governing relation above using named inputs and outputs. Draw or describe the source, load, storage or reference frame that makes it valid. Mark whether the calculated result is a switching-period average, fundamental value, transient peak, energy, current, power, frequency or loss.

Exercise B — parameter sensitivity. Reproduce the numerical case but change the most influential stated input by +10% while keeping all other inputs fixed. Show the substituted equation and the new number. Explain whether the response is expected to be linear, reciprocal, quadratic or nonlinear, and whether the modified point remains inside the same assumed operating regime.

Exercise C — challenge the assumption. Identify one concrete event, such as a load step, missing feedback signal, frequency detuning, angle-estimation error, current sign reversal or temperature change, that makes the basic calculation incomplete. State which extra measurement or model parameter would be necessary to proceed.

Exercise D — compare choices. Evaluate a second solution concept, not simply a different numerical parameter. Compare source-current stress, controllability, complexity and validation burden. Give a reason the choice could change at light load or at a different source voltage.

Exercise E — audit someone else's answer. A classmate reports a precise 'safe and efficient' result after using only the simplified equation in this lesson. Write a six-line technical review identifying one valid quantitative conclusion, one ignored uncertainty, one protection concern, one proposed simulation, one missing empirical test and the exact boundary of the claim.

Answer guidance and grading rubric

For Exercise A, the key is a consistent sign convention and correct categorization of the calculated quantity. In Exercise B the arithmetic must start from the same stated units, and a legitimate answer must note when a changed parameter would require a new operating regime. In Exercise C the missing variable must materially affect the behavior, rather than being a vague appeal to 'more data'. Exercise D earns full credit only when the alternate architecture changes an engineering tradeoff; merely changing a plotted color is not a design option. Exercise E must not describe software results as measurements or claim an external safety approval. Partial credit is appropriate for an otherwise correct derivation with an explicit, honest limitation; no credit for physically inconsistent units or an unstated phase-voltage reference.

Bridge to the unit model

Operating points across resonance: Resonant gain is a function of frequency and loading rather than a single fixed transformer turns ratio. A soft-switching assumption can be true at one operating point and false at another. The most dangerous regions may be startup and light load, not maximum delivered power.

Plot voltage gain or current magnitude on a frequency axis using fixed, documented component values; repeat with at least two load values. Locate the resonant peak, mark the chosen command range, and explain what a linear model cannot tell you about switch-node commutation.

The companion simulation uses deterministic, intentionally simplified equations. Preserve input settings and screenshot or export the computed parameters together with any graph. A successful interactive plot demonstrates software operation and internal mathematical consistency for the declared formulas; it does not prove real component compatibility. Return to the central question of this chapter: what is calculated, what is assumed, and what is still unknown?

Unit 5 project: Resonant tank gain and soft-switching boundary review

Scope: software-only engineering study and analytical notebook. No mains, traction battery, energized utility interface, or uncontrolled rotating machine is authorized. Deliverables: calculation sheet, documented assumptions, parameter sweep, self-check plot, uncertainty register and short technical decision record.

Project brief

Evaluate a series tank with L=10 µH, C=100 nF and R values 1, 2 and 4 Ω over 50–300 kHz. Compute the natural resonance and draw the magnitude of current for a 10 V RMS sinusoidal source. Highlight the idealized maximum for each resistance.

Begin with a clear control volume and state where power enters and exits. Draw the useful storage variables alongside the PWM switching states. Specify both time scales that matter: a switching or sampled control step, and the slower physical response. Fix a baseline and use identical physical units in every table. Give each graph explicit axis units and distinguish the dependent variable from the manipulated independent parameter.

Experiment 1 — reproduce the baseline

Calculate all baseline quantities by hand or a reproducible script using the equations in Lessons 5.1–5.4. Retain three significant figures before rounding. Use a dimensional cross-check and, where possible, an energy-conservation check. If the model has only a steady-state answer, state why it cannot predict transient overshoot or a semiconductor edge event. Record a short comment explaining whether the computed output is peak, RMS, mean or instantaneous.

Experiment 2 — a controlled perturbation

Recompute resonance for L and C independently changing by ±10%. State why a component tolerance that raises resonance may shift the operating range into a high-current region or undermine an intended soft-switching interval.

An informative parameter sweep changes one physical variable at a time and makes the boundary of the model visible. Where the response is proportional to a square, plot both the direct input and its square so a linear relationship in the transformed variable is evident. Where frequency is varied, avoid mixing hertz and radians per second. Add a small error budget that separates rounding, parameter tolerance and explicitly unmodeled physics. Never present the neatness of a plotted line as independent validation of a physical circuit.

Deliverable and evidence standard

Submit a resonance table, quality-factor comparison, annotated simulated frequency sweep, list of unmodeled LLC phenomena, and an explicit criterion distinguishing a simulated zero-voltage event from measured power-stage ZVS.

Include a table with columns: claim; governing equation; assumed parameter; predicted number; sensitivity to a changed parameter; required physical measurement; status. At least three rows must be marked 'analytical estimate', one must be marked 'simulation only', and two must be marked 'unverified without real data'. If a control function is said to protect a system, describe the software state that changes; do not imply that a high-energy circuit is safely disconnected by an untested algorithm.

Critical decision memo

Write 300–500 words comparing the baseline design against one alternative, showing what improves, what becomes more difficult and what would stop a release. Quantify at least one tradeoff. A technically credible answer may decline to rank options when necessary thermal or component properties were not specified. In that case identify the least-cost experiment or authoritative datasheet information that would resolve the ambiguity. Conclude with an operating-region sketch rather than an unsupported single optimum.

Instructor solution and boundary conditions

With the base L and C, fr≈159.15 kHz. At resonance the series current under the assumed sinusoid is V/R, giving 10 A, 5 A and 2.5 A for R=1,2,4 Ω respectively. The resulting current peaks are not a real device current rating recommendation.

An acceptable submission reproduces the numerical baseline independently; makes the units and sign conventions unambiguous; describes what extra physical or sampled-time behavior could invalidate the results; and includes an explicit exclusion of hardware safety certification. An incorrect submission treats a nominal fundamental voltage as total broadband RMS, mistakes a mathematical natural frequency for an empirical stability limit, or declares a component safe without its applicable manufacturer ratings. Project success demonstrates reasoning and traceable calculation, not a built converter.