The DCM flyback as a loss-free resistor
Intent
Section titled “Intent”- Size a fixed-duty-ratio DCM flyback so that it presents a source’s resistance.
- Find the source amplitude above which it leaves DCM, and know what it does then.
- Know what voltage its switch blocks, and why more power through the same resistance needs more of it.
Theory
Section titled “Theory”Sizing the loss-free resistor
Section titled “Sizing the loss-free resistor”A flyback in DCM with a fixed duty ratio presents the loss-free resistor at its input [Erickson & Maksimović 2020, Ch. 15 (AC and DC Equivalent Circuit Modeling of the Discontinuous Conduction Mode)]. Solved for the magnetizing inductance, that resistance gives the inductance a design needs:
- magnetizing inductance (primary)
- duty ratio
- emulated input resistance
- switching frequency
Assumptions, convention and source
- Assumptions
- ideal (lossless) switches and passive components
- discontinuous conduction mode (DCM)
- periodic steady state
- Notes
- the loss-free resistor solved for ; to match a linear source,
- Source
- Erickson & Maksimović 2020, Ch. 15 (AC and DC Equivalent Circuit Modeling of the Discontinuous Conduction Mode); derived here; Singer 1990
- Derivation
- step-by-step sympy derivation
- Equation id
lfr.L_M· equations.yaml entry
To match a linear source, the input resistance is set to the source resistance (extraction by a loss-free resistor). A lower switching frequency, or a larger duty ratio, needs a larger inductance for the same resistance. The output voltage does not enter: in DCM the input resistance depends only on the inductance, the switching frequency and the duty ratio.
Where DCM ends
Section titled “Where DCM ends”The flyback stays in DCM while its input voltage is below the critical input voltage, which the output voltage, the diode’s drop, the duty ratio and the turns ratio set. A source strong enough to raise the divider voltage (bus voltage of a loss-free resistor) above it drives the flyback into CCM. With the output fixed, the CCM conversion ratio then allows only one input voltage, the critical one [Erickson & Maksimović 2020, Ch. 6 (Converter Circuits)]: the bus is held there, and the flyback becomes a constant-voltage sink, whose share of the available power depends on the source’s amplitude (constant-voltage extraction).
What the switch blocks, and more power
Section titled “What the switch blocks, and more power”The switch blocks the input voltage plus the output voltage reflected through the turns ratio (switch voltage), and the leakage inductance’s spike adds on top (snubbers and clamps). Through the same input resistance, a larger power needs a higher input voltage:
- input voltage
- power
- emulated input resistance
Assumptions, convention and source
- Assumptions
- ideal (lossless) switches and passive components
- discontinuous conduction mode (DCM)
- periodic steady state
- Notes
- more power through the same input resistance needs a higher input voltage, which the switch must also block
- Source
- Erickson & Maksimović 2020, Ch. 15 (AC and DC Equivalent Circuit Modeling of the Discontinuous Conduction Mode); derived here; Singer 1990
- Derivation
- step-by-step sympy derivation
- Equation id
lfr.Vg_power· equations.yaml entry
so drawing more power through a matched flyback raises its switch’s voltage. That holds up to the critical voltage. There CCM holds the bus, and while the flyback switches, the switch voltage stays at its CCM value whatever power the source then pushes in; the largest power the flyback draws as a resistor is the power a DCM converter draws at the critical voltage.
Worked example
Section titled “Worked example”A flyback sized to present the source’s resistance:
| Symbol | Value | How it is obtained |
|---|---|---|
| source open-circuit voltage | 150 V | given |
| source resistance | 10 kΩ | given |
| duty ratio | 0.2 | given |
| switching frequency | 10 kHz | given |
| output voltage | 5 V | given |
| output-diode forward drop | 500 mV | given |
| turns ratio, secondary/primary | 0.1 | given |
| magnetizing inductance (primary) | 20 mH | Magnetizing inductance of a DCM flyback that presents a given input resistance |
| emulated input resistance | 10 kΩ | Input resistance of a DCM buck-boost or flyback (loss-free resistor) |
| input voltage | 75 V | Bus voltage of a loss-free resistor fed by a linear source |
| share of the available power extracted | 1 | Extraction fraction of a loss-free resistor |
| largest power available | 563 mW | Maximum power from a linear source |
| input voltage at the CCM/DCM boundary | 220 V | Flyback: input voltage at the CCM/DCM boundary (fixed D, fixed output) |
| switch voltage while off | 130 V | Flyback switch voltage while off (without the leakage spike) |
Operating mode: DCM: the flyback is a loss-free resistor (: holds)
At 0.2 and 10 kHz, a magnetizing inductance of 20 mH presents 10 kΩ, the source’s resistance. The source’s 150 V then divides to 75 V, below the critical input voltage of 220 V: the flyback takes the whole available 563 mW, and its switch blocks 130 V before the leakage spike.
Try it
Section titled “Try it”▶ Open in the equation explorer: Magnetizing inductance of a DCM flyback that presents a given input resistance
Preset from the example lfr-flyback
Sweep the duty ratio: the inductance that presents the same resistance grows as its square.
▶ Open in the simulator: Flyback
Preset from the example flyback-source
A stronger source into the same kind of flyback: the bus rises until CCM begins and settles at the critical input voltage.
Bench exercise
Section titled “Bench exercise”Build the flyback with its duty ratio fixed and a bus capacitor across its input, large enough that with the series resistor it averages the pulsed input current over many switching periods, and feed it from a bench supply through a series resistor equal to its computed input resistance. Measure the input voltage: it should sit at half the supply’s voltage. Raise the supply slowly until the input voltage stops following it; that is the critical input voltage, to compare with the formula. The supply must reach twice that voltage, several hundred volts with the example’s numbers, and the bus capacitor holds what it reaches: keep the circuit enclosed, and discharge the capacitor through a resistor before touching it. A larger turns ratio n (N_s/N_p) lowers the critical voltage (critical input voltage) and keeps the exercise at a safer voltage. At each step, capture the switch’s drain voltage with a probe rated for it (probes), and read the plateau before the leakage spike against the formula.
Gotchas
Section titled “Gotchas”- Above the critical input voltage the flyback no longer matches. CCM holds the bus there (critical input voltage).
- The switch voltage includes the reflected output, and the leakage spike adds to it (switch voltage).
- While the flyback does not switch, the bus charges to the open-circuit voltage: at start-up, in an undervoltage lockout or after a fault, nothing draws on the source. The switch then blocks that voltage plus the reflected output: rate it for that, or clamp the bus (the design case).
- More power through the same resistance needs a higher voltage (input voltage for a given power).
- The match is forgiving. The share is flat at its top: a small error in the inductance moves the input resistance by the same fraction, and the share falls by only about a quarter of that fraction squared (extraction by a loss-free resistor).
Go deeper
Section titled “Go deeper”- Book chapter AC and DC Equivalent Circuit Modeling of the Discontinuous Conduction Mode (Ch. 15)
The DCM averaged switch model, in which the input behaves as a loss-free resistor. - Book chapter The Discontinuous Conduction Mode (Ch. 5)
Origin of DCM, the K and K_crit boundary and the DCM conversion ratios derived with charge balance. - Paper Optimized piezoelectric energy harvesting circuit using step-down converter in discontinuous conduction mode
A step-down converter in DCM between a piezoelectric element and a battery, run at the duty ratio that harvests the most.
A flyback at 5 kHz and a duty ratio of 0.1 must present 20 kohm, the source resistance, in DCM. What magnetizing inductance does it need?
Answer and explanation
Correct answer: A The input resistance times the duty ratio squared over twice the switching frequency: 2e4 times 0.01 over 1e4, which is 0.02 H.
The duty ratio is doubled to 0.2 with the same switching frequency and resistance. What inductance is needed now?
Answer and explanation
Correct answer: C The inductance grows as the square of the duty ratio: four times 20 mH.
Where does a DCM flyback matched to a linear source hold its input voltage?
Answer and explanation
Correct answer: D Its input resistance equals the source resistance, so the two divide the source voltage in half.
The source grows until the divider voltage would exceed the critical input voltage. What does the flyback do?
Answer and explanation
Correct answer: A With the output fixed, the CCM conversion ratio allows only the critical input voltage: the bus is held there, and the flyback becomes a constant-voltage sink.
A flyback with a 5 V output, a 0.5 V diode, a duty ratio of 0.2 and a turns ratio of 0.1 sits at 75 V. What is its critical input voltage, and is it in DCM?
Answer and explanation
Correct answer: B 5.5 V times 0.8 over (0.1 times 0.2), which is 220 V; the input is below it, so the flyback is in DCM.
What voltage does its switch block, before the leakage spike?
Answer and explanation
Correct answer: C The input voltage plus the output and diode voltage reflected through the turns ratio: 75 V plus 5.5 V over 0.1.
The magnetizing inductance comes out 10 % low. About how much of the available power does the flyback lose?
Answer and explanation
Correct answer: D The input resistance is 10 % low too, and at the top of the share a fraction off costs about a quarter of its square: 4 times 0.9 over 1.9 squared is 0.997.
The numbers in the examples, presets and exercises on this site are synthetic: round teaching values, not data from any real design.