Continuous Conduction Mode in an SMPS: What is it and Why it Matters

Zachariah Peterson
|  Created: May 6, 2021
Continuous conduction mode

Switched-mode power supplies seem simple enough to design and analyze: it seems like you plug in wall power, and you get out a stable DC voltage, right? I think it would be great if power supply design was that simple, but that is not really the case. Things like topology, component selection, layout decisions, isolation, and grounding all influence noise, stability, and transients in the supply’s output response. One factor that isn’t always considered in switching power supplies is the conduction mode, or how the energy storage section and components release energy to deliver power to the output terminals.

The continuous conduction mode is often desired by default when designing power supplies, but there is also a discontinuous conduction mode that can be accessed in switching power supplies. To summarize what this means, the energy stored in a coil in a power supply will drop to zero in the discontinuous conduction mode, and it never drops to zero in the continuous conduction mode. As far as power delivery and what you would measure, the current in the coil will cross 0 A due to switching in the discontinuous mode, while it will not cross 0 A in the continuous mode.

Why is this important, and which mode should we try to reach in a power supply? We’d prefer the continuous mode, but it’s important to understand why we might end up in the discontinuous mode and what tradeoffs are involved. Let’s look at some reasons to reach for the continuous conduction mode in your regulator design and how you can tell if you’ve reached the discontinuous mode.

Why the Continuous Conduction Mode is Important

As was mentioned above, the continuous conduction mode in a power supply is reached when the current in the charging/discharging coil never drops to or crosses over 0 A. If you look at the waveform for the inductor current in a switching converter, you can quite easily see whether the system is operating in the continuous or discontinuous mode. As long as the current in the inductor is always pointing in the same direction as the input current, then you’re operating in the continuous conduction mode.

The graph below shows an example of what can happen in the discontinuous mode. Here, I’ve simulated a simple buck topology with 50% duty cycle @100 kHz and a small inductor (only 500 nH) connected to a very small (10 Ohm) load. Here, we see that the inductor current briefly drops to -40 mA while the switch is on due to undershoot in the transient waveform. When the switch is off, we see that the OFF-state circuit is an underdamped RLC oscillator, where the inductor current oscillates around 0 A before the next PWM cycle. Note the peak in the transient response reaches approximately -200 mA during this oscillation with significant ringing, making this a rather undesired inductor current.

Discontinuous conduction mode waveform
Inductor current in a voltage regulator operating in discontinuous conduction mode. Note the strong ringing here.

In light of the above graph, it’s a fair question to ask: why do we care about the continuous conduction mode? There are several reasons:

  1. In discontinuous conduction mode, the output voltage depends on the duty cycle, inductor size, PWM frequency, and the input voltage value. In continuous conduction mode, the output voltage only depends on the PWM duty cycle.
  2. This means that simply adjusting the duty cycle to compensate for changes in the input voltage is no longer a useful control strategy when in the discontinuous mode.
  3. As we see above, in the discontinuous conduction mode, there is a potentially undesired transient response in the inductor current that can propagate to the output voltage.
  4. The transient response in the inductor current can be underdamped with some ringing during PWM switching, leading to EMI emission at high currents.

In point 1 above, I’ve ignored any of the nonlinear effects in the switching MOSFET, but these points are valid regardless. If you’re designing a power converter to operate at one specific PWM frequency and duty cycle, and there is no feedback sensing or PWM adjustment, then you’re probably not worried about the continuous conduction mode. As long as you get the power you want and EMI isn’t too terrible, then don’t worry about it. Real systems that require precise control over the regulator output and low EMI should opt for continuous conduction mode designs as there is only one lever needed to compensate for changes in the output voltage.

Designing for the Continuous Conduction Mode

If the load in the system is too low, your SMPS will enter the discontinuous conduction mode. The process for designing to the continuous conduction mode follows a specific process: select the desired output voltage, calculate the coil inductance and output capacitor values, and select the PWM driver parameters. These tasks can be performed for a target load resistance value.

What Happens in Discontinuous Mode

When you’re operating in the discontinuous conduction mode, the output voltage will depend on the inductor value, PWM frequency, and duty cycle. For simple topologies with a single PWM source and MOSFET, the output voltage is given by the following equations:

Discontinuous conduction mode output voltage
Buck and boost output voltage values in the discontinuous conduction mode.

The above equations are well-known. I don’t often reference Wikipedia, but their articles on buck and boost converters contain the derivations of these equations. Follow their steps if you want to derive expressions for more complex converter topologies and determine the output voltage, inductor current, and the border between discontinuous and continuous conduction.

Pick the Right Inductor for Continuous Conduction Mode

There are a couple other points to notice both from the above equations and from the basic function of an inductor in a DC-DC converter:

  • The inductor should generally be large to dampen the ripple current. As it turns out, there is also a minimum inductor value that will ensure continuous conduction mode operation. From the above, we see that the correct in discontinuous mode vanishes as L → infinity.
  • The output capacitor should also be large, both to suppress ripple and to ensure slow discharge when the inductor is releasing energy. There is a minimum output capacitance value for a given ripple current and load that will ensure the design operations in the continuous conduction mode.

While the equations for minimum capacitance and inductance are found in many application notes for basic buck/boost designs, more complex topologies can be difficult to analyze, and SPICE simulations can be used to determine the minimum load resistance that will ensure your converter operates in the continuous conduction mode.

What to Evaluate in Your Design

Obviously, the inductor current should be evaluated in a SPICE simulation when checking for continuous conduction mode operation. The design strategy for ensuring the inductor current does not fall to zero during switching is to iterate through values for other circuit elements, namely the output capacitance and load resistance values. Run through different load and capacitor values to find a region where the inductor current remains positive for your chosen PWM parameters.

Continuous conduction mode circuit design
Simple buck converter topology. The output circuit values should be adjusted to prevent discontinuous operation.

Nonlinear effects in the MOSFET will also influence the rise/fall time of the inductor current, so the PWM driving voltage and the range of input values might also be design candidates for avoiding discontinuous operation. Make sure you have a valid simulation model for your MOSFETs and make use of DC sweeps to spot the linear range for your converter when selecting PWM parameters.

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About Author

About Author

Zachariah Peterson has an extensive technical background in academia and industry. He currently provides research, design, and marketing services to companies in the electronics industry. Prior to working in the PCB industry, he taught at Portland State University and conducted research on random laser theory, materials, and stability. His background in scientific research spans topics in nanoparticle lasers, electronic and optoelectronic semiconductor devices, environmental sensors, and stochastics. His work has been published in over a dozen peer-reviewed journals and conference proceedings, and he has written 1000+ technical blogs on PCB design for a number of companies. He is a member of IEEE Photonics Society, IEEE Electronics Packaging Society, American Physical Society, and Printed Circuit Engineering Association (PCEA), and he currently serves on the INCITS Quantum Computing Technical Advisory Committee.

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