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Switching Power Supplies

Pick up your phone charger. Look at a laptop power brick. Examine the wall adapter for your Wi-Fi router. Every one of these is a switching power supply — a device that converts electrical energy with dramatically higher efficiency than a traditional linear supply by rapidly switching a transistor on and off rather than dissipating excess voltage as heat. Switching power supplies (also called switch-mode power supplies, or SMPS) now dominate consumer electronics because they are small, light, efficient, and inexpensive to manufacture. Many modern ham transceivers use them internally as well.

For the ham radio operator, switching power supplies are a double-edged sword. Their efficiency advantages are real and valuable. But every SMPS generates broadband radio frequency interference as a direct consequence of its operating principle, and a cheap or poorly designed SMPS near your HF receiver can raise your noise floor by 20 to 40 dB — enough to make weak signals completely inaudible. Understanding how switching supplies work is essential for both using them intelligently and defending your station against their interference.

What you will learn: Why switching is more efficient than linear regulation, how the buck, boost, and flyback converters work, how PWM control maintains regulation, the EMI generated by switching transitions, how to identify and eliminate switching supply noise in your station, and how to choose between linear and switching supplies for ham radio use.

Why Switching Instead of Linear?

A linear voltage regulator wastes energy as heat. The pass transistor sits between the input and output, and it must drop a voltage equal to (Vin − Vout) while passing the full load current. Every watt of power dropped across the transistor becomes heat. If you are regulating from 18 V down to 13.8 V at 10 A, the transistor dissipates (18 − 13.8) × 10 = 42 W. That 42 W must be removed by a heatsink, which requires a large chunk of aluminum, good airflow, and accounts for significant size and weight. The efficiency of this linear supply is only (13.8 × 10) / (18 × 10) = 76.7%.

Now consider a car alternator charging at 13.8 V, supplying 10 A: it delivers 138 W to the load. The linear supply takes 180 W from the transformer, wastes 42 W as heat, and delivers 138 W — efficiency 76.7%. A switching supply achieving 90% efficiency takes only 153 W from the transformer and wastes only 15 W as heat. The heatsink can be much smaller. The transformer can be much smaller. The entire supply is lighter and cheaper to manufacture.

At higher input voltages, the advantage becomes even more dramatic. A 5 V computer supply derived from 120 V AC line voltage through a linear regulator would have an efficiency of roughly 5/170 = 3% — totally impractical. Switching supplies handle this ratio efficiently. This is why switching topologies are used in virtually every AC-to-DC adapter manufactured today.

The Fundamental Principle

The key insight behind all switching power supplies is the behaviour of an inductor when a voltage is applied and then removed. When you connect a voltage across an inductor, current rises linearly. The inductor stores energy in its magnetic field. When you disconnect that voltage, the inductor's magnetic field collapses and it generates a voltage to maintain current flow — the "inductive kick." This energy can be directed into a load instead of being wasted.

The switching supply uses a transistor (usually a MOSFET) to rapidly connect and disconnect the input voltage from the inductor. During the on-time, energy flows from the input into the inductor's magnetic field. During the off-time, the inductor releases its stored energy to the output. The output capacitor smooths the current pulses into a steady DC voltage. The ratio of on-time to the total switching period — the duty cycle D — controls how much energy is transferred per cycle and therefore sets the output voltage.

The higher the switching frequency, the smaller the inductors and capacitors needed to store and smooth the energy pulses. This is why higher switching frequencies allow smaller, lighter power supplies. Modern switching supplies typically operate at frequencies between 20 kHz (just above audio range, to avoid audible whine) and 1 MHz or higher (ultracompact laptop adapters). Higher frequencies mean more switching transitions per second, which means more radio frequency interference generated per unit time.

Block diagram of a switching power supply showing AC input, EMI filter, bridge rectifier, bulk capacitor, PWM switch MOSFET, inductor and transformer, output diode, output capacitor, load, and feedback path from output to PWM controller

SMPS block diagram: the PWM controller adjusts the duty cycle in response to output feedback, maintaining constant output voltage regardless of input variations or load changes. Every switching transition creates RF noise.

View Larger

The Buck (Step-Down) Converter

The buck converter is the simplest and most common switching topology. It always produces an output voltage lower than its input voltage — hence "step down." You will find buck converters in computer motherboard voltage regulators (converting 12 V to 1.2 V for the CPU), in solar charge controllers, in USB charging adapters, and in many battery-operated ham radio accessories.

Circuit Elements and Operation

The buck converter uses four passive components plus the switching transistor: a series switch (MOSFET Q), a freewheeling diode D, an inductor L, and an output filter capacitor C. The load RL connects across the capacitor.

Switch ON phase: When the MOSFET turns on, current flows from Vin through the inductor to the output capacitor and load. The inductor current ramps up linearly because the voltage across it is (Vin − Vout). Energy is stored in the inductor's magnetic field. The freewheeling diode is reverse-biased and carries no current.

Switch OFF phase: When the MOSFET turns off, the inductor cannot allow its current to stop instantaneously. It generates a reverse voltage to maintain current flow, forward-biasing the freewheeling diode. Current now flows from the inductor through the freewheeling diode, continuing to supply the output capacitor and load. The inductor current ramps down as energy is released. This phase ends when the MOSFET turns on again.

The average output voltage is determined by the duty cycle:

Buck Converter Output Voltage:
Vout = D × Vin

Where D = ton / T (on-time divided by total period), ranging from 0 to 1.
Worked Example:
Vin = 20 V, desired Vout = 13.8 V
Required duty cycle: D = Vout / Vin = 13.8 / 20 = 0.69 = 69%
At a switching frequency of 100 kHz: T = 10 µs total period.
On-time: ton = 0.69 × 10 µs = 6.9 µs
Off-time: toff = 3.1 µs
The PWM controller generates this 69% duty cycle waveform to drive the MOSFET gate.

The PWM controller measures the output voltage with a feedback divider and automatically adjusts D to compensate for changes in Vin or load current. If the output tries to drop below 13.8 V, the controller increases D to pass more energy per cycle. If the output tries to rise, D is reduced. This feedback loop is what makes the output regulation precise.

Buck converter schematic showing PWM-controlled switch transistor Q, freewheeling diode D1, inductor L, output capacitor C, and load R, with two states labeled: switch-on showing current building in inductor, and switch-off showing inductor freewheeling through D1. Duty cycle D equals Vout divided by Vin.

Buck converter operation: during switch-on, energy builds in the inductor. During switch-off, the inductor delivers stored energy to the output through the freewheeling diode. Output voltage = duty cycle × input voltage.

View Larger

The Boost (Step-Up) Converter

The boost converter does the opposite of the buck — it produces an output voltage higher than its input voltage. This seems counterintuitive, but it follows directly from the inductor's energy-storage behaviour.

How Boost Conversion Works

Switch ON phase: The MOSFET switch connects the inductor directly from Vin to ground. Current builds in the inductor from the input source. The output diode is reverse-biased, so the output capacitor supplies the load on its own during this phase.

Switch OFF phase: The MOSFET turns off. The inductor now has current flowing through it and nowhere to send it — so it generates a voltage in the same direction as Vin. The total voltage at the top of the inductor becomes Vin + VL, which can greatly exceed Vin. This higher voltage forward-biases the output diode, driving current into the output capacitor and load at the boosted voltage.

Boost Converter Output Voltage:
Vout = Vin / (1 − D)

As D approaches 1 (100% duty cycle, switch always on), Vout approaches infinity — in practice limited by inductor resistance, switch losses, and capacitor ripple.
Worked Example — Boosting 12 V battery to 24 V:
Vin = 12 V, Vout = 24 V
Required duty cycle: D = 1 − (Vin / Vout) = 1 − (12 / 24) = 1 − 0.5 = 0.5 = 50%

Ham radio application: Some older 24 V transceivers or amplifiers need a 24 V supply in a vehicle that only has 12 V available. A boost converter running at 50% duty cycle provides exactly this. Modern MPPT solar charge controllers also use boost converters to efficiently transfer energy from solar panels whose voltage may be below the battery voltage.

The boost converter's output current is lower than its input current (conservation of energy: if voltage doubles and efficiency is 100%, current halves). At 90% efficiency boosting 12 V at 5 A to 24 V: output current ≈ 12 × 5 × 0.90 / 24 ≈ 2.25 A. This must be considered when designing boost converters for loads requiring significant current.

The Flyback Converter (Isolated)

The buck and boost converters share a direct electrical connection between input and output — they are non-isolated. This is fine for battery-to-battery or DC-to-DC applications, but when converting from AC line voltage to low-voltage DC (as in a phone charger or laptop adapter), isolation between the high-voltage AC input and the low-voltage DC output is essential for safety and to meet regulatory requirements.

The flyback converter achieves isolation by using a transformer instead of a simple inductor. The operating principle is similar to a buck-boost converter: during the switch-on phase, energy is stored in the transformer's magnetizing inductance (like an inductor). During the switch-off phase, the stored energy is transferred through the transformer to the secondary winding and thence to the output through a diode and capacitor. The transformer turns ratio sets the relationship between input and output voltages.

Because there is no direct electrical connection between primary and secondary, the output is completely isolated from the AC input. This is the safety isolation that protects you from electrical shock when you touch the output terminals of a power adapter. Regulatory agencies (UL, IEC, CE) require this isolation in any consumer product that derives low-voltage DC from line voltage AC. The flyback converter is the dominant topology in phone chargers, laptop adapters, and all AC-DC wall warts.

A key practical point: in a flyback converter, the voltage across the switch at turn-off is Vin plus a voltage spike caused by the transformer's leakage inductance. This spike can easily reach 400–600 V even in supplies designed for 120 V AC input. The MOSFET switch must be rated for this voltage — typically 600 V for 120 V AC applications and 900 V for universal 85–265 V AC input designs.

PWM Control and Voltage Regulation

All three topologies above require a control circuit that adjusts the duty cycle in response to output voltage changes. This is accomplished by a pulse-width modulation (PWM) controller IC. The operation is straightforward:

  1. A feedback voltage divider samples the output voltage and feeds it to a comparator inside the PWM controller.
  2. The comparator compares the feedback voltage to a precise internal reference (typically 1.25 V or 2.5 V).
  3. If the output is too low, the comparator increases the duty cycle — more on-time, more energy per cycle, output rises.
  4. If the output is too high, the duty cycle decreases — less on-time, output falls.
  5. The system reaches equilibrium when the error is zero — output voltage equals the setpoint.

The response speed of this feedback loop determines the transient response of the supply — how quickly it recovers when the load changes suddenly. A fast loop (high bandwidth) recovers in microseconds. A slow loop may allow the output to droop for milliseconds, which can cause problems for processors or RF circuits that need stable supply voltage during transients.

Common PWM controller ICs include the UC3842, UC3844, SG3525, and TL494, all of which have been in continuous production since the 1980s. Modern compact designs increasingly use single-chip solutions where the controller, MOSFET driver, and sometimes the MOSFET itself are integrated into one package.

Typical switching frequencies range from 20 kHz (the limit of human hearing — below 20 kHz, the inductor can audibly whine) to 1 MHz and beyond. In laptop adapters, frequencies of 65–130 kHz are common. In very compact USB-C chargers, frequencies up to 1 MHz or more allow the inductors to shrink to a few millimeters in height.

Efficiency Advantage: Worked Numbers

The contrast between linear and switching efficiency is most dramatic in high-power, wide input-output voltage difference applications. Here is a direct comparison for a 13.8 V, 10 A supply:

Linear regulator (LM338 + transformer):
Input from transformer: Vin = 18 V DC (after rectification and filtering)
Output: Vout = 13.8 V at Iout = 10 A
Output power: Pout = 13.8 × 10 = 138 W
Power lost in regulator: Ploss = (18 − 13.8) × 10 = 4.2 × 10 = 42 W
Total input power: 138 + 42 = 180 W
Efficiency: 138 / 180 = 76.7%
Heat generated: 42 W — requires a large heatsink and fan in a hot shack

Switching supply (buck converter):
Assumes 90% efficiency.
Input power: Pin = Pout / efficiency = 138 / 0.90 = 153 W
Power lost: 153 − 138 = 15 W
Efficiency: 90%
Heat generated: 15 W — a small heatsink suffices; the whole supply is much lighter

The 15 W difference between linear (42 W loss) and SMPS (15 W loss) is 27 W — permanently. Over an eight-hour operating session: 27 × 8 = 216 Wh = 0.216 kWh saved. Over a year of daily use: roughly 79 kWh saved. At US electricity prices around $0.15/kWh, the SMPS saves about $12 per year in electricity — and produces a much cooler shack.

For portable and battery-powered operation, the efficiency difference is even more critical. Running a transceiver from a 12 V LiFePO4 battery at 20 W receive power: a 90% efficient switching supply gives you 90% of your battery capacity, while a 70% efficient linear supply gives you only 70%. For a 30 Ah battery, that difference is 6 Ah of usable capacity — several extra hours of operation on a SOTA or field day expedition.

EMI and RFI — The Ham Radio Problem

Every switching transition in an SMPS creates a brief but intense electromagnetic disturbance. When the MOSFET switch turns on or off, the current and voltage change at rates of millions of amperes per second. These rapid di/dt and dv/dt transitions generate broadband radio frequency energy that radiates from the wiring and components inside the supply. This energy appears across a wide frequency range — from the fundamental switching frequency all the way up through hundreds of megahertz — because fast square-wave transitions have harmonics extending to very high frequencies.

Two Types of Interference

Conducted interference travels along the power leads connecting the SMPS to your equipment. The RF noise generated inside the supply flows back out through the DC output leads (which act as antennas) and into anything connected to them — your transceiver, your SDR, your preamplifier. It also flows back up the AC input lead and into the electrical wiring of your house, from where it can be picked up by any antenna connected to any sensitive receiver nearby.

Radiated interference is emitted directly from the SMPS as radio waves. The switching waveforms on the internal wiring and PCB traces act as antennas. Every loop of wire carrying pulsing current radiates. The high-frequency harmonics can travel through walls and floors and directly into your receive antenna or feedline.

The Frequency Pattern

The interference from a switching supply appears on a receiver as a series of noise peaks spaced exactly at the switching frequency. A 100 kHz switching supply generates peaks at 100 kHz, 200 kHz, 300 kHz, and so on up through the full HF spectrum and beyond — every 100 kHz across 0–30 MHz is 300 potential interference peaks, many of them in amateur radio bands. The amplitude of the harmonics generally decreases with frequency but the pattern can extend surprisingly high — a 100 kHz SMPS can produce significant interference at 21 MHz (210th harmonic) if it is poorly filtered.

A switching supply at 500 kHz produces harmonics at 500 kHz intervals — 60 peaks across 0–30 MHz. This is generally less visible on an HF receiver than a 100 kHz supply, which is why some SMPS designs deliberately use higher switching frequencies to push the fundamental and low harmonics above the HF spectrum.

Real-world impact: A single inexpensive USB wall charger plugged into an outlet 3 meters from your HF station can raise the noise floor on 40 and 80 meters by 20–40 dB. An S-unit is approximately 6 dB — so a bad charger can add 5–7 S-units of noise, turning an S7 signal into an unreadable S1 or completely burying it. This is not hypothetical: it is one of the most common problems reported on amateur radio forums worldwide.

EMI Filtering and FCC Compliance

Switching supplies intended for sale in the United States must pass FCC Part 15 Class B testing for unintentional radiators. This limits the conducted emissions on the AC input leads and the radiated emissions from the device. The tests use a calibrated receiver and a defined test setup. Passing Class B means the supply is unlikely to cause harmful interference in a normal residential environment — to normal devices like televisions and AM radio receivers.

However, a ham radio HF receiver is far more sensitive than the devices FCC testing is designed to protect. A supply that passes Class B with comfortable margin may still produce interference clearly audible on an HF receiver in the same room. Some supplies that nominally bear FCC marks are counterfeits or do not actually comply — enforcement against imported consumer goods is limited.

Quality SMPS designs include multiple stages of EMI filtering: common-mode chokes on the AC input leads, X-capacitors across the AC input, Y-capacitors from each AC line to the chassis ground, shielded transformers, and additional output filtering. A properly designed and manufactured SMPS can be nearly as quiet as a linear supply — the supply itself is not inherently noisy, but cheap, cut-down designs omit the filtering to reduce cost.

Identifying SMPS Noise in Your Station

If your HF receiver seems noisier than it should be, or you notice a pattern of equally-spaced noise peaks across the band, the systematic approach to identifying the source is straightforward:

  1. Connect the receiver to a dummy load so it is not picking up signals from your antenna. Leave the antenna port disconnected or terminated in 50 Ω. Sweep 1–30 MHz and note the noise pattern you see or hear. Any noise you see now is entering through the power leads or directly radiated into the receiver itself.
  2. Unplug switching supplies one at a time and observe whether the noise drops. Start with anything near the receiver: USB chargers, laptop adapters, LED light drivers (many LED lights use SMPS internally), LCD monitor power bricks, phone chargers, router power adapters. Unplug each one and observe the noise level. You will quickly identify the culprit or culprits.
  3. Reconnect the antenna once you have identified the source, to check whether the interference also comes through the antenna. If it only appears with the antenna connected, the noise is being radiated from the supply and picked up by your antenna. If it appears through both the power lead and the antenna, both conducted and radiated paths are contributing.
  4. Measure the harmonic spacing on the noise peaks. If peaks are 100 kHz apart, the switching frequency is 100 kHz. If 65 kHz apart, 65 kHz. This can help identify the specific supply even before you unplug it.

Once you have identified the source, your options are: replace it with a quieter supply, move it physically farther from your receiver and antenna leads, add ferrite clamp-on cores to its DC output leads to reduce conducted noise, or use a shielded enclosure. Adding a ferrite clamp (Fair-Rite type 31 material, or the split-core snap-on type) with multiple turns of the cable through it is often highly effective and costs only a few dollars.

Choosing Between Linear and SMPS for Ham Radio

There is no single correct answer — the right choice depends on the application, power level, and how much you value efficiency versus noise performance.

Factor Linear Supply Quality SMPS Cheap SMPS
Efficiency 60–80% 85–95% 75–85%
Weight (13.8V, 10A) 3–8 kg (heavy transformer) 0.5–1 kg 0.3–0.7 kg
RFI risk Very low (zero switching) Low (well filtered) High (poor filtering)
Output noise voltage 100–500 µV RMS 1–10 mV RMS 20–100 mV RMS
Cost Higher (large transformer) Moderate Low
Complexity Simple circuit Complex, no repair Complex, no repair
Repairability Easy (simple components) Difficult Difficult and unsafe
Best for HF Yes — quiet Yes — if ham-rated No — avoid

Recommendation for a fixed HF station: A quality linear supply (Astron RS series, which uses a large transformer and simple regulator circuit) or a high-quality ham-specific SMPS (Samlex SEC series, MFJ switching models tested for ham use) is the right choice. The Astron RS-35M is extremely popular among HF operators precisely because it uses a simple linear design that produces essentially no RFI. It is heavy and inefficient but it is completely silent.

Recommendation for portable or mobile operation: A quality ham-specific SMPS makes more sense for field day, SOTA, or mobile use because of weight and efficiency. The Samlex America SEC-1235 and similar products are tested and specified for ham radio use. Avoid generic computer SMPS units or cheap imports from unknown manufacturers.

For laptop, phone, and peripheral power in the shack: Physically separate chargers and adapters from the transceiver and antenna feedlines as much as possible. Add ferrite clamp-on cores to all power leads entering the shack area. Use a separate AC circuit for the transceiver that does not share a circuit with computer equipment if you can.

Frequently Asked Questions

Why does my radio receive more noise when a phone charger is plugged in?

Phone chargers are flyback switching supplies that typically operate between 50 kHz and 300 kHz. Their switching transitions generate harmonics across the entire HF spectrum. The interference travels both through the electrical wiring (conducted) and directly as radio waves (radiated). Even if the charger passes FCC Class B testing, an HF receiver is far more sensitive than the television receivers and AM radios that FCC testing is designed to protect. Moving the charger farther from your radio, adding ferrite clamps to its cable, or replacing it with a higher-quality model (or a battery) often resolves the problem.

Can I repair a switching power supply?

With the right knowledge and safety precautions, yes — but it is significantly more complex and dangerous than repairing a linear supply. The primary side of an AC-to-DC flyback converter operates at line voltage (120 V AC peak around 170 V) and the bulk capacitors may store several hundred volts after the supply is unplugged. Never work inside an SMPS without discharging the capacitors first and measuring to confirm they are discharged. Common failure modes are: shorted MOSFET switch, failed PWM controller IC, failed snubber diode causing MOSFET overvoltage, and open output diode. These are all repairable if you have schematic information, but the work requires a cautious approach, appropriate test equipment, and experience with high-voltage circuits.

What is synchronous rectification?

In a standard buck converter, the freewheeling diode dissipates power equal to Vf × Idiode, where Vf is the diode's forward voltage (0.3–0.6 V for a Schottky diode). At high currents, this loss is significant. Synchronous rectification replaces the freewheeling diode with a second MOSFET that turns on in synchrony with the off-phase of the main switch. A MOSFET's on-resistance voltage drop (I × Rds_on) is lower than a diode forward voltage, so the conduction loss is reduced. Synchronous rectification is used in high-efficiency SMPS designs to achieve efficiencies above 90%, particularly in low-voltage high-current applications like computer CPU regulators.

Are all switching supplies equally noisy?

No — there is enormous variation. A well-designed SMPS from a reputable manufacturer includes multiple EMI filter stages, proper PCB layout with minimized switching current loops, shielded transformer, and Y-capacitors to drain common-mode noise to the chassis. Such a supply can be very quiet at an HF receiver even a meter away. A cheap import may omit most or all of this filtering to save a few cents, and can produce 30 dB more interference than the good design. Products from established ham radio supply manufacturers (Samlex, Cotek, Powerwerx, MFJ) have typically been tested by amateur radio operators and found acceptable. Generic computer supplies, cheap wall warts, and LED light drivers are the most problematic categories.

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