A coil is simply a physical winding of conductive wire. An inductor, however, is a discrete electronic component engineered with a specific core material, air gap, and geometry to store energy in a magnetic field and provide a predictable inductance under load. While the terms coil and inductor are often used interchangeably on the bench, specifying the right inductor for a buck converter, RF filter, or audio crossover requires looking past the copper wire and into the core material, saturation current, and DC resistance (DCR).

Whether you are designing a switch-mode power supply (SMPS) or repairing a blown motherboard, choosing the wrong magnetic component will result in excessive heat, electromagnetic interference (EMI), or catastrophic MOSFET failure. This guide breaks down the physical construction, marking schemes, and failure modes of inductors, giving you the exact criteria needed to select or substitute parts safely.

Inductor Types and Selection Criteria: Which Type for Which Job

Not all inductors are created equal. The core material dictates how the component behaves under high DC bias and high-frequency AC ripple. Below is a comparison of the four most common inductor constructions you will encounter in modern electronics.

Type / Construction Core Material Typical Tolerance Tempco / Stability Typical Use Case
Multilayer Ceramic Ferrite tape layers ±10% to ±20% Moderate / Good high-freq RF filtering, signal lines, GHz decoupling
Unshielded Drum Core Ferrite drum ±20% Moderate / Prone to EMI General purpose DC-DC, low-cost buck converters
Shielded Molded Carbonyl iron / Alloy powder ±10% to ±20% Excellent / Soft saturation High-current SMPS, CPU VRMs, noise-sensitive boards
Toroidal Tape-wound ferrite or iron ±10% to ±15% Excellent / Low stray flux EMI common-mode chokes, audio crossovers, AC line filtering

Selection Rule of Thumb: Use shielded molded inductors (like the Würth WE-LQS or Coilcraft XEL series) for any DC-DC converter operating near sensitive analog circuitry or high-speed digital lines. The magnetic flux is contained within the composite core, preventing inductive coupling into adjacent traces. Use unshielded drum cores only when cost is the primary driver and EMI is not a concern.

Decoding Inductor Markings and Part Codes

Reading the value printed on a physical inductor is a frequent stumbling block because the coding standards differ between SMD and through-hole packages, and they do not always match capacitor coding conventions.

SMD Inductor Codes

Most surface-mount inductors use a three-digit code or an alphanumeric code with an 'R' for the decimal point. The value is almost always in microhenries (µH).

  • Three-Digit Code: The first two digits are the significant figures, and the third digit is the multiplier (number of zeros).
    • 100 = 10 × 10⁰ = 10 µH (Not 100 µH!)
    • 101 = 10 × 10¹ = 100 µH
    • 472 = 47 × 10² = 4700 µH (or 4.7 mH)
  • Alphanumeric Code: The 'R' acts as a decimal point.
    • 4R7 = 4.7 µH
    • R10 = 0.10 µH (100 nH)

Through-Hole Color Bands

Through-hole axial inductors often use a four-band color code similar to resistors, but the resulting value is in microhenries (µH), not ohms. For example, a band sequence of Brown (1), Black (0), Orange (×1,000), and Silver (±10% tolerance) translates to 10,000 µH, which is 10 mH. Always verify with an LCR meter if the bands are faded, as phenolic coatings can yellow over time and skew color perception.

Failure Modes and Visual Diagnostics

Inductors are generally robust, but they operate in high-stress environments—especially in switch-mode power supplies where they endure high di/dt (current slew rates) and thermal cycling. Here is how they fail and what to look for on the bench.

⚠️ WARNING: Core Saturation and MOSFET Death
Core saturation is not a permanent failure of the inductor itself, but a functional failure mode. If the peak current exceeds the inductor's saturation current ($I_{sat}$), the core loses its magnetic permeability. The inductance drops to near-zero, effectively turning the inductor into a short piece of wire. In a buck converter, this causes the switching MOSFET to pull massive, uncontrolled current from the source, leading to catastrophic thermal runaway and an exploded FET. Always check the MOSFET if an inductor looks physically fine but the power rail is dead.
  • Inter-Turn Short Circuit:
    • Cause: Insulation breakdown between copper windings due to voltage spikes or excessive heat.
    • Visual Symptoms: Discolored or melted epoxy coating, bulging casing, or a distinct smell of burnt phenolic resin. The part may measure a lower-than-expected DCR (DC Resistance) on a multimeter.
  • Open Circuit (Wire Break):
    • Cause: Mechanical shock, thermal fatigue at the solder joint, or a transient current spike that literally fuses the internal wire.
    • Visual Symptoms: Often invisible externally. On SMD parts, you may see a cracked solder fillet or pad lift. An LCR meter or multimeter will read infinite resistance (OL).
  • Core Fracture:
    • Cause: Physical impact or severe thermal shock cracking the ferrite material.
    • Visual Symptoms: Visible hairline cracks in the ferrite drum or shield. This alters the magnetic air gap, causing the inductance value to drop unpredictably and increasing EMI radiation.

Safe Substitution Rules When the Exact Part is Missing

When you are repairing a board and don't have the exact OEM inductor in your bins, you can substitute a different part—but only if you respect the electrical and magnetic boundaries. According to Coilcraft's inductor selection guidelines, swapping parts blindly is the leading cause of post-repair thermal failures.

  1. Match or Exceed Saturation Current ($I_{sat}$): This is non-negotiable. $I_{sat}$ is the current at which the inductance drops by a specified percentage (usually 20% or 30%). Your replacement must have an $I_{sat}$ rating higher than the peak switching current of the circuit. If the original was 3.2A, use a 3.5A or 4.0A part.
  2. Match or Exceed RMS Current ($I_{rms}$): $I_{rms}$ dictates the thermal limit of the copper wire. If your replacement has a lower $I_{rms}$ rating, it will overheat and fail open over time.
  3. Keep DCR Equal or Lower: DC Resistance causes $I²R$ heating. A replacement with higher DCR will run hotter and drop more voltage, potentially causing the regulator to fall out of regulation.
  4. Check the Self-Resonant Frequency (SRF): Every inductor has parasitic capacitance, creating a resonant frequency. For a DC-DC converter switching at 500 kHz, the inductor's SRF must be significantly higher (e.g., >10 MHz) so it behaves inductively at the switching frequency.
  5. Shielding Compatibility: You can almost always substitute a shielded inductor for an unshielded one. However, substituting an unshielded part into a design that originally used a shielded part may cause EMI failures or interfere with nearby Hall-effect sensors and RF antennas.

Frequently Asked Questions

Can I use a coil and inductor interchangeably in a DC power supply?

In casual conversation, yes. In engineering practice, no. A raw "coil" (like a hand-wound solenoid or a simple air-core winding) lacks the engineered core material and air gaps required to handle the high DC bias currents in a power supply without saturating. A power supply requires a discrete inductor—specifically one with a gapped ferrite or powdered iron core designed to maintain its inductance under heavy DC load. Using a simple coil in a buck converter will result in immediate core saturation and a blown switching transistor.

Why does my replacement inductor get hot while the original stayed cool?

This is almost always caused by a mismatch in either DC Resistance (DCR) or core loss characteristics. If your replacement has a higher DCR, it will dissipate more heat via copper losses ($I²R$). Alternatively, if the replacement uses a different core material (e.g., swapping a powdered iron core for a standard ferrite core in a high-ripple-current circuit), the core losses (hysteresis and eddy currents) will generate significant internal heat. Always check the datasheet for both DCR and core loss curves when substituting parts.

How do I measure the inductance of an unmarked toroidal coil?

You cannot accurately measure inductance with a standard multimeter; you need an LCR meter. Set the LCR meter to measure inductance (L) in series equivalent circuit mode (Ls) at a test frequency appropriate for the application (usually 1 kHz or 100 kHz for power inductors). Pass the test leads through the center of the toroid and connect them to the wire ends. If the coil is still in-circuit, you must desolder at least one leg first, as parallel PCB traces and capacitors will skew the reading.

What causes audible coil whine, and how do I fix it?

Coil whine is caused by magnetostriction—the physical expansion and contraction of the magnetic core material as the magnetic field changes at an audible frequency (usually between 1 kHz and 20 kHz). In a DC-DC converter, this often happens during burst-mode or pulse-skipping light-load operation when the switching frequency drops into the audible range. To fix it, you can try applying a dab of non-conductive epoxy or RTV silicone to the windings to dampen the physical vibration, or reprogram the controller (if possible) to operate in forced continuous conduction mode (CCM) to keep the switching frequency above 20 kHz.