The basic structure of an inductor is simple: winding an enameled wire around a magnetic core forms an inductor. However, in practical applications, there are multiple choices:
Core materials: Ferrite, powdered iron, etc.
Core shapes: Toroidal, E-shaped, and other specialized geometries
Winding types: Single-strand wire, multi-strand twisted wire (rope-type), or Litz wire
Engineers must select the most suitable inductor type based on the specific application scenario.
Material Selection:
Nanocrystalline materials are often used in common-mode chokes (CMC) due to their broadband frequency characteristics.
However, in motor drives or high-power switch-mode power supplies (SMPS), electromagnetic interference (EMI) typically starts in the kHz range, making manganese-zinc (MnZn) cores more suitable.
Inductance Calculation:
Theoretical formula:

Where:
n: Number of turns
A: Cross-sectional area of the core
k: Coil geometric coefficient
\mu_0: Permeability of free space
Design Trade-offs:
Increasing the number of turns enhances inductance (proportional to the square of turns), but inter-turn capacitance also rises, leading to:
A downward shift in resonant frequency
Dominance of capacitive effects (especially above 20 MHz)
This is a key reason why inductors may perform poorly in certain designs.
A DC-DC converter employed a two-stage CMC filter (targeting 20–30 MHz noise suppression). Despite the CMC datasheet showing good attenuation in this range, actual testing revealed:
After removing the CMC: Noise in the 20–30 MHz range decreased by ≥6 dB (capacitive effects dominated).
Low-frequency range (150 kHz–1 MHz): Noise worsened (due to leakage inductance).
Solution: Switching to a ferrite core and reducing the number of turns.

Illustration:
The figure shows two common-mode chokes (REO model CHII31) in the DC-DC converter's two-stage filter.
Structure: Nanocrystalline core + rope-type winding
Failure Analysis:
High-frequency failure: Winding capacitance caused inefficiency above 20 MHz.
Low-frequency dependency: Leakage inductance still provided suppression at 150 kHz–1 MHz.
Shielding effect: Using copper tape to shield the inductor reduced conducted emission noise by 10 dB.

Curve comparison: Purple (bare PCB) vs. green (shielded inductor).

Primary principle: Minimize magnetic flux coupling.
Magnetic field strength decays as 1/r (where r is distance).
Common coupling mechanisms (see Fig. 11):
Between conductors
Between inductor and conductors
Cross-coupling between inductors/transformers
PCB Design:
Prefer shielded inductors.
Place filter inductors on the PCB's "quiet side."
In large systems (e.g., industrial motor drives): Keep inductors far from other cables.
Magnetic flux leakage between conductors → Magnetic coupling
Coupling between inductor and conductors
Cross-coupling between inductors/transformers
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