Ampère's Law in Toroids
The Basics of Ampère's Law
Ampère's Law states that the line integral of the magnetic field B around a closed path is proportional to the total current enclosed:
Ampère's Law: ∮ B · dl = μ₀I
In a toroid, the magnetic flux is largely confined to the core. Current through a winding generates a circular magnetic field, and the field strength scales with the number of ampere-turns (current × turns).
Toroids: Magnetic Loops
Toroids are excellent at confining flux, which makes them ideal for:
- Inductors
- Return current suppressors (chokes)
- Current transformers
- Voltage transformers
But only if they are wound correctly.
The Most Common Mistake: Magnetic Cancellation
If windings enclose equal and opposite ampere-turns, flux cancels and the choke fails:
I = 0 ⇒ ∮ B · dl = 0 ⇒ no net flux
Result: no inductance, no suppression.
Cancellation in Wire vs. Coax
This happens when bifilar or separate wires are mirrored on opposite sides of a core, or when coax winding direction is reversed mid-core. The opposing turns cancel magnetic flux instead of adding.
Even coaxial cable isn’t immune: shield currents couple to ferrite imperfectly, especially since braided shields leak magnetic flux. Double-shielded coax with foil is even worse: the foil blocks magnetic coupling, reducing choke effectiveness. For serious HF chokes, single-braid coax with good coverage is usually better.
Design Rule
- Wind all turns in the same physical direction.
- Do not reverse direction when routing back across the core.
- Visual symmetry ≠ magnetic symmetry. Flux cares only about net ampere-turns.
Preferred Layout: Loop-Back or Crossover
- Wind 4–5 turns on one side of the toroid.
- Route the cable back across.
- Continue winding in the same direction.
This ensures constructive flux buildup and high choking impedance.
Symmetry Can Mislead
Mirrored bifilar chokes look neat but create two current paths with unequal coupling. The result: unpredictable division, poor suppression, and higher RFI risk.
- Skin effect sensitivity: mirrored wires couple differently to their environment.
- Multipath ambiguity: RF divides unpredictably across the two paths.
- Current displacement: symmetry on paper ≠ symmetry in practice.
Mirrored chokes often suck common-mode energy back in, creating imbalance rather than preventing it.
Return Current Suppressors vs. Baluns
What many hams call a “balun” is often just a return current suppressor. Its purpose: block unwanted shield currents and force proper current return per Kirchhoff’s Law. By contrast, a true voltage balun (Ruthroff) transforms impedance but does not suppress imbalance.
Guanella current baluns work by inserting high impedance into the unwanted current path. Their performance depends critically on winding layout and core choice.
Correct Winding Philosophy
A choke is not a transformer — its job is to insert high series impedance to stray currents. Key points:
- Ferrite impedance is complex: Z = R + jX. For suppression, we want the R component to dominate.
- Too many turns add capacitance → self-resonance → choke fails at higher HF.
- Optimize turns for the target band and material (#31 for LF/HF, #43 for HF/low-VHF).
Summary
Ampère’s Law reminds us: magnetic flux in a toroid depends on net current. Good choke design means:
- Every turn adds flux in the same direction.
- Avoid mirrored or reversed layouts.
- Choose cores and turns to maximize resistive loss (R) where you need suppression.
Wind for flux, not for looks. A neat mirrored choke may actually be a dummy load for your ferrite.
Mini-FAQ
- Why do mirrored bifilar windings fail? — They split return currents into two unequal paths, causing cancellation or imbalance.
- Does coax shield foil hurt choke performance? — Yes. Foil shields block magnetic coupling, reducing ferrite effectiveness.
- What’s the goal of a choke? — Not power transfer. It’s to present high series impedance to stray or return currents.
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