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GAPPED TOROIDAL CORES


The design of a storage choke or transformer which also carries direct current normally requires air gaps which prevent the core from being magnetized by the dc current above 1/2 B max.

An air gap in a core has the effect of flattening/ shearing the B-H loop of the material, lowering the residual flux and the permeability, extending the incremental a.c. permeability to higher values of B and H. Precise control of the inductance L, or the remanence Br is therefore possible with gapped toroids.

Figure 4 shows a comparison of hysteresis loops for a core with and without gaps.


Hysteresis loops with and without gaps


For larger air gaps, the B field fringes over a larger area. The actual μg or Lg is then significantly greater than calculated. The deviation increases with lg, with 1/Ac and the more Ac deviates from a square area.

When an unbalanced dc current flows in a winding, the core is subjected to a dc magnetizing force. This results in a flux density which may be expressed as

Bdc = .4π x N Idc / Ig + Im/μm

Ig and Im in cm.

If the sum of Bac and Bdc are over the maximum operating flux density of the core material, the incremental permeability and inductance are greatly reduced; to reduce Bdc the Ig increases the inductance will decrease, therefore, the designer should balance Ig to produce maximum inductance. See Hanna curvers.