This information is part of the Modelica Standard Library maintained by the Modelica Association.

Educational example of a magnetic circuit containing an iron core and an airgap:

A current ramp is applied in positive electric direction through the exciting coil, causing a rising magnetomotive force (mmf) in positive magnetic direction of the electromagnetic converter. The mmf in turn causes a magnetic flux through the circuit in the direction indicated by the flux sensor. From that magnetic flux, flux density can be calculated in every element of the magnetic circuit. Flux density is used to derive magnetic field strength. Magnetic field strength times length of the flux line gives magnetic potential difference of each element. The sum of all magnetic potential differences is covered by the mmf of the exciting coil.

Using the parameter values, the results can be validated by analytic calculations:

element	cross section	length	rel. permeability	B	H	mmf
left leg	a*a	l - a	μr	flux / cross section	B/(μr*μ0)	H*length
upper yoke	a*a	l - a	μr	flux / cross section	B/(μr*μ0)	H*length
right leg	a*a	l - a - delta	μr	flux / cross section	B/(μr*μ0)	H*length
airgap	a*a	delta	1	useful flux / cross section	B/μ0	H*length
lower yoke	a*a	l - a	μr	flux / cross section	B/(μr*μ0)	H*length
total						Σ mmf = N*I

Note that there is a leakage flux path present. Therefore the total magnetic flux of in core splits into

• the useful flux through the airgap and
• the leakage flux through the leakage element.

However, the magnetic voltage across the airgap and the leakage model are equal. The ratio of the useful flux over the flux in the core is equal to 1 - σ. In the core the magnetic flux is the same in every element as they are connected in series. For the calculation of the length of flux lines inside the core, a medium flux line (dashed line) is used

Additionally, a measuring coil is placed in the airgap. Due to Faraday's law, the time derivative of flux causes an induced voltage both in the exciting coil (in positive direction) and in the measuring coil (in negative direction). Since the quasi static current and therefore flux follow a time dependent ramp, the quasi static induced voltages follow a ramp as well.

Note the proper usage of electric and magnetic grounds to define zero potential.

l	Value: 0.1 Type: Length (m) Description: Outer length of iron core
a	Value: 0.01 Type: Length (m) Description: Side length of square cross section
mu_r	Value: 1000 Type: Real Description: Relative permeability of core
delta	Value: 0.001 Type: Length (m) Description: Length of airgap
sigma	Value: 0.1 Type: Real Description: Leakage coefficient
N	Value: 500 Type: Integer Description: Number of turns of exciting coil
I	Value: 1.5 Type: Current (A) Description: Maximum exciting current