The total current density in magnetized material is the sum of the free and bound current densities. The free current arises due to the motion of free electrons within the material, while the bound current arises due to the alignment of magnetic dipole moments.

The differential form of Ampere's law in vacuum states that the curl of the magnetic field equals the permeability times the current density. In a magnetized material, the law is modified to incorporate the free and bound current densities.

The equation is modified when the bound current density is expressed as the curl of the magnetization vector. The terms involving the curl of the parameters are rearranged as

The terms in the bracket can be expressed as magnetic field intensity, . It is the magnetic field vector upon permeability minus the magnetization vector.

Thus, Ampere's law in matter states that the curl of the equals the free current density.

The equation can be written in integral form as

The line integral of along a closed Amperian loop equals the net free current passing through the loop.

The magnetic field intensity helps express Ampere's law in matter in terms of the free current. Similarly, the electric displacement vector helps in representing Gauss's law in matter in terms of the free charge. Thus, the magnetic field intensity vector in magnetostatics is analogous to the electric displacement vector in electrostatics.

Since an electromagnet is formed when current is passed through a coil, the free current is the known parameter. On the other hand, the B field is a material characteristic. Hence, the H field is often used in experiments rather than the B field.