In the two different medium of permeability μ1 and μ2, the magnetic fields are (B1, H1) and (B2, H2) respectively as shown in the figure:

If the interface carrier no current, then the current relation(s) for the angle θ1 and θ2 is/are:

1
B1 cos θ1 = B2 cos θ2
2
H1 cos θ1 = H2 cos θ2
3
B1 sin θ1 = B2 sin θ2
4
H1 sin θ1 = H2 sin θ2

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