By integral form of modified Maxwell's equations, we have:
∮∂SB⋅dℓ=μ0∫S(J+ϵ0∂E∂t)⋅dS
Where the displacement current density is given by:
JD=ϵ0∂E∂t
The above integral states that, the line integral of magnetic field around any loop is equal to μ0 times the surface integral of the total current density.