The article describes the application of brand new field type through New Axioms and Laws. The present study uses Expanded Field Theory. It changes the Classic Field Theory to a much more general theory that consists of 2 new axioms and 8 laws. It was described from previous works of the same author. In this report is used only 1 axioms and 6 laws only. It is known that Maxwell’s laws (1864) are based on a single axiom [1]. It states that the movement in a closed loop leads to evenly movement (with constant speed) of a vector E: div rot E = 0. The author change this axiom with a new one, according which the movement in an open loop or vortex leads to unevenly movement (with variable speed) of a vector E:div rot E ≠ 0, div V or E ≠ 0 for vortex [2]. The subsequent results are: the evenly movement is replaced with unevenly movement which can be decelerating or accelerating; in 2D it exists a cross vortex and in 3D it exists a longitudinal vortex; the cross vortex in 2D is transformed to a longitudinal vortex in 3D through a transformation Δ1; the longitudinal vortexin 3D is transformed to a cross vortex in 2D through special transformation Δ2; decelerating vortex emits free cross vortices to the environment that are called “free energy”; accelerating vortex sucks the same ones free cross vortices and so on. The vector E is not a simple. It turns to be a complex vector: E=A+iV, E=V+ iA or E=-A-iV, E= -V- iA. It can has or amplitude A in a real part, or velocity V as a real part. Cross vortices can form two kinds vortices: a vortex that is generated by amplitude A and the vortex that is generated by velocity V. Each of these may be accelerating or decelerating. Both of them are generators. They are prototypes of material particles. Due to the suction of cross vortices by the accelerating vortex the temperature decreases and due to the emitting of cross vortices by the decelerating field the temperature increases. Inside of the conductor the velocity of Electromagnetic field is constant. On the periphery it decelerates because of resistance to the wall of conductor. This report offers a specific application of the above theory. In order to understand the nature of superconductivity we have to understand first the nature of conductivity by conductor. Then we can very easily model a superconductor by constructing it orthogonally on the conductor.
