This is given in Eqs. (1), (2) and (3). The first solution is given in Eqs. (9), (10) and (11). They can be combined into one general solution (4), (5) and (6). There also exist the solutions (12), (13) and (14). However these are not obeyed by a circular current loop and are considered to be too restrictive and unphysical. Eqs. (12) to (14) are obeyed only by a static magnetic field and a potential A = (B(0) / 2) ( – Y i bold + X j bold) as in previous work. This is not the vector potential of a circular current loop. The other solutions can be physically meaningful solutions for the spin connection components of a circular current loop. The next note will proceed to the most general possible solution (15), which obeys del B = 0 by construction. Conservation of antisymmetry is a fundamental law of electrodynamics, gravitation, and fluid dynamics. Any current density can be chosen, and any vector potential computed from it using Eq. (8). The current loop gives more than one possible spin connection. Antisymmetry is obeyed by construction for all solutions. It is important to note that conservation of antisymmetry entirely refutes the standard model of physics because it refutes the standard U(1) sector theory (Maxwell Heaviside theory). Therefore the electroweak theory is also refuted (U(1) x SU(2)). These are major advances in understanding. Any magnet such as a bar magnet is accompanied by pattens of spin connections in spacetime, the vacuum or aether.