Systems and methods of interacting complex electric fields and static electric fields to effect motion are disclosed. An example method includes producing an action force having a reaction force perpendicular to the action force by interacting a relative velocity electric field based on charge of a moving first charged object and a static charge on a second charged object in a different inertial frame of reference. Another example method includes producing an action force having a reaction force perpendicular to the action force by interacting an acceleration generated electric field based on acceleration of a first charged object and a static charge on a second charged object in a different inertial frame of reference. Another example method includes producing an action force having a reaction force perpendicular to the action force by interacting a scalar electric potential and static electric field. 1. A method comprising producing an action force having a reaction force perpendicular to the action force by interaction of a relative velocity electric field based on charge of a moving first charged object and a static charge on a second charged object in a different inertial frame of reference. 2. The method of claim 1, wherein the relative velocity electric field is defined by a cross product of velocity and charge of the first charged object and the static charge on the second charged object. 3. The method of claim 1, wherein the relative velocity electric field is defined by a dot product of velocity and charge of the first charged object and the static charge on the second charged object. 4. The method of claim 1, wherein the relative velocity electric field is defined by a potential of a dot product of velocity and charge of the first charged object and the static charge on the second charged object. 5. The method of claim 1, wherein the interacting is defined by acceleration generated electric fields of an accelerated charged object. 6. The method of claim 1, further comprising amplification of the relative velocity electric fields from moving different charged objects. 7. The method of claim 6, wherein the amplification of the relative velocity electric fields is perpendicular to the direction of motion over a flat moving charged object. 8. The method of claim 6, wherein the amplification of the relative velocity electric fields that is in a direction of motion over a flat moving charged object. 9. The method of claim 6, wherein non-amplification of the relative velocity electric field is over a curved moving charged object. 10. The method of claim 1, wherein the relative velocity electric fields are produced from electric potentials that are decoupled from the first and second charged objects. 11. A method comprising producing an action force having a reaction force perpendicular to the action force by interacting an acceleration generated electric field based on acceleration of a first charged object and a static charge on a second charged object in a different inertial frame of reference. 12. A system comprising: a first charge-holding object, and a second charge-holding object; means for producing an action force having a reaction force perpendicular to the action force by interacting a relative velocity electric field based on a charge of moving the first charge-holding object and a static charge on the second charge-holding object in a different inertial frame of reference. 13. The system of claim 12 wherein the charge-holding objects include a dielectric. 14. The system of claim 12 wherein the charge-holding objects include are electrically conductive. 15. The system of claim 12 wherein the charge-holding objects include are within a non-conductive assembly. 16. The system of claim 12 wherein the charge-holding objects move at different velocities. 17. The system of claim 12 wherein the charge-holding objects are accelerated at different rates. 18. A method comprising producing an action force having a reaction force perpendicular to the action force by interacting a scalar electric potential and static electric field. 19. The method of claim 18 further comprising decoupling scalar electric potentials defined by the dot product of electric charges and relative velocities and accelerations of the electric charges. 20. The method of claim 18 wherein buildup of the scalar electric potentials generates large electric fields. BACKGROUND: The mathematical framework used in physics and electrical engineering today to describe electromagnetic fields is based on work by Gauss, Faraday, and Ampere. The work is embodied in differential equations based on vector calculus, which today are referred to as Maxwell's equations. These equations were derived under the assumption that only electromagnetic fields (E and B) are physical, and that the electromagnetic potentials are purely mathematical constructs. By the 1980's the Aharonov-Bohm effect had proven the physicality of the electromagnetic potentials. The standard equations by including only the fields and not their associated potentials end up not completely describing all the effects observed from electrical convection currents. DETAILED DESCRIPTION: Magnetic forces generated from current-carrying conductors are due to the effect of Lorentz contraction of moving negative charge carriers relative to the positive stationary ions. An electric convection current is composed of moving electrical charges that have the same inertial frames of reference, generating no magnetic force in the traditional sense, but resulting in relative velocity electric fields due to Lorentz contraction when observed from different frames of reference. An action force may be generated with a reaction force perpendicular to the action force based on an interaction of complex electric fields generated from electrical convection currents. Embodiments describe rotating and stationary charged disks, conical structures, and embedded capacitor arrays to exploit relative velocity electric fields, scalar electric potentials, and acceleration-generated fields to produce axial forces and motion without standard mass expulsion.