Axiomatic Formulation of «A Derivation of Faraday's law from Coulomb's Law and Relativity»

 

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A Derivation of Faraday's law from Coulomb's Law and Relativity / 1.The Progressing Electric Field Model

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Erosion protection of Tokamak and magnetic force on single charge

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Letter to readers for the new magnetic force law

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PengKuan’s work on electromagnetism

From Coulomb’s force to magnetic force and experiments that show magnetic force parallel to current

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Longitudinal magnetic force and high field magnet

Showing tangential magnetic force by experiment

Plasma under Coulomb magnetic force

5th methode: Positively charged coils for confinement

Since Fsp is created by the currents that produce the magnetic field for confining plasma, Fsp is a force that attracts the positive particles qa toward the currents. So, we can create in the wires for confinement a positive electric field E that pushes the positive particles qa off the wires, see Figure 6. Because E is contrary to Fsp, the positive ions of the plasma are kept off the wall.

As the circuit for confinement magnetic field is already well insulated, the positive electric field can be created just by putting a high voltage on the whole circuit for confinement after disconnecting the circuit from the ground.

However, the reaction chamber must be insulated from the ground because the positive charge in the wire will create a capacitance with the metallic chamber which will be charged negatively by a current from the ground and annihilate the electric field E inside the chamber.

The voltage should be adjusted such that the force on the electrons from the electric field E balances the force Fsp to avoid the contact of the electron with the wall of the chamber.

This method is explained in the article.

 

Coulomb magnetic force

Changing distance effect

Continuous rotation of a circular coil experiment

Tangential magnetic force experiment with circular coil

Length-contraction-magnetic-force between arbitrary currents

Relativistic length contraction and magnetic force

A 1.95 m long solenoid exerting Aharonov–Bohm force on a coil

Sliding wire parallel action experiment

Correction:

Today, I have done this experiment with a larger magnet whose magnetic field has much smaller vertical component. But the wire did not move. When I approached the wire to the edge of the magnet where the vertical component is stronger, the wire moved. So, the yesterday's conclusion was wrong: the movement of the wire was due to the the vertical component near the edge but not due to force parallel to current.

I apologize for having posted a wrong result.

However, I think it's useful to keep this post for those who have already read it in order to inform them this correction. It is also good for me to remember this disaster.

Sorry again.

PengKuan

Disc magnet parallel action experiment

Earth’s magnetic field and parallel action

More photograph of the hairpin wire