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Chapter 3: The extension of the momentum order

 

So far, the momentum of an electron pair which the momentum order handles placed in the mind only the direction (abbreviating with " the direction of electric current " after this) in which the permanent current flows. I extend it by my creation to the direction (abbreviating with " the direction of electromagnetic force " after this) in which the electromagnetic force by the outer magnetic field acting on the permanent current arises.

 

Let's think of what to take place when not doing this extension.

 

The basics: The impulse and the momentum

The impulse is " force ~ time ".

Supposing that the force is F and that the time is T, an impulse is shown by FT.

The force is " mass ~ acceleration ".

Supposing that the acceleration is ƒΏ, supposing that the mass is M, it becomes F=MƒΏ (Newton's second law of motion).

Since a momentum is " mass ~ velocity ", supposing that the velocity is V,

momentum is shown by MV.

There is a relation that the impulse is equal to the momentum.

I multiply both sides of "F=MƒΏ" by T.

T~F=MƒΏ~T

The left side shows an impulse.

I think about the right side.

Since the velocity is " acceleration ~ time ", it becomes V=ƒΏ~T.

I substitute this for the right side.

The relation of "FT=MV" is formed.

Therefore, the impulse which was added to the permanent current becomes the momentum of electron pairs.

The impulse of the electromagnetic force made by the outer magnetic field acting on the permanent current, too, changes into the momentum.

 

There are cases where the strength of the outer magnetic field isn't uniform.

Since the strength of the outer magnetic field isn't uniform, impulses whose sizes are different are supposed to have been given in a definite time to each electron pair which composes a permanent current.

 


Figure 6: When impulses of different size are given to electron pairs; a

 

Suppose that these impulses are changed into momentums just as they are.

 

Figure 7: Outcome of the impulses of different size which have changed into the momentums; a

 

Combining the momentum in the direction of electric current with the momentum in the direction of electromagnetic force, the size of the combined momentum which an electron pair as a whole has becomes scattered. Under the present condition, the momentum order that each electron pair has a same momentum and changes the momentum into the other same momentum isn't realized. The electric resistance arises and the permanent current will collapse.

 

Therefore, the regulation by the momentum order works in the direction of the electromagnetic force, too, and the extra impulse is thought to be canceled without changing into the momentum of the motion of center of gravity of electron pairs. And the impulse which could not change into the momentum is thought to change into the other energy. That is not the energy of the motion of center of gravity of electron pairs but the kinetic energy of each electron. This other energy is slipped outside as heat energy through the scattering of each electron.

 

 


Figure 8: The regulation of the momentum order to act on the impulses of different size; a

The impulses beyond " Constant value by the momentum order " are canceled.

 

Figure 9: The outcome of the regulation of the momentum order to have acted on the impulses of different size; a

 

 

As a result, the momentum of each electron pair changes into the same momentum all together, the momentum order is materialized and the permanent current flows permanently.

 

Then, when the minimum one of the impulse given to an electron pair by the electromagnetic force doesn't fill a constant value in a constant time, I think that all impulses are canceled without changing into momentums. It is because an electron pair, too, is a quantum to think of the constant value. The superconductivity is said to be a macro quantum phenomenon. Then, it is because of the thought that the function of the regulation of the momentum order, too, has a limit of ability to think of the constant time. Then, if the impulse given in the constant time doesnft change into the motion of center of gravity, all of the impulse change into the other energy.

 


Figure 10: When impulses of different size are given to electron pairs; b

 

Under the present condition, the combined momentums become scattered like figure 7.

 

Figure 11: The regulation of the momentum order to act on the impulses of different size; b

The regulation of the momentum order acts on the all impulses.

 

Figure 12: The outcome of the regulation of the momentum order to have acted on the impulses of different size; a

 

All impulses are canceled without changing into momentums.

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