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From: Xaustein on 13 Jun 2010 13:37
In electrostatics we have defined the positive charge and the charge
negative, depending on when Catacroc electrostatic charges are not
we move to a similar position when the masses
show relative motion of one over the other, ie
when the radial component of the total field is zero and we only
the field is tangential way:

+ / - Sqr (a ^ 2 - r ^ 2) * b / r

Well defined as cargo "positive" tangential field
for the sign "+" square root "sqr (a ^ 2 - r ^ 2)" and
as cargo "negative" for the tangential field "-" sign
square root.

The repulsive force between like charges is due to because of
"Spin" of the tangential fields cancel each other in space
that between two loads and add in the "not between charges"
and the attractive force between unlike charges is due to the "spin"
tangential field join each other in the space between
charges and subtract in the "not between charges."

Greetings.
From: Xaustein on 13 Jun 2010 13:38
On 13 jun, 19:37, Xaustein <gx...(a)xtec.net> wrote:
> In electrostatics we have defined the positive charge and the charge
> negative, depending on when Catacroc electrostatic charges are not
> we move to a similar position when the masses
> show relative motion of one over the other, ie
> when the radial component of the total field is zero and we only
> the field is tangential way:
>
> + / - Sqr (a ^ 2 - r ^ 2) * b / r
>
> Well defined as cargo "positive" tangential field
> for the sign "+" square root "sqr (a ^ 2 - r ^ 2)" and
> as cargo "negative" for the tangential field "-" sign
> square root.
>
> The repulsive force between like charges is due to because of
> "Spin" of the tangential fields cancel each other in space
> that between two loads and add in the "not between charges"
> and the attractive force between unlike charges is due to the "spin"
> tangential field join each other in the space between
> charges and subtract in the "not between charges."
>
> Greetings.

En electrostática tenemos definidas la carga positiva y la carga
negativa, según la electrostática del Catacroc cuando las cargas no
se
mueven tenemos la situación equivalente a cuando las masas no
presentan movimiento relativo la una respecto de la otra, o sea,
cuando la componente radial del campo total es nula y solamente nos
queda el campo tangencial de forma:

+/- sqr(a^2 - r^2) * b/r

Pues bien definimos como carga "positiva" el campo tangencial
correspondiente al signo "+" de la raiz cuadrada "sqr(a^2- r^2)" y
como carga "negativa" el campo tangencial correspondiente al signo
"-"
de la raiz cuadrada.

La fuerza repulsiva entre cargas iguales es debida a que por causa
del
"spin" del campo tangencial se anulan uno con el otro en el espacio
que hay entre ambas cargas y se suman en el espacio "no entre
cargas",
y la fuerza atractiva entre cargas distintas es debida a que el
"spin"
del campo tangencial se suman uno con el otro en el espacio entre
cargas y se restan en el espacio "no entre cargas".

Saludos.
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