# Citobehavior equations

Citobehavior equations are equations that deal with the interrelationships of the different types of behavior of cidentireplicas.

An example of a citobehavior equation is the:

$4_u4_wBD_\rightsquigarrow^{\S_{x_n}^{y_n}} \blacktriangleleft Cito_u(O,U,E,D_\rightsquigarrow^{\S{x_n}},T,S,C) =\!\!B\!\!= Cito_w(O,U,E,D_\rightsquigarrow^{\S{y_n}},T,S,F)$

Any cidentireplica traveling through any path through space will have an identical behavior to that produced by any different cidentireplica traveling a different path through space, if $Cito_u(O,U,E,T,S,C) == Cito_w(O,U,E,T,S,F)$, for every point on the path. This equation represents the Principle of Transitive Spacial Citobehavior.

Specific case Equation $1.4BE_1^2D_1^2 \blacktriangleleft Ori(O,U,E_1,D_1,T,S,F) =\!\!B\!\!= Cito(O,U,E_2,D_2,T,S,F)$

This is the specific case of citobehavior. It states that the original with a specific materiality and place will have the behavior of a cidentireplica with a different specific materiality and placement when all the other conditions are met.

General case Equation $1.4BE_1^m,D_1^n \blacktriangleleft Ori(O,U,E_1,D_1,T,S,F) =\!\!B\!\!= Cito(O,U,E_m,D_n,T,S,F)$

This equation is the mathematical representation of principle 2 of the first chapter. The cidentireplica if made of different matter (E m rather than En ) , and in a different space (D2 rather than D1,) if it had the same structure S , in the same time T, and functioning the same F, will have the same behavior.

The equation $1.4MO \blacktriangleleft Ori_{(O)} =\!\!M\!\!= Cito_{(O)}$ is true at time t=0 after t=0 the original can function any divergent way from that of the cidentireplica. Because the functioning is not specified.