d.3
d.1 Another modality of action of the matter.
d.2 Useful values of the angular movement.
d.3 Other features of the “action d”.
d.4 “Action d” and thermodynamic balances.
d.5 Effects of the “action d” on the Earth.
Other features of the “action d”.
Its formula.
.1
The formula of the “action d” would resemble that used for gravitation, with the important difference that the distance is to be raised to the 3rd power (as we see in the case of the ocean tides), and not to the 2nd power.
Range of action.
.2
Thus its range of action is limited, in comparison to that of the gravity.
.3
Indeed, only the movements of the two masses - the Moon, and the Sun - would have enough range of action, to act on the configurations of water molecules, in our planet.
.4
As for those of the EFAs molecules in seeds, so far, only the movements of the Moon have shown to have effects.
Interacting with the other forces.
.5
The gravitation, the other long range force of the matter, has not shown to act in the discrete ways, typical of the short range forces; nor to interact with them. At least, so far.
.6
On the contrary, the “action d”, in more than one instance reported in this work, shows clearly not only to behave in discrete ways, but also to interact with magnetism (insert E).
.7
Furthermore, an open structure molecule, that is not in a magnetic field, seems not to be able to take advantage of the “action d”, as activation energy.
.8
These features of the “action d” are susceptible to provide the ground for more comprehensive theories on the behaviour of the matter, maybe suggesting the missing link between the short range forces, and the long range ones.