Dimensions
of an electric charge
When
writing the formulas of attraction of two masses M (Newton's law) and
two charges Q (Coulomb's force), both are oppositely charged forces (
attraction and repulsion)
On each side in equation (1) there is a "force". Both these forces should, according to our inicial hypothesis, have the same "dimensions". This force will be
named "negative" if it is an attraction force (two masses that
are attracted to each other, according to Newton) and "positive"
(when two electric charges of the same signs repel each other, according
to Coulomb's formula) . Equation (2)
provides two solutions to Q ==>> Q = i M and
Q = - i M with (i)² = - 1 Similarly, two positive
or two negative masses will attract each other (negative force) and two
oppositely charged masses will repel each other (positive force), according
to the same Newton formula ( 1/ R² ). The dimensions of charge will therefore be the same as the dimensions of mass, but complex: i L³/T² or - i L³/T². Some electric quantities will also have "complex" dimensions. i represents a "complex" or "imaginary" number, defined by the relation: ( i)² = - 1 We can even assume that a "space-time" deformation will have a real component (mass) and a complex component (charge). In a general M + iQ and the general formula of attraction of "masses-charges" becomes: F = ((M1+iQ1).(M2+iQ2))/R²
(3) This force will have two real components (two masses attract each other and two charges of the same signs repel each other). ((M1).(M2))/R²
and ((iQ1).(iQ2))/R² This same force will
have two complex components ( charge does not affect mass). In LorentzHeaviside units (also called rationalized) the Coulomb constant is ke = 1/4 p )
Since we know that the electric charge has i L3 T -2 we can determine the dimensions of:
Those same quantities can vary in relation to time:
Electrical quantities (charge, potential, intensity, electric field) would be therefore complex quantities, contrary to mechanical quantities, that would be real and directly measurable. To measure an electrical
quantity (charge, potential, intensity, electric field) it will be necessary
to use electricity to obtain a real, measurable quantity (for example
force or displacement). For example, a charge (complex quantity) situated in an electric field (another complex quantity) will result in a force (real quantity) that will have the same dimensions as mechanical force ( L4 T -4 ). We can also see that an electric potential (volt V) with a certain intensity (ampere A ) will result in a power ( W = VA ) that will have the same dimensions as a mechanical power ( L5 T -5 ). On the other hand,
a charge (complex quantity) situated in a gravitational field (real quantity)
will result in an unmeasurable real quantity (complex force?). Some
fundamental relations in physics (complex quantities are in
red, " i L3 T-2" will be written as " L3
T -2 ") Q.Ê
= F (
L3 T
-2 ) ( L1 T -2 ) =
( L4 T -4 ) => charge
. elecric field = force
Dimensions
of some quantities in physics (complex
quantities in red) acceleration
= ( L1 T -2 ) |