Biomedical Engineering Reference
In-Depth Information
Figure 2.2
Field forms. (a) CEM, (b)QFTand (c)SFT.
the E and H fields of SFT. In QFT the fields (potentials) are modelled
as impulse functions specified at charge points. Within SFT, a pair
of particles defines the bi-spinorial field and its motion, this pair
of particles and its bi-spinorial field form a unique couple. Due to
orthogonality the fields of this couple do not influence any other
chargesapartfromthecouple.ThetransitoftheSFTfieldisspecified
viathebi-spinorialfunctionandassumesvariousmotions,including
spiral helices as it transits between the electron and proton within
thehydrogenatom.ThereisavastdifferencebetweentheSFTtime-
variant field motion and the time-invariant CEM where the field
ubiquitously covers all solid angles with no definition other than its
vector nature as to the actual field motion, field flux being the only
indicatoroffieldmotion.Similarlytheuncertaintyofthefieldwithin
QFT is related to its lack of a complete and coupled EM bi-spinorial
field form.
There are other major differences, including an absence of
Heisenberg's uncertainty principle (HUP) within SFT. As the photon
is modelled via bi-spinors uncertainty is obviated. In SFT the
electron's self-fields are modelled via a complete EM function that
explicitly includes both E and H fields, enabling the complete
analysis of the mutual self-field effect between two particles. Unlike
the quantum potentials that are expectations yielding probabilistic
solutions, the bi-spinorial field variables of SFT allow completely
deterministic solutions. This results in a clearer picture of the
physics that includes the particle-photon interactions and the
binding mechanism. The solution is complete (coupled) and based
on the first-order ML equations; hence neither SR nor gauge
