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Friday, July 10, 2015

The Diode and Boltzmann

What if it is possible to increase or decrease ψ at when ψ=0?  When "nothing" (ψ=0), is travelling down tc or tg at light speed, what can be done to "nothing"?

rqT used in the post "Broken Boltzmann Constant" could it be aψ the radius of ψ?  That the radius of the partial charge is the radius of ψ around the temperature particle?

Since the spin axis of the particle is also in motion and the complete electric field around the particle is the time average of spin and the motion of the spin axis. Strictly,

rqTaψ

Does it matter?  Yes, this serves as an upper bound on the value of rqT.  Lower values of rqT will result in higher values of kB.

Given,

kB=nTα2qTq24πεorqT1KqT

from the post "Broken Boltzmann Constant",  it is possible to change kB by changing nT.  We do so by popping temperature particles with their corresponding photons (just like the photoelectric effect) or allow photons to be captured as temperature particles by slowing the photons down.

VT of a diode will then change as kB changes.  All other fractured parts can be experimented with by observing their effects on the VT of a diode.

Is nT the emission coefficient, n in the diode equation?

I=Is(eVD/nVT1)

Maybe?  There are other fractured parts in kB, including N that we set to one, N=1 for an abrupt junction one n-p thick.