On Mon, 18 Feb 2013 12:22:40, "Tom Potter" <email@example.com> wrote:
> > "Will Janoschka" <firstname.lastname@example.org> wrote in message > news:DmJ5SKFdRQph-pn2-oCtz7KLHB26Z@209-142-179-161.dyn.centurytel.net... > > On Sun, 17 Feb 2013 09:13:37, "Tom Potter" <email@example.com> wrote: > > > >> 1. The most fundamental physical property is angular displacement. > >> > >> 2. Quantum changes occur when systems exchange angular displacement. > >> > >> ( You can add or take away cycles from a pendulum > >> or oscillating system. ) > >> > >> 3. The most fundamental quanta of change is best modeled by "i' > >> ( The square root of minus one. ) > >> > >> 4. i^1 = a quarter cycle counter-clockwise angular displacement > >> i^2 = a half cycle counter-clockwise angular displacement > >> i^4 = one cycle counter-clockwise angular displacement > >> i^n = n quarter cycles counter-clockwise angular displacement > >> i^4n = n cycles counter-clockwise angular displacement > >> > >> 5. Changes occur in quanta of i^n > >> http://www.microwaves101.com/Encyclopedia/quarterwave.cfm > >> > >> http://www.microwaves101.com/ENCYCLOPEDIA/smithchart.cfm > >> > >> 6. The quanta units of angular displacement include: > >> a. cycles = i^n/4 > >> b. half cycles ( cycles * 2 ) > >> c. Quarter cycles ( cycles * 4) > >> > >> 7. The real number units of angular displacement include: > >> a. radians = ( 2 * pi * cycles ) > >> ( Which is an angular displacement referenced to a space unit.) > >> b. action = Planck's Constant * i^n/4 > >> ( Which is an angular displacement referenced to an energy unit.) > >> > >> 8. Angular displacements are measured using > >> an external standard frequency source. > >> > >> Since 1967, the International System of Units (SI) has defined > >> the second as the duration of 9192631770 cycles of radiation > >> corresponding to the transition between two energy levels of the > >> caesium-133 > >> atom. > >> > >> In other words, although i^n is the most fundamental quanta of change, > >> in order to measure it, > >> it must be referenced to an external source, > >> and at the present time, > >> that reference is an energy level transition of the caesium-133 atom. > >> > >> 9. The Potter Equation is the most fundamental physics equation. > >> x = e^(i^n * m*pi) = e^((i^n)^2 * k) > >> > >> It expands the "Euler Identity" equation (e^(i*pi) + 1 = 0) > >> http://www.songho.ca/math/euler/euler.html > >> > >> and relates pure math to physical reality. > >> > >> ( Note that "m" and the "k" > >> interface quanta angular displacements to a linear space. > >> 2*pi*r, pi*d, k = pi*n*r ) > >> > >> The Potter Equation which features quanta of angular displacement > >> > >> is more fundamental than e = hf > >> ( Which features Planck's quanta of action.) > >> > >> and is more fundamental than e = mc^2 > >> ( Which features Einstein's non existent quanta of energy.) > >> > >> 10. Change is conveyed from sources to sinks in quanta of i^n, > >> ( Quarter wave quanta ) > >> > >> Planck's Constant is a constant > >> used to convert angular displacement quanta to action. > >> ( i^n * h = action ) > >> > >> And Einstein's quanta of energy is action quanta "h" affected by > >> velocity. > >> ( energy = hf and relative motion affects f.) > >> > >> 11. Several other constants come into play > >> when equating measurements based on > >> either cycles (Quanta) or radians (Real) to reality > >> > >> Cycles are bosons and many bosons can occupy a point. > >> > >> ( You can add or take away cycles from a pendulum > >> or oscillating system. ) > >> > >> The measured value of a batch of bosons > >> depends upon how the measurement is made > >> and expressed: > >> > >> peak > >> peak to peak > >> average > >> rms, > >> quasi-peak > >> etc. > >> > >> Observe that peak and peak to peak > >> quantize a batch of bosons at a point in time > >> whereas quasi-peak, average and RMS > >> quantize the batch over some time period. > >> > >> 11. Quanta of angular displacement tend to > >> migrate from high temperature systems > >> to contiguous lower temperature systems. > >> > >> For more information visit my physics web site. > >> http://220.127.116.11/~tompotte/menu.html > >> > >> I think this post is bulletproof > >> and like to see anyone shoot a hole in it. > >> > >> I welcome feedback, comments, criticism, > >> and even sharpshooting. > >> > >> (A 'sharpshooter' criticizes without offering suggestions.) > >> > > > > Very good mathematics, but nothing to bring home the bacon. > > Sorry just a engineering viepoint. -will- > > > > Ps, I still think Erwin's stuff is more fundimental. > > If you want to do the math, fourspace is inadequate. > > Try thinking in octonions! (just a suggestion) > > Here's some bacon for you. > > 1. i^4n = n cycles counter-clockwise angular displacement > > 2. Observe and auto-correlate the cycles associate with various "cycle" > sources, > preferably cycles associated with pulsars. > http://en.wikipedia.org/wiki/Autocorrelation > http://en.wikipedia.org/wiki/Pulsar > "For some millisecond pulsars, the regularity of pulsation is more precise > than an atomic clock." > > 3. Use the Doppler and Hubble effects to project three points > with the highest auto-correlations onto the surface of a sphere > and reference all celestical objects and events to the sphere surface. > > ( Assuming that space is homogeneous, > all object and event locations can located within the volume of the sphere. > It would be useful to project ALL objects and events onto > the model sphere surface and add velocity and space "tags" > to indicate it's location and motion in the volume.) > > 4. Use the pulsar with the highest auto-correlation as a > time/space/clock/calendar reference. > > a. Sync a local oscillator to the pulsar, > and use the frequency of the oscillator as your time unit. > > b. Use time unit pulses to drive the clock to synchronize with Earth days. > > c. Use time unit pulses to drive the calendar to synchronize with Earth > years. > > d. Use the "standing wave" from the local oscillator > as your space unit. > http://www.microwave.gr/content/lecher.gif > > 5. Use the time interval of your reference point as your time unit > to open and close a gate, and count the number of counts > from other e-m sources to determine the frequencies of those points. > http://www.radio-electronics.com/info/t_and_m/frequency_counter/counter_basics.php > > 6. Accumulate the cycles received from a "coherent" source with a blackbody > to equate temperature to an i^4 count. > > 7. Generate heat with friction, chemical reactions, etc. > to equate mechanical and chemical heating effects to the heating effect > from one's heat generating i^4n source. > > 8. Use the space units from #4d to establish an Earth baseline > and use geometry to find the distances to > nearby celestical objects. > ( Use i^1, i^2, i^3, and i^4 as direction references, > and use the local oscillator to subdivide to finer angle units.) > > 9. As can be seen form lesson 3 at: > http://18.104.22.168/~tompotte/menu.html > > The time equivalence of a mass can be obtained by multiplying the mass by a > universal time per mass constant "k". > > time equivalence(mass(A)) = mass(A) * k > > k = G / C^3 > C = universal distance per interaction-time constant ("speed of light") > G = universal gravitational constant > > I will show the link between angular displacement > with most physical properties when I get time. > > Making bacon. > http://im3-tub-com.yandex.net/i?id=270345054-29-72&n=21 > Please understand that you said. I welcome feedback, comments, criticism, and even sharpshooting.
I have little knowledge in what you post, It is interesting, Is it useful?