Physical Significance of the Transition from Classical to Non-classical Behavior
in the Orbits of Stars

In MQ Form

9.072419 10^3 light-years

When the effective mass exceeds the mass frequency bound, measurable mass exceeds what can be measured. The result is observed as a constraining phenomenon on the strength of gravity (more commonly referred to as the dark matter phenomenon).

Inputs

  • θsi can be measured as the polarization angle of quantum entangled X-rays at the degenerate frequency of a maximal Bell state. As an angle θsi=3.26239 rad ± 2 μrad; as a momentum θsi=3.26239030392(48) kg m s-1 and with respect to the Target Frame, θsi has no units. The relation of angle and mass is mathematically demonstrated, as well, by No-Ping Chen, et. al.
  • lf, mf and tf are the fundamental measures, more precise expressions for Planck’s units – length, mass, and time – that consider the effects of length contraction associated with discrete measure.
  • nLr describes the count of lf representative of a change in position of an observable measured with respect to the observer’s frame of reference.
  • vm is the modelled velocity best reflecting the measurement data.
  • ve is the escape velocity associated with a gravitational mass.
  • ve is the effective velocity, a function of the effective mass – that count of mf constrained by the Planck frequency – and reflecting the mass profile of a system.
  • R is the distance between a center of mass and an inertial frame.

Terms

  • vb is the bound velocity that corresponds to the bound mass constrained by the Planck frequency.
  • nLr describes the count of lf representative of the position of an observable with respect to the frame of a center of mass.
  • nLc describes the count of lf representative of a change in position of light measured with respect to the observer’s frame of reference.
  • H is the value of H0 m s-1Mpc-1 when resolved with respect to universal expansion (i.e., the Target Frame).
  • HU is the rate of universal expansion with respect to the diameter of the universe (per DU). This differs from stellar expansion (i.e., Hubble’s description).
  • c is the speed of light which may also be written as c=nLlf/nTtf=299,792,458 m/s such that nL=nT=1 is physically significant.
  • Mtot is the total mass of the universe, including all forms of energy.
  • Macr is the rate of mass accretion in the universe.
  • Me is the effective mass which represents the gravitational mass measurable by an observer.
  • Mb is the bound mass which represents the upper count bound of mf that can be measured per tf in a homogenous mass distribution.

Calculations


Experimental Support

[4]   McGaugh, S.S.: Milky Way Mass Models and MOND (2008) ApJ, 683, 137-148, doi:10.1086/589148.

[5]   McGaugh, S.S.: A Precise Milky Way Rotation Curve Model for an Accurate Galactocentric Distance (August 2018) Res. Notes AAS, 2, 156, doi:10.3847/2515-5172/aadd4b.


Discussion

While the mystery surrounding dark matter has been difficult, perhaps as puzzling is why star velocities are consistently much faster than expected across a galactic disk, yet roughly the same across the outer 2/3rds of a disk. One might conjecture there are two effects at work. We will describe both and identify their intersection.

In this article we specifically address what we call the quantization crossover. This is defined as that distance from a galactic core where the total mass of a system exceeds the measureable mass. Using the Measurement Quantization (MQ) approach to classical description, we resolve this distance at the Planck frequency bound, the upper count bound of fundamental units of mass mf that can be measured per increment of fundamental time tf.

Without going into too much detail regarding physical support for MQ, we refer the reader to several articles, noting here that MQ recognizes that the notion of measure is a count phenomenon with respect to length, mass and time references as resolved with respect to the internal Measurement Frame of the observer. Likewise, it is shown that because the universe has no external reference, the Target Frame of the universe must be non-discrete. And when considering the difference between these frames, we resolve values and expressions for the physical constants and the laws of nature.

Importantly, discrete measures carries with it a length contraction effect - the Informativity differential. This effect is not related to Einstein's relativity.

This effect can and has already been measured with respect to existing CODATA publications for the values of G and ħ. Over the last decade, there has been little agreement as to what these values should be. In the paper entitled, Measurement Quantization, we use our understanding of this effect to calculate G and ħ, thus identifying the conditions of each experiment used for the 2010, 2014, and 2018 publications.

[1]   P. Mohr, B. Taylor, and D. Newell, CODATA Recommended Values of the Fundamental Physical Constants: 2010, p. 73 (2012), arXiv:1203.5425v1, doi:10.48550/arXiv.1203.5425.

[2]   P. Mohr, B. Taylor, D. Newell, CODATA Recommended Values of the Fundamental Physical Constants: 2014, p. 3, (2015), arXiv: 1507.07956v1, doi:10.1063/1.4954402.

[3]   NIST: CODATA Recommended Values of the Fundamental Physical Constants: 2018, (May 2019), https://physics.nist.gov/cuu/pdf/wall_2018.pdf, doi:10.1103/RevModPhys.93.025010.

We now turn our attention to count bounds, for instance, the count relation between fundamental length and time, often described with respect to the speed of light. We call this the length frequency bound. It describes the upper count bound of length measures per count of time measures. In that the fundamental measures are references and therein do not have smaller physically significant features such as contraction/dilation or curvature, we separate the counts from the measures. With this MQ nomenclature, we recognize and can demonstrate that it is the counts that vary.

As such, we also recognize a mass frequency bound, that is the upper count bound nM of mass measures with respect to a count nT of time measures . And finally there is the length-to-mass count bound nL/nT.

With this foundation, we carry out calculations to resolve the bound velocity and then the associated bound mass for a system. This is resolved with respect to the internal Measurement Frame of the observer and must then be transformed against the Target Frame, by multiplying by θsi. Thereafter, we contrast the relation with the effective velocity and corresponding effective mass and reduce.

The expression is complicated in that data regarding the mass distribution of a galaxy is difficult to gather. Most often, source data comes in the form of velocity measurements, such as that by McGaugh's mass model data representing the first 85,000 lightyears of the Milky Way. This data is then modelled using MOND to describe what is observed.

We refer the reader to the linked article on dark matter for details. As regards this calculation, our focus is identifying the quantization crossover, the point where the modelled mass increases above the bound mass. We have identified this distance at 9.072419 103 light-years. This is the radial distance at which star velocities flat line. Thereafter all velocities are roughly equal for the remainder of stars across the disk.

We emphasize, not all galaxies will demonstrate flat lining across the entire disk. This behavior will only appear so long as the effective mass (red curve) exceeds the bound mass (purpose line). Even with respect to the Milky Way, this behvior disappears near the edge of the disk.

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