Cosmic Potential Theory (CPT): Cosmology without the Big Bang or dark matter #368
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In Peter Wolff's original paper "Kosmologie ohne Urknall und dunkle Materie", his modified Newton-Mach Principle appears not as a purely conservative force but as a dissipative acceleration. As for all dissipative processes, the solution is an exponential described by the Beer-Lambert law. Wolff solves the equation (once again) to get an energy loss that follows a
Ok good, red-shifted light comes out of that dissipative gravity! We know this is the correct Hubble function (e.g. https://doi.org/10.3390/galaxies10060108) for the angular distance. However Wolff's model doesn't explain anything beyond that. How is the CMB explained? (His explanation as "thermalized starlight" has been proposed by others and was falsified.) Why is the MOND acceleration equal to "Cosmic Potential Theory" is another example of a theory invented to solve a specific problem, but it doesn't answer anything else. The theory is missing predictive power and falsifiability (either observational or theoretical falsifiability). I didn't know about this theory, thanks @luisenrique-arch for pointing it out. Another one I will add to my collection of "dead cosmologies". |
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The cmb temp evolve with redshift (1+z) this pose a fine tuning problem to the age/steady state of light. |
It starts off so simply, almost romantically, but before long we will have a score of ballet dancers and an orchestral accompaniment! The reviewers are looking for red and blue to make waves. |
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Cosmic Potential Theory (CPT): Cosmology without the Big Bang or dark matter
by Peter Wolff
Translation by lluisenrique-arch
Overview: Classical gravitation, both in Newton’s formulation and in Einstein’s General Relativity, is fundamentally a local theory. It does not, by itself, make precise claims about an infinitely extended universe unless additional assumptions about the global structure of the cosmos are introduced. A key but often implicit assumption is that a perfectly isotropic, infinitely extended spherical shell of mass surrounding any finite and observationally accessible region of the universe produces no net gravitational field inside it. This is strictly true for finite isotropic shells in both Newtonian gravity and General Relativity, as expressed by Birkhoff’s theorem. The implication is that, on very large scales and under isotropy, gravitational fields are determined only by local distributions of mass and energy. However, the Einstein-Mach principle suggests something different. It proposes that inertia, which in Newtonian physics is simply postulated, is actually induced by the total distribution of mass in the universe, including extremely distant matter. This idea, however, is not fully supported even within General Relativity, as illustrated for example by the Gödel universe model.
The Newton-Mach Principle (modified): Here we define a modified version of the Einstein-Mach idea. In this formulation, inertia is determined exclusively by the infinitely extended isotropic mass shell described above, while finite distributions of matter play only a negligible role. The advantage of this modification is that an actually infinite mass shell can, unlike a finite one, provide a physical foundation for Newton’s concept of absolute space, or at least make it plausible. On sufficiently large cosmological scales, only this infinite and isotropic mass shell is relevant. Local structures, which are anisotropic, finite and inhomogeneous, contribute only secondary corrections that vanish as the density ρ approaches zero.
Core idea of modified cosmic gravity: In an idealized homogeneous and isotropic universe extending infinitely, filled uniformly with matter, classical Kepler-Newton gravity appears not as a purely conservative force but as a kind of cosmological dissipative acceleration that slows down test masses. For light, this effect is constant because the speed of light in vacuum is locally constant and equal to c. The source of this cosmic gravitational effect is the infinite isotropic mass shell that encloses any finite observable region of the universe. Local masses within a finite region around the observer do not directly determine this global acceleration. They influence it only indirectly by shaping local gravitational fields, which can slightly redirect the global effect. This leads, in galactic dynamics, to behavior similar to MOND theories. This framework introduces a universal deceleration scale proportional to Hc, where H is related to cosmic parameters. This plays a central role in the Cosmic Potential Theory (CPT).
The static cosmology core of CPT: In standard Big Bang cosmology, the Hubble expansion is interpreted as a real expansion of space that is accelerating. In CPT, a different interpretation is proposed. Using a kind of mathematical reinterpretation based on Einstein’s equivalence principle (1907), particularly the elevator or rocket thought experiment, it is assumed that light traveling toward us is actually being gradually decelerated by gravity. At the same time, we interpret observations as if we were moving away from the light source with constant acceleration. This dual interpretation reproduces the observed redshift without requiring cosmic expansion. In this sense, the debate resembles the historical opposition between Aristotelian-Ptolemaic and Copernican-Aristarchian cosmologies. In CPT, it is not the universe that expands and accelerates. Instead, light is progressively “slowed down” or “aged” by cosmic gravitational effects.
Consequences for Hubble expansion and dark energy: The observed accelerated expansion since 1998 is interpreted in CPT as strong evidence for this framework. Within standard cosmology, the data require acceleration to fit supernova observations, but this acceleration has no intuitive physical explanation. Dark energy is introduced in standard models as an additional unknown component. In CPT, it is instead viewed as a placeholder for an unexplained interpretation of observational data within an expanding-universe framework.
Hubble constant and cosmic density: In CPT, the Hubble constant H is related to the average density of the universe ρ, which is not directly measurable on the largest scales. A plausible approximation assumes that the density ρ₀ measured on the largest accessible scales is close to the true cosmic density ρ. This yields:
H² = (8π/3) G ρ ≈ (8π/3) G ρ₀
where G is the gravitational constant. In this framework, H does not represent an expansion velocity. Instead, it represents a cosmic deceleration scale that affects light propagation and produces redshift effects without requiring expanding space.
Cosmological constant and dark energy: The cosmological constant Λ, associated in standard cosmology with dark energy, emerges in CPT as:
Λ ≈ (3/c²) H²
In standard physics, Λ is poorly constrained and can differ from theoretical vacuum energy estimates by 60 to 120 orders of magnitude depending on assumptions. In CPT, Friedmann models are not fundamental but instead act as parameter-fitting frameworks. Similarly, dark matter is not required as an independent physical substance but as a modeling parameter introduced to reconcile theory with observations.
Space-time structure in CPT: CPT describes space-time as a reinterpretation of Special Relativity combined with a Newtonian-like absolute reference frame. This frame is defined with respect to the cosmic microwave background and distant galaxies and quasars, similar to a Poincaré-Minkowski inertial frame at rest relative to the universe at large. On cosmic scales, rest and motion are distinguished physically by the presence of a gravitational deceleration field. This leads to:
MOND-like galactic dynamics: One of the strengths of CPT is that it naturally produces behavior similar to MOND (Modified Newtonian Dynamics), including flat galactic rotation curves and the Tully-Fisher relation. When gravitational accelerations fall below a characteristic scale a₀ ≈ Hc, Newtonian dynamics begins to deviate. This transition emerges naturally from including cosmic deceleration in gravitational dynamics. The MOND scale is therefore not an independent empirical constant but arises from cosmological structure itself.
Cosmic microwave background: In CPT, the cosmic microwave background is interpreted primarily as highly redshifted and thermally equilibrated starlight. Because the universe is assumed to be static, there is sufficient time for radiation to thermalize into a near-perfect blackbody spectrum. Remaining anisotropies are attributed to matter distribution and foreground effects, such as the Sunyaev-Zel’dovich effect. Importantly, unlike classical tired-light models, CPT preserves the blackbody nature of the spectrum.
Supernova observations: CPT claims to reproduce supernova type Ia luminosity-redshift relations without free parameters, relying instead on cosmic density and H. These results are presented as being competitive with or superior to standard cosmological models, which require dark energy and additional adjustable parameters.
Additional assumptions: To complete the framework, CPT introduces several supplementary hypotheses:
Original source: https://www.wolff.ch/astro/it/index.htm
What I translated is only an introduction that the author of the theory wrote on his website back in 2008. Here you can find the full paper, where the entire theory is laid out in detail:
https://www.wolff.ch/astro/ur.pdf
Unfortunately, the paper is written in German, so you’ll have to translate it little by little
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