Jump to content
Main menu
Main menu
move to sidebar
hide
Navigation
Main page
Recent changes
Random page
freem
Search
Search
Appearance
Create account
Log in
Personal tools
Create account
Log in
Pages for logged out editors
learn more
Contributions
Talk
Editing
Openai/6897769e-4ee4-800f-aba5-69cca34f701c
(section)
Add languages
Page
Discussion
English
Read
Edit
Edit source
View history
Tools
Tools
move to sidebar
hide
Actions
Read
Edit
Edit source
View history
General
What links here
Related changes
Special pages
Page information
Appearance
move to sidebar
hide
Warning:
You are not logged in. Your IP address will be publicly visible if you make any edits. If you
log in
or
create an account
, your edits will be attributed to your username, along with other benefits.
Anti-spam check. Do
not
fill this in!
===== Assume the Universe can be modelled as causal spheres of radius R(t)=c tR(t)=c\,tR(t)=ct and that each independent angular quantum (mode) on the boundary contributes a fixed mass unit m⋆m_\starm⋆ (emergent mass per mode). The number of modes up to angular resolution set by a microscopic length scale ℓ\ellℓ (for example, proton Compton length λp=h/(mpc)\lambda_{p}=h/(m_p c)λp=h/(mpc)) is ===== Nmodes(t) ∼ 4πR(t)2ℓ2 ⇒ Mu(t) ∼ m⋆ 4πc2t2ℓ2.\mathcal{N}_{\rm modes}(t)\;\sim\; \frac{4\pi R(t)^2}{\ell^2} \;\Rightarrow\; M_u(t)\;\sim\; m_\star\,\frac{4\pi c^2 t^2}{\ell^2}.Nmodes(t)∼ℓ24πR(t)2⇒Mu(t)∼m⋆ℓ24πc2t2. This gives Mu∝t2M_u\propto t^2Mu∝t2 directly. * Choose ℓ\ellℓ as a fixed microscopic length (Compton wavelength), then Mu(t)mp∼4πm⋆mp(ctℓ)2.\frac{M_u(t)}{m_p}\sim \frac{4\pi m_\star}{m_p}\left(\frac{c t}{\ell}\right)^2.mpMu(t)∼mp4πm⋆(ℓct)2. If m⋆∼mpm_\star\sim m_pm⋆∼mp up to constants, you recover the Dirac large-number squares N∼(ct/ℓ)2N\sim (ct/\ell)^2N∼(ct/ℓ)2. Strengths: Simple, geometric, matches Dirac scaling exactly. Weaknesses: Why should mass be assigned per angular mode? Conservation issues: where does the energy come from? Must specify m⋆m_\starm⋆ mechanism and explain local matter-energy conservation.
Summary:
Please note that all contributions to freem are considered to be released under the Creative Commons Attribution-ShareAlike 4.0 (see
Freem:Copyrights
for details). If you do not want your writing to be edited mercilessly and redistributed at will, then do not submit it here.
You are also promising us that you wrote this yourself, or copied it from a public domain or similar free resource.
Do not submit copyrighted work without permission!
Cancel
Editing help
(opens in new window)