There is no global meaning to energy conservation. There is the Hamiltonian 
constraint Nℌ = 0, which just says that for a local region where the lapse 
function can be parallel translated to the energy is zero. This is for 
Petrov type O solutions 

Nℌ = 0 = ½(da/dt)^2 - 4πGρa^2/3c^3 - k

Which leads to the FLRW constraint

(a’/a)^2 = 8πGρ/3c^3 – k/a^2 a’ = da/dt

Where the Hubble parameter H = 70km/s-Mpc  is (a’/a)^2 = H^2. This means 
that in a local region we have energy conservation FAPP. The difficulty is 
this is not a property of the symmetries of the system so we have no way to 
extend this globally.

What this ultimately means is that all physics is local. It does not mean 
we have mass-energy locally vanishing. The apparent increase in the kinetic 
energy due to expansion is well enough compensated for by a decease in 
gravitational potential energy. There is nothing mysterious going on here. 
All this means is there is a limitation or horizon to our ability to know 
if there are global symmetries to the universe. As such there is no meaning 
to conservation principles.

LC


On Friday, May 8, 2020 at 3:00:18 AM UTC-5, Alan Grayson wrote:

> If it's not conserved, as seems implied by the red shift due to expansion, 
> where does it go? TIA, AG
>

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