I Some questions related to the Cosmological Constant

Arman777
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In Barbara Ryden's introduction to cosmology book its written that
"Introducing ##\Lambda## into the Poisson's equation allows the universe to be static, if you set ##\Lambda = 4\pi G\rho##"

Then later on, in the book energy density of the ##\Lambda## defined as ##\epsilon_{\Lambda} = \frac{c^2\Lambda}{8\pi G}##

But this not make much sense. Since in this case
$$\epsilon_{\Lambda} = \frac{c^2 4\pi G\rho}{8\pi G} $$
$$\epsilon_{\Lambda} = \rho/2 c^2 $$
Which is not correct.

From other sources I see that actually

##\Lambda = 8\pi G\rho## and
##\epsilon_{\Lambda} = \frac{c^4\Lambda}{8\pi G}##

And it seems that other sources definiton is the correct one. So the information on the book is wrong ? Or the ##\Lambda## for the static universe case is different then the general ##\Lambda## ?

Also,
##\epsilon_{\Lambda} = \frac{c^4\Lambda}{8\pi G}## and we know that ##\Omega_{\Lambda} = \frac{\epsilon_{\Lambda}}{\epsilon_c}##
and ##\epsilon_c = \frac{3H^2c^2}{8 \pi G}##

so we get

$$\Lambda = \frac{3H^2\Omega_{\Lambda}} {c^2}$$

So is this means that ##\Lambda## is actually a time dependent thing since it involves ##H(t)## and ##\Omega_{\Lambda}## ?
 
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Arman777 said:
$$\epsilon_{\Lambda} = \rho/2 c^2 $$
Which is not correct.
Its correct with ##c^2## in the numerator.
Arman777 said:
$$\Lambda = \frac{3H^2\Omega_{\Lambda}} {c^2}$$

So is this means that ##\Lambda## is actually a time dependent thing since it involves ##H(t)## and ##\Omega_{\Lambda}## ?
It only appears to be. With ##\Omega_\Lambda=\frac{8\pi{G}\rho_\Lambda}{3H^2}## you obtain ##\Lambda=8\pi{G}\rho_\Lambda##.
 
timmdeeg said:
Its correct with c2c2c^2 in the numerator.
Well 2 is dimensionless so it has not much effect on the equation itself. But I don't think its normal to have a 2.

timmdeeg said:
##\Lambda = 8 \pi G\rho_{\Lambda}##
So the equations on the book is wrong ?

timmdeeg said:
It only appears to be.
Hmm I see. Its also interesting. Then ##H^2(t)\Omega_{\Lambda}(t) = Constant## for all times
 
Arman777 said:
Well 2 is dimensionless so it has not much effect on the equation itself. But I don't think its normal to have a 2.
If you combine the first 2 equations in your OP you get 2 in the denominator. Nothing wrong.
Your first equation follows from the 2. Friedmann Equation with the 2. derivative of the scale factor set zero (because static).
 
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Hmm okay than
 
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