Hellmut1956 said:
In the moment of the Big Bang the universe had the size of a "mathematical point" and then it started to expand.
Describing "the singularity" as a "mathematical point" is not a good approach when we try to understand what really happened. When we try to explain "How the universe begin?" we should always use the "singularity" and try to avoid the term like "point".
Hellmut1956 said:
1.1 There was an initial "speed" of how the universe expanded.
We know that in the cosmic inflation theory, SM (Standart Model) particles created after the inflation (by inflation). Hence we can say that in the inflation period the universe was de Sitter Universe, where ##a(t)∝e^{Ht}## (Not exactly like this but close to this). Now, Inflation happened and SM particles get created by inflation and then (since there are now matter and radiation) the universe starts to evolve in a different way, For example, In the early universe radiation will be dominated and the universe will evolve like ##a(t)∝t^{\frac {1} {2}}## after a time the effect of the radiation density to the expansion will be unimportant. Hence, the universe will evolve as a matter dominated case, which ##a(t)∝t^{\frac {2} {3}}##.
Hellmut1956 said:
-did the "dark energy" then already impacted as an accelerating moment to the expansion rate that did "equal" the slowing effect of gravity approximately 5 billion years ago?
I will separate your question into the two parts. First part is that the density of the cosmological constant doesn't change with time. It's a just a property of the cosmological constant.
The second part is about the Hubble Parameter, In the early universe as I said the density of the radiation had much more effect on the Hubble parameter. Why? Because the density of the Radiation goes by ##a^{-4}## while the matter is ##a^{-3}## and as I said the density of the cosmological constant doesn't change with time.
So let's make a chronological order,
After the inflation universe was radiation dominated, then it turned to be matter dominated, and in the future when the density of the matter gets really low, the universe will be Lambda-dominated. And scale factor will be proportional to the ##e^{Ht}## as I described above.
In this sense the answer to your question will be; Lambda was affecting the same because the density of the lambda doesn't change with time. But the expansion rate was a bit higher. Because for a matter dominated universe H goes like ##\frac {2} {3t}## so in the past H was a bit higher.
Hellmut1956 said:
Can we identify how the effect of the expansion rate of the universe was, is and will be in the future due to the 2 effects, gravity and dark energy impacting it?
You can use the Friedmann Equation in this form.
##\frac {H^2} {(H_0)^2}=Ω_{0,R}a^{-4}+Ω_{0,M}a^{-3}+Ω_{0,κ}a^{-2}+Ω_{0,Λ}##
For a flat universe ##Ω_{0,κ}=0## and we can also assume ##Ω_{0,R}=0## (Since radiation density is only important in the early universe) then we have,
##\frac {H^2} {(H_0)^2}=+Ω_{0,M}a^{-3}+Ω_{0,Λ}##
You should take ##a(t_0)=1## so that the ##a## term in the equation will represent the past
For example 5 billion years ago, scale factor will be, ##a(t)=0.625##
you can do this from here,
http://home.fnal.gov/~gnedin/cc/