Calculate the age of the Universe at a temperature

AI Thread Summary
The discussion revolves around calculating the age of the Universe at a temperature of T = 1 MeV, with an initial condition of a(t=0)=0. The calculated Hubble parameter at this temperature is approximately H(1 MeV) ≈ 0.6 s⁻¹, leading to a derived age of t = 0.85 s in a radiation-dominated Universe. The importance of the condition a(t=0)=0 is clarified as essential for defining the integration constant in the Friedmann equations, ensuring a correct derivation of the relationship between scale factor and time. The conversation highlights the connection between the Hubble parameter and the scale factor's evolution, emphasizing the role of initial conditions in cosmological calculations. Understanding these concepts is crucial for accurately modeling the early Universe.
Denver Dang
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Homework Statement


I've been told to calculate the age of the Universe at T = 1 \, \text{MeV}, assuming that a(t=0)=0.

Homework Equations


Now, I've already calculated the value of H at that temperature, which was around H(1\,\text{MeV}) \approx 0.6 \,\text{s}^{-1}. I've also shown, that in a radiation dominated Universe, which I assume much be the case at T = 1 \, \text{MeV}, that:
H = \frac{1}{2}t^{-1}

The Attempt at a Solution


So basically, my idea was just to solve for t in that equation, and use the value for H I calculated, and then I end up with t = 0.85 \, \text{s}, which seems okay reasonable to me, but, my main question is the info: "assuming that a(t=0)=0". I haven't really used that information here, so either it's just not important, or I have missed something. But what ?
 
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You cannot derive ##H = \frac{1}{2}t^{-1}## without that convention. It is needed to define where t=0 is.
 
Well, I have shown that:

\rho _R =\rho_{R0}\left(\frac{a_0}{a}\right)^{4}

So from the Friedmann equation I get:

\begin{align}
\frac{\dot a^{2}}{a^{2}} &= \frac{8 \pi G}{3} \frac{\rho_{R0}}{a^{4}} \nonumber \\
&\Updownarrow \nonumber \\
\left(a\frac{da}{dt}\right)^{2} &= \frac{8 \pi G}{3} \rho_{R0} \nonumber \\
&\Updownarrow \nonumber \\
a\frac{da}{dt} &= \sqrt{\frac{8 \pi G}{3}\rho_{R0}} \nonumber \\
&\Updownarrow \nonumber \\
a\,da &= \sqrt{\frac{8 \pi G}{3}\rho_{R0}} \,\, dt \nonumber \\
&\Updownarrow \nonumber \\
\int a\, da &= \sqrt{\frac{8 \pi G}{3}\rho_{R0}} \int dt \nonumber \\
&\Updownarrow \nonumber \\
\frac{1}{2} a^{2} &= \sqrt{\frac{8 \pi G}{3}\rho_{R0}} \, t \nonumber \\
&\Updownarrow \nonumber \\
a &= \sqrt[4]{\frac{32 \pi G}{3}\rho_{R0}} \, t^{1/2} \nonumber \\
&\Updownarrow \nonumber \\
a &\propto t^{1/2}
\end{align}

And from that I, again, can use the Friedmann equation, giving:

\begin{align}
H &= \frac{\dot a}{a} \nonumber \\
&\Updownarrow \nonumber \\
H &= \frac{\frac{da}{dt}}{a} \nonumber \\
&\Updownarrow \nonumber \\
H &= \frac{1}{t^{1/2}} \frac{d}{dt}t^{1/2} \nonumber \\
&= \frac{1}{t^{1/2}} \left(\frac{1}{2}\frac{1}{t^{1/2}}\right) \nonumber \\
&= \frac{1}{2} t^{-1}
\end{align}

That's how I got the other equation.
 
The step where you perform the integration over dt and over a da should have a free integration constant. Fixing a(t=0)=0 sets this constant to zero.
 
Hmmm, I'm not sure I follow. How does that help me ?
 
What do you mean with "help"? You asked where you need the additional information you had, and I answered that question. The result is the same as before, but now with a correct derivation.
 
Ah, I see what you mean now. Sorry for the confusing on my part.
Thank you very much :)
 
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