Modern Cosmology Dodelson Problem 6.12b (Inflation)

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Homework Help Overview

The problem involves demonstrating a relationship in modern cosmology related to inflation, specifically showing that \(4\pi G(\dot \phi)^2=\epsilon a^2 H^2\). The context includes equations of motion for the scale factor \(a\), the Hubble parameter \(H\), and the energy density \(\rho\) and pressure \(P\) in a cosmological setting.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • The original poster attempts to manipulate various equations related to the scale factor and the energy density to derive the desired relationship. Some participants question the correctness of the original poster's expressions and suggest careful reevaluation of the derivatives involved.

Discussion Status

Participants are actively engaging with the problem, with one participant successfully resolving their confusion after reassessing the second derivative of the scale factor. There is acknowledgment of typographical errors in the original equations, which have been corrected in the discussion.

Contextual Notes

There are indications of potential misunderstandings regarding the relationships between derivatives and the physical quantities involved, as well as the need for careful attention to the signs in the equations.

travelingscienceman
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Homework Statement



Show that ##4\pi G(\dot \phi)^2=\epsilon a^2 H^2##

Homework Equations



Over dots mean derivative with respect to ##\eta##.
$$\frac{1}{a}\frac{d}{d\eta}=\frac{d}{dt}$$
$$H=\frac{\dot a}{a^2}$$
$$\epsilon=\frac{-\dot H}{aH^2}$$
$$(\frac{\dot a}{a^2})^2=(\frac{da/dt}{a})^2=\frac{8\pi G\rho}{3}$$
$$\frac{\ddot a}{a^3}=\frac{d^2 a/dt^2}{a}=-\frac{4\pi G}{3}(\rho-P)$$
$$\rho=\frac{1}{2}(\frac{d\phi}{dt})^2 + V(\phi)$$
$$P=\frac{1}{2}(\frac{d\phi}{dt})^2 - V(\phi)$$
$$\frac{d\phi}{dt}=\frac{\dot\phi}{a}$$

The Attempt at a Solution



First I plug ##\epsilon## into the main equation so I get ##4\pi G(\dot phi)^2=-a \dot H##. Then I find
$$\dot H=\frac{\ddot a a-2\dot a^2}{a^3}$$
$$-a\dot H=\frac{2\dot a^2-\ddot a a}{a^2}=2a^2(\frac{\dot a}{a^2})^2-a^2\frac{\ddot a}{a^3}$$
$$=a^2(\frac{16\pi G}{3}\rho+\frac{4\pi G}{3}(\rho+3P))$$
$$=a^2\frac{4\pi G}{3}(4\rho +\rho+3P)=a^2\frac{4\pi G}{3}(5\rho +3P)$$
$$=a^2\frac{4\pi G}{3}(\frac{5}{2}\frac{\dot\phi^2}{a^2}+5V+\frac{3}{2}\frac{\dot\phi^2}{a^2}-3V)$$
$$=a^2\frac{4\pi G}{3}(4\frac{\dot\phi^2}{a^2}+2V)$$

Which is where I have problems as I cannot simplify things further to get the desired ##4\pi G(\dot \phi)^2##. If the 2V was gone and there was one less factor of ##\dot \phi^2## then I would get the right answer, but I keep coming to this same equation. Any help would be appreciated. Thanks in advance!
 
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travelingscienceman said:
$$ \frac{\ddot a}{a^3}=\frac{d^2 a/dt^2}{a}=-\frac{4\pi G}{3}(\rho-P)$$
##\large \frac{\ddot a}{a^3} \neq \frac{d^2 a/dt^2}{a}## You will need to be careful when relating ##\large \frac{d^2 a}{dt^2}## to ##\ddot a##.

Also, ##\large \frac{d^2 a/dt^2}{a}## ##\neq -\frac{4\pi G}{3}(\rho-P)##. Looks like a typographical error here. Shouldn't the ##-P## be ##+3P##?
 
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Thanks for your help once again! I was able to solve it after reevaluating ##\frac{d^2 a}{dt^2}## and got ##\frac{\ddot a a-\dot a^2}{a^3}##.

And yeah it's 3P, messed up typing it in.
 
travelingscienceman said:
I was able to solve it after reevaluating ##\frac{d^2 a}{dt^2}## and got ##\frac{\ddot a a-\dot a^2}{a^3}##.
Looks good.
 

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