Solving Friedmann Equation w/ Friedmann Eqn Hmwk Stmt

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Homework Help Overview

The discussion revolves around solving the Friedmann equation using a parametric open solution involving the scale factor \( a(\psi) \) and time \( t(\psi) \). Participants are attempting to show that these expressions satisfy the Friedmann equation through substitution and manipulation of derivatives.

Discussion Character

  • Exploratory, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants are exploring different methods to relate the derivatives of the scale factor and time with respect to the parameter \( \psi \). There are attempts to express \( \dot{a} \) in terms of \( \psi \) and to manipulate the resulting equations to achieve the desired equality.

Discussion Status

Some participants have provided alternative approaches to express the derivatives and are questioning the correctness of each other's calculations. There is ongoing exploration of algebraic manipulation to equate both sides of the Friedmann equation, but no consensus has been reached on the correctness of the approaches taken.

Contextual Notes

Participants are working under the constraints of the problem statement and are questioning the validity of their assumptions and calculations without resolving them. There is a focus on ensuring that the expressions derived align with the original Friedmann equation.

Logarythmic
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Homework Statement


By substituting in

\left( \frac{\dot{a}}{a_0} \right)^2 = H^2_0 \left(\Omega_0 \frac{a_0}{a} + 1 - \Omega_0 \right)

show that the parametric open solution given by

a(\psi)=a_0 \frac{\Omega_0}{2(1-\Omega_0)}(\cosh{\psi} - 1)

and

t(\psi)=\frac{1}{2H_0} \frac{\Omega_0}{(1 - \Omega_0)^{3/2}}(\sinh{\psi} - \psi)

solve the Friedmann equation.2. The attempt at a solution
I get

\dot{a} = a_0 \frac{\Omega_0}{2(1 - \Omega_0)}(\dot{\psi}\sinh{\psi})

and

\dot{\psi}=\frac{2H_0(1-\Omega_0)^{3/2}}{\Omega_0(\cosh{\psi}-1)}

but I can't get to the first equality. Is this the correct approach?
 
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You may find it easier to write \dot{a} = \frac{\frac{da}{d\psi}}{\frac{dt}{d\psi}}. Dividing by a_0 and squaring should leave you with some expression involving only \psi. A little algebra is then all you need to re-express things in terms of a.
 
I get the right hand side to equal

H^2_0 \frac{2(1-\Omega_0}{\cosh{\psi}-1}

and the LHS

H^2_0 \frac{(1-\Omega_0)\sinh^2{\psi}}{(\cosh{\psi}-1)^2}

but I can't get them equal...
 
I agree with your second expression from computing da/dt, but I think you've made a mistake with your first expression.
 

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