- #1
Logarythmic
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Homework Statement
By substituting in
[tex]\left( \frac{\dot{a}}{a_0} \right)^2 = H^2_0 \left(\Omega_0 \frac{a_0}{a} + 1 - \Omega_0 \right)[/tex]
show that the parametric open solution given by
[tex]a(\psi)=a_0 \frac{\Omega_0}{2(1-\Omega_0)}(\cosh{\psi} - 1)[/tex]
and
[tex]t(\psi)=\frac{1}{2H_0} \frac{\Omega_0}{(1 - \Omega_0)^{3/2}}(\sinh{\psi} - \psi)[/tex]
solve the Friedmann equation.2. The attempt at a solution
I get
[tex]\dot{a} = a_0 \frac{\Omega_0}{2(1 - \Omega_0)}(\dot{\psi}\sinh{\psi})[/tex]
and
[tex]\dot{\psi}=\frac{2H_0(1-\Omega_0)^{3/2}}{\Omega_0(\cosh{\psi}-1)}[/tex]
but I can't get to the first equality. Is this the correct approach?