Difference between revisions of "Evolution of Universe"

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[[Category:Standard Cosmological Model|2]]
 
[[Category:Standard Cosmological Model|2]]
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<div id="SCM_24"></div>
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<div style="border: 1px solid #AAA; padding:5px;">
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=== Problem 28 ===
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Find the redshift dependence of the deceleration parameter. Analyze the limiting cases.
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<div class="NavFrame collapsed">
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  <div class="NavHead">solution</div>
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  <div style="width:100%;" class="NavContent">
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    <p style="text-align: left;">
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$$
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\begin{gathered}
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  q \equiv  - \frac{a\ddot a}{\dot a^2} =  - \frac{\ddot a}{a}\frac{1}{H^2}; \\
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  \frac{\ddot a}{a} =  - \frac{4\pi G}{3}\sum\limits_i \left( \rho _i + 3p_i \right) =  - \frac{1}{2}H_0^2\sum\limits_i \Omega _{i0}\left(1 + 3w_i\right)(1 + z)^{3\left(1 + w_i\right)} ;  \\
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  H^2 = H_0^2\sum\limits_i \Omega _{i0}(1 + z)^{3\left( 1 + w_i \right)};  \\
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  q = \frac{3}{2}\frac{\sum\limits_i \Omega _{i0}\left( 1 + w_i \right)(1 + z)^{3\left( 1 + w_i \right)}}
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{\sum\limits_i \Omega _{i0}(1 + z)^{3\left( 1 + w_i\right)} } - 1\\
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\end{gathered}
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$$
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In the SCM
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$$
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q = \frac{1}{2}\frac{\Omega _{m0}(1 + z)^3- 2\Omega _{\Lambda 0} }
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{\Omega _{m0}(1 + z)^3+\Omega_{\Lambda 0}}
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$$
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$$
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q(z \to \infty ) = \frac{1}{2},\;q(z \to  - 1) =  - 1
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$$
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<gallery widths=600px heights=500px>
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File:12_24.jpg|
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</gallery>
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Dependence of the deceleration parameter on the redshift.
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</p>
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  </div>
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</div></div>

Revision as of 08:51, 4 October 2012


Problem 28

Find the redshift dependence of the deceleration parameter. Analyze the limiting cases.