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Consider a hypothetical Universe described by the Friedmann equation,

\n

$ \\left( \\frac{\\dot{a}}{a} \\right)^{2} = \\frac{8  \\pi G \\rho}{3} - \\frac{k c^{2}}{a^{2}},$

\n

where all parameters have their usual meanings. Matter is the only contributor to the mass-energy density, with a present-day density parameter $\\Omega_{M,0} = \\var{Om}$.

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Calculate the value of the constant $k c^{2}$ as a multiple of $H_{0}^{2}$.

\n

$kc^{2}/H_{0}^{2}  =$ [[0]] 

\n

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Calculate the value of the Hubble parameter, $H$ at a redshift $z = \\var{zz}$ as a multiple of its current value $H_{0}$.

\n

$H(z=\\var{zz})/H_{0} =$ [[0]]

\n

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Calculate the matter density parameter at redshift $z=\\var{zz}$.

\n

$\\Omega_{M} (z=\\var{zz}) = $ [[0]]

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This question tests the ability to relate observed redshifts in cosmology to the expansion factors of the Universe at the times of emission and observation.

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 As observed from Earth at the present time, Galaxy A has an observed redshift of $z=\\var{za}$. Galaxy B, along the same light of sight, has an observed redshift of $z = \\var{zb}$. Calculate the redshift of Galaxy A, as seen from an observer in a Galaxy B, at the following cosmic epochs:

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At the time when the light we (on Earth) currently observe from galaxy B was emitted.

\n

[[0]]

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At the current cosmic epoch.

\n

\n

For this part, you may assume a matter-only Universe at the critical density, in which the comoving separation between a galaxy which emits light at $a=a_{1}$ and a galaxy which receives it at $a=a_{2}$ is given by

\n

$r_{cm} = \\frac{2c}{H_{0}} [ \\sqrt{a_{2}} - \\sqrt{a_{1}} ].$

\n

[[0]]

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Calculate the value of the constant $k c^{2}$ as a multiple of $H_{0}^{2}$.

\n

$kc^{2}/H_{0}^{2}  =$ [[0]] 

\n

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Calculate the value of the Hubble parameter, $H$ at a redshift $z = \\var{zz}$ as a multiple of its current value $H_{0}$.

\n

$H(z=\\var{zz})/H_{0} =$ [[0]]

\n

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Calculate the density parameters in the 3 components at redshift $z=\\var{zz}$.

\n

$\\Omega_{M} (z=\\var{zz}) = $ [[0]]

\n

$\\Omega_{\\Lambda} (z=\\var{zz}) = $ [[1]]

\n

$\\Omega_{\\gamma} (z=\\var{zz}) = $ [[2]]

\n

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Consider a hypothetical Universe described by the Friedmann equation,

\n

$ \\left( \\frac{\\dot{a}}{a} \\right)^{2} = \\frac{8  \\pi G \\rho}{3} - \\frac{k c^{2}}{a^{2}},$

\n

where all parameters have their usual meanings.

\n

The mass-energy density budget comprises contributions from matter, cosmological constant and relativistic particles (the latter including the background radiation), with present-day density parameters shown below:

\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n\n
Matter$\\Omega_{M,0} = \\var{Om}$
Cosmological Constant$\\Omega_{\\Lambda,0} = \\var{Olam}$
Radiation$\\Omega_{\\gamma,0} = \\var{Orad}$
\n

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Given this range in density, calculate the maximum possible age of the Universe, in Gyr:[[0]]

\n

State the density parameter of the Universe for the latter case:[[1]]

\n

Calculate the minimum possible age of the Universe, also in Gyr: [[2]]

\n

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A galaxy at a distance of $\\var{d}$ Mpc emits an emission line of rest-frame wavelength 500.00 nm.

\n

The recession velocity of this galaxy in km s$^{-1}$ is: [[0]].

\n

The redshift of the galaxy is: [[1]].

\n

The observed wavelength of the emission line in nm is [[2]].

\n

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Consider a hypothetical Universe with a Hubble constant of $H_{0} = \\var{h}$ km s$^{-1}$ Mpc$^{-1}$. The Universe contains only matter with an unknown density which may range anywhere from zero to the critical density.

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