A1
^{ ??}
Does the Hubble law imply that the solar system is in the region of the Universe where the Big Bang occurred? (Because Hubble made his observations from the Earth!) Explain your answer with a drawing and formula.

A2
^{ ??}
Calculate the gravitational potential energy $E_G$ of the NU at a time $t$ when its radius is equal to $R$. Give your answer as a formula expressing $E_G$ in terms of $M$ and $R$.

*Remark:* if the mass of the system increases from $m$ to $m + \Delta m$ without any changing the relative mass distribution, the gravitational potential energy increases by

\[ \Delta E_G = \int\limits_0^{\Delta m} \varphi \, dm,\]

where $\varphi$ is a gravitational potential at the point of mass $dm$. Also $\varphi$ is chosen so that $\varphi=0$ on infinity.

H1
Use Guass's law for the gravitational field

\[\int_\Gamma \vec{g} \cdot d\vec{S} = -4\pi Gm,\] where $m$ is the mass enclosed within the closed surface $\Gamma$ to find a gravitational field and a gravitational potential in the universe.

\[\int_\Gamma \vec{g} \cdot d\vec{S} = -4\pi Gm,\] where $m$ is the mass enclosed within the closed surface $\Gamma$ to find a gravitational field and a gravitational potential in the universe.

H2
The gravitational field $g(r)$ in the massive ball with radius $R$ and mass $M$

\[ g(r) = GM \frac{r}{R^3}\]

\[ g(r) = GM \frac{r}{R^3}\]

H3
The gravitational potential $\varphi(r)$ in the massive ball with radius $R$ and mass $M$

\[ \varphi(r) = -\frac{3GM}{2R} + \frac{GMr^2}{2R^3}.\]

\[ \varphi(r) = -\frac{3GM}{2R} + \frac{GMr^2}{2R^3}.\]

A3
^{ ??}
Calculate the kinetic energy $E_K$ of the NU at the same time $t$. Give your answer as a formula expressing $E_K$ in terms of $M$, $H$ and $R$.

A4
^{ ??}
At what relation between $\rho(t)$ and $H(t)$ will the expansion of the NU stop at a finit size and be replaced by compression? Give the answer in the form of an inequality.

H1
The total energy of the universe is conserved.

A5
^{ ??}
Let the total energy of matter in the NU, i.e. the sum of kinetic energy and potential energy of gravitational interaction, be equal to

\[E = -\frac{2}{15} Mc^2,\]

where $c$ is the speed of light in vacuum. Find the maximum radius of the NU in the process of expansion. Write down the formula and get a numerical answer in parsecs ($1 ~\text{parsec}$ is approximately equal to $3.2~\text{light years}$, or $3\cdot10^{16}~\text{m}$).

\[E = -\frac{2}{15} Mc^2,\]

where $c$ is the speed of light in vacuum. Find the maximum radius of the NU in the process of expansion. Write down the formula and get a numerical answer in parsecs ($1 ~\text{parsec}$ is approximately equal to $3.2~\text{light years}$, or $3\cdot10^{16}~\text{m}$).

A6
^{ ??}
For the conditions described in question A5, find the total lifetime of the NU from the Big Bang to the Big Implosion. Write down the formula and get a numerical answer in years.

*Remark:* $$ \int\limits_{0}^{1} \frac{\sqrt{x}}{\sqrt{1-x}} d x=(y=\sqrt{1-x})=2 \int\limits_{0}^{1} \sqrt{1-y^{2}} d y $$

H1
To calculate the integral mentioned in the remark, you can use the substitution $y = \sin \phi$.

A7
^{ ??}
What are the options for further motion of matter in the Universe at different ratios between the density and the Hubble constant? Describe the qualitative behavior of the NU radius for each of the possible cases. Draw graphs: three different pairs of graphs showing the NU radius $R$ and the rate of its expansion $\dot{R}$ versus time $t$ (keep in mind that at the time of the Big Bang $t = 0$ and the radius of the NU is considered to be almost zero). Draw the graphs qualitatively, showing all the important details and features.