# Gravitational Potential Energy

## Practice

### practice problem 1

- Calculate the speed needed to escape the Earth from its surface.
- Calculate the speed needed to escape the sun at the distance of the Earth's orbit.
- Calculate the speed needed to escape the Milky Way from the position of our solar system 25,000 light years from the galactic center or half the distance to the edge of the galaxy. (The sun's orbit encloses a mass that is 78.3 billion times the mass of the sun.)

#### solution

- Answer it
- Answer it
- Answer it

### practice problem 2

- If the sun were a black hole what would be the radius of its event horizon?
- If the Earth were a black hole what would be the radius of its event horizon?
- If you were a black hole what would be the radius of your event horizon?

#### solution

- Answer it
- Answer it
- Answer it

### practice problem 3

When we look at galaxies and other objects outside our own Milky Way we see that they are generally moving away from us and that their recessional velocities are nearly directly proportional to their distance. This observation was first made in 1929 by the American astronomer Edwin Hubble (1889–1953) and is now known as Hubble's law. Mathematically, Hubble's law is written…

*v* = *Hr*

where…

v = |
the object's recessional velocity (usually stated in km/s) |

r = |
the object's distance from the Milky Way (usually stated in megaparsecs or Mpc) |

H = |
a constant of proportionality known as the Hubble constant (69.3 ± 0.8 km/s/Mpc). |

Perform the following set of calculations.

- Given that one parsec equals 3.08568 × 10
^{16}m…- Convert the Hubble constant to SI fundamental units.
- By how much does a meter of space expand in ten years? About how big is this?
- How far away in light years is a distant quasar if it appears to be moving away from us at 90% of the speed of light?
- How far away in light years is the edge of the observable universe? (Your answer to this question can also be used to determine the age of the universe.)

- Will the universe continue expanding forever or will gravity eventually cause it all to collapse in a big crunch?
- Derive an expression for the critical density of the universe. (Hint: Use the formulas for escape velocity, the Hubble law, and the density of a uniform sphere.)
- Compute the critical density in terms of hydrogen atoms per cubic meter.
- Speculate on the fate of the universe given that the mean density of a galaxy is roughly one hydrogen atom per cubic centimeter while the mean density of the space between galaxies is about one hydrogen atom per cubic meter.
- Speculate on the fate of the universe given that the Hubble constant appears to be increasing.

#### solution

The solutions to this practice problem can be found in the discussion section of this topic.

### practice problem 4

Signatories to the Outer Space Treaty of 1967 agreed that they "shall not place nuclear weapons or other weapons of mass destruction in orbit or on celestial bodies or station them in outer space in any other manner". That hasn't stopped them from doing feasibility studies, however, or looking for loopholes in the law. Is a massive object a weapon? What if there was a satellite orbiting the earth that was full of massive objects? Massive objects with dimensions similar to a telephone pole made of a dense material? Would that be a weapon? Drop one from space and tell me what happens.

Schemes like this have been in the works in the United States since 1964 (under the informal name of Project Thor) and are revived from time to time — for example, by the RAND Corporation in 2002 and by the US Air Force in 2003. They have been described as hypervelocity rod bundles, orbital telephone poles, and Rods from God. They have also been met with legal, political, economic, and scientific skepticism. It was also used as a plot device in the 2013 action-adventure movie GI Joe: Retaliation.

Given the values in the table to the right, determine the following quantities for a hypothetical, hypervelocity, orbiting, rod bundle system…

characteristic | value |
---|---|

platform altitude | 8,000 km |

rod diameter | 40 cm |

rod length | 7 m |

rod material | tungsten carbide |

rod density | 15,630 kg/m^{3} |

- the orbital speed of the platform
- the orbital period of the platform
- the mass of one rod
- the energy to de-orbit one rod (the energy needed to change its orbital speed to zero)
- the gravitational potential energy of one rod relative to the surface of the earth
- in joules
- in tons of TNT equivalent

- the impact velocity of a de-orbitted rod (disregarding aerodynamic drag and the rotational motion of the earth)

#### solution

The orbital speed of the platform

*F*_{c}= *F*_{g}*mv*^{2}= *Gm*_{1}*m*_{2}*r*^{2}*r**v*=√ *Gm**r**v*=√ (6.67 × 10 ^{−11}Nm^{2}/kg^{2})(5.97 × 10^{24}kg)(6,670,000 m + 8,000,000 m) *v*= 5,210 m/sThe orbital period of the platform in hours and minutes

∆ *t*=∆ *s*= 2π *r**v**v*∆ *t*=2π(6,670,000 m + 8,000,000 m) 5,210 m/s ∆ *t*= 17,692 s = 4:55The mass of one rod

*m*= ρ*V*= ρπ*rh**m*= (15,630 kg/m^{3})π(0.20 m)(7 m)*m*= 68,700 kg = 68.7 tonnesThe energy to de-orbit one rod (the energy needed to change its orbital speed to zero)

*K*= ½*mv*^{2}*K*= ½(68,700 kg)(5,210 m/s)^{2}*K*= 9.32 × 10^{11}J = 932 GJThe gravitational potential energy of one rod relative to the surface of the earth

*U*= −_{g}*Gm*_{1}*m*_{2}*r*∆ *U*= −_{g}*Gm*_{1}*m*_{2}⎛

⎝1 − 1 ⎞

⎠*r*_{0}*r*∆ *U*=_{g}(6.67 × 10 ^{−11}Nm^{2}/kg^{2})(5.97 × 10^{24}kg)(68,700 kg)× ⎛

⎝1 − 1 ⎞

⎠(6,670,000 m) (6,670,000 m + 8,000,000 m) ∆

*U*= 2.24 × 10_{g}^{12}J = 2,240 GJ = 2.24 TJOne ton of TNT is equivalent to 4.184 GJ by definition.

∆ *U*=_{g}2,240 GJ = 535 tons TNT 4.184 GJ/ton TNT I would call this half a ton of TNT to be less precise, yet more meaningful.

The impact velocity of a de-orbitted rod (disregarding aerodynamic drag and the rotational motion of the earth)

*v*= √2∆ *U*_{g}*m**v*= √2(2.24 × 10 ^{12}J)68,700 kg *v*= 8,075 m/s