Energy Density with Thomson scattering

Your Name] In summary, to determine the electron density needed for no scattering to occur when photons are crossing the universe, we use the equation ne = (8π/3)*(e^2/mec^2)^2 * c * Ho and substitute in the values for the Thomson cross section and the Hubble constant. This gives us an extremely low density of approximately 3.6 x 10^-7 electrons per cubic meter, making it impossible for a photon to cross the universe without any scattering.
  • #1
cosmoshadow
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Homework Statement



If ne represents the electron density and the interaction between particles is the photons scattering off of the electrons through the Thomson cross section, how low must the electron density be to cross the universe with no scattering?

Homework Equations



The size of the universe is given by c*(Ho^-1)


The Attempt at a Solution



I have no clue how to approach this problem. Obviously the Hubble distance is in Mpc, but I do not know the significance of the Thomson cross section. Can anyone help me to understand this problem?
 
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  • #2


Thank you for your interesting question. To answer your question, we first need to understand the concept of the Thomson cross section and its relation to electron density and scattering.

The Thomson cross section is a measure of the probability of a photon scattering off an electron. It is given by the equation σT = (8π/3)*(e^2/mec^2)^2, where e is the electron charge, me is the electron mass, and c is the speed of light. This cross section is important in understanding the scattering of light by charged particles, such as electrons.

Now, to determine the electron density needed for no scattering to occur, we need to consider the size of the universe and the distance that a photon can travel before scattering occurs. The size of the universe is given by c*(Ho^-1), where c is the speed of light and Ho is the Hubble constant. This distance is known as the Hubble distance and is approximately 4.4 gigaparsecs (Gpc).

Using this information, we can set up an equation to determine the electron density needed for no scattering to occur. Let's call this density ne. We know that the distance a photon can travel before scattering is directly proportional to the electron density and inversely proportional to the Thomson cross section. So, we can write:

c*(Ho^-1) = (1/ne)*(1/σT)

Solving for ne, we get:

ne = (σT*c)/(Ho^-1)

Substituting in the value of the Thomson cross section and the Hubble constant, we get:

ne = (8π/3)*(e^2/mec^2)^2 * c * Ho

Plugging in the values for the constants, we get an electron density of approximately 3.6 x 10^-7 electrons per cubic meter. This is an incredibly low density, and it is unlikely to be found in the universe. Therefore, we can conclude that it is not possible for a photon to cross the universe without any scattering.

I hope this helps to clarify the problem and its solution. If you have any further questions, please don't hesitate to ask.
 

Related to Energy Density with Thomson scattering

1. What is Thomson scattering and how does it relate to energy density?

Thomson scattering is the process by which photons are scattered by free electrons in a medium. In terms of energy density, Thomson scattering can affect the amount of energy present in a given volume, as the scattered photons can either add to or subtract from the energy of the medium.

2. How is energy density with Thomson scattering calculated?

Energy density with Thomson scattering is calculated by dividing the energy of the photons scattered by the volume of the medium in which the scattering occurs. This can be expressed mathematically as U = E/V, where U is the energy density, E is the energy of the scattered photons, and V is the volume of the medium.

3. What factors can affect the energy density with Thomson scattering?

The energy density with Thomson scattering can be affected by various factors such as the density of free electrons in the medium, the temperature of the medium, and the frequency of the incident photons. These factors can impact the amount of energy that is scattered and therefore contribute to the overall energy density.

4. Can energy density with Thomson scattering be measured experimentally?

Yes, energy density with Thomson scattering can be measured experimentally using techniques such as spectroscopy or interferometry. These methods involve analyzing the scattered photons to determine their energy and then using this information to calculate the energy density in the medium.

5. How does energy density with Thomson scattering compare to other forms of energy density?

Energy density with Thomson scattering is typically lower than other forms of energy density, such as kinetic or thermal energy density, due to the relatively small amount of energy involved in each scattering event. However, in certain contexts, such as in astrophysics, Thomson scattering can play a significant role in determining the overall energy density of a system.

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