Mean free path of electron in gas.

In summary: Stanford Linear Accelerator. In summary, the mean free path for electrons in a gas is affected by the number of molecules, volume, and the motion of oncoming particles. For electrons to travel 3 km through the SLAC without significant scattering losses, the pressure inside the accelerator must be reduced to a point where the mean free path is at least 50 km. Assuming a temperature of 50°C, the maximum possible pressure inside the tube can be calculated using the ideal gas law.
  • #1
lacunae
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Homework Statement



The expression for the mean free path in a gas of a particle with radius r is
((N/V)*pi*r^2*4*(2)^.5)^-1
in which N is the number of molecules, and V is the volume, and the factor of √2 in the denomiator accounts for the motion of the oncoming particles in the gas. Electrons can be thought of as point particles with zero radius.

Electrons travel 3 km through the Stanford Linear Accelerator (SLAC). In order for
scattering losses to be negligible, the pressure inside the accelerator tube must be reduced to the point where the mean free path of the electrons is at least 50 km. What is the maximum possible pressure inside the tube, assuming T=50 C? Give your answer in Pascals.

Homework Equations



a) None other than the one above.
b) PV=NkT

The Attempt at a Solution



The model used to describe mean free path is the number of molecules within a cylinder of radius r swept out by a particle over a distance v*t. The number of molecules within the cylinder = number of collisions. However, since electrons have no radius, I'm not sure where to go from here. The "cylinder" would have to be infinitely small, hence no collisions, and an infinite mean free path. The SLAC is filled with He or N2, can't remember which, but putting in the radius for one of these molecules doesn't seem correct to me. The second part is easy enough, but I am absolutely stuck on the first half. Any help is appreciated.
 
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  • #2
If the electron approximates an atom within the radius of the atom they will collide. You can imagine that the electron carries the scattering cross section instead of the atoms and the atoms of the gas are stationary points inside the cylinder.

ehild
 

Related to Mean free path of electron in gas.

What is the mean free path of an electron in gas?

The mean free path of an electron in gas is the average distance an electron travels between collisions with other particles in the gas. It is a measure of how far an electron can travel without being scattered or absorbed by other particles in the gas.

What factors affect the mean free path?

The mean free path is affected by the density of the gas, the temperature, and the cross-sectional area of the particles in the gas. Higher gas density and lower temperature will result in a shorter mean free path, while larger particle cross-sections will result in a longer mean free path.

How is the mean free path calculated?

The mean free path can be calculated using the following equation: λ = (1/σn), where λ is the mean free path, σ is the collision cross-section of the particles in the gas, and n is the number of particles per unit volume. This equation assumes that the particles in the gas are uniformly distributed and do not interact with each other.

Why is the mean free path important in gas physics?

The mean free path is important in gas physics because it helps us understand how particles move and interact in a gas. It is also a key factor in determining the transport properties of gases, such as thermal conductivity and viscosity.

How does the mean free path differ for different gases?

The mean free path can vary significantly between different gases due to differences in particle size, density, and temperature. For example, at the same temperature and pressure, the mean free path of helium will be much shorter than that of oxygen due to its smaller particle size.

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