Collision of a free electron and a hydrogen atom - energies

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SUMMARY

The discussion revolves around the collision of a free electron with a hydrogen atom in its ground state, specifically analyzing the kinetic energy (KE) of the electron post-collision. The initial KE of the electron is 11.5 eV, which can either remain unchanged if it misses the orbiting electron or be reduced to 10.2 eV if it excites the electron to the n=2 state. The energy levels are defined by the equation E_n = -E_0/n², where E_0 is 13.6 eV. The conversation also addresses the conditions under which the orbiting electron can be excited and the implications of energy conservation in the collision process.

PREREQUISITES
  • Understanding of kinetic energy in particle collisions
  • Familiarity with quantum mechanics, specifically the Schrödinger equation
  • Knowledge of quantized energy levels in hydrogen atoms
  • Basic principles of electron transitions between energy states
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  • Explore the concept of quantized energy levels in hydrogen and other atoms
  • Investigate electron collision theory and energy transfer mechanisms
  • Learn about higher energy transitions in hydrogen and their requirements
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kapitan90
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Homework Statement


An electron of know KE collides with a hydrogen atom in its ground state. With what possible KE may it rebound?
KE = 11.5 eV

2. The attempt at a solution
I assumed that the electron may either hit an orbiting electron and excite him (maximum layer is n = 2, change in KE = 11.5 - (13.6 - 3.4) = 1.3 eV)
or miss it (KE unaltered = 11.5eV)

Those answers are correct, yet I don't understand them fully.

3. Relevant questions
How do we know that the orbiting electron will take the maximum amount of energy it can take? Is it a simplification or a free electron has to give this amount of energy to the orbiting electron? Why?

Also, can we speak of 'rebounding off the atom' if the electron doesn't hit the free electron? It cannot collide with atom's nucleus as it's energy is unaltered, so how may it rebound?
 
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If it collides with the nucleus, since the nucleus is so massive, it will just bounce right back with its energy unchanged. It is like throwing a ball against a brick wall.

The orbiting electron can only exist in quantized states. To see why, you will have to solve the Schrödinger equation. The energy of any state is

E_n = - \frac{E_0}{n^2}

where n is an integer, and E0 is the ground state energy 13.6eV. So the incident electron can only rebound with quantized energy levels.

K_f = K_i - \Delta E_{atom} = K_i - (E_n - E_0)
 
But why can't an orbiting electron be excited to n = 1, only to n = 2?
 
kapitan90 said:
But why can't an orbiting electron be excited to n = 1, only to n = 2?

For higher transitions, it will take more and more energy. Does the incident electron have enough energy to make the orbiting electron transfer from n=1 to n=3?
 

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