Mean Free Time Silicon (PURCELL 4.12)

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SUMMARY

The discussion centers on calculating the mean free time between collisions of an electron in silicon at 500K, using Purcell's equation for conductivity. The conductivity value is confirmed as 0.3 (ohm-cm)-1, not 0.3 sec-1. The mean free time is derived using the formula T=(Mass*σ)/(2Ne2), resulting in a value of approximately 5.92x10-25 seconds. The factor of 2 in the equation accounts for collisions with both electrons and holes, effectively doubling the number density of mobile charge carriers.

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  • Understanding of semiconductor physics
  • Familiarity with Purcell's equations on conductivity
  • Knowledge of electron and hole density in silicon
  • Basic grasp of collision theory in physics
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  • Study the derivation of conductivity in semiconductors using Purcell's equations
  • Learn about the role of holes in semiconductor conductivity
  • Explore the implications of mean free time on electron mobility in silicon
  • Investigate temperature effects on conductivity and mean free time in semiconductors
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Homework Statement


This is Purcell 4.12... Given that conductivity in silicon at 500K is 0.3 sec-1, deduce the mean free time between collisions of an electron.


Homework Equations


Electron mass is 9.1x10-28 grams (mass of a hole is exactly the same), the charge on an electron is 4.8x10-10, the density of electrons and holes is each 1015.


The Attempt at a Solution


I solved Purcell's equation for conductivity to find mean free time instead:

T=(Mass*σ)/(2Ne2)... and I get something like 5.92x10-25 seconds. Isn't this way too small? Or did I do something wrong?
 
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Are you sure that the holes count as mobile? What is their mass? Would counting them effectively halve the time you're looking for?
 
According to page 147 of Purcell, the conductivity of pure silicon at 500 K is 0.3 (ohm-cm)-1 rather than 0.3 sec-1.
 
Ah! So the OP's problem was conversion.

What about that factor of 2?
 
I believe the factor of 2 is there because an electron could collide with either another electron or a hole. So, the number density of particles that the electron could collide with would be twice that of just the number density of electrons alone.
 

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