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Consider a PN junction diode

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Now, this system will naturally form a depletion region due to diffusion and will convert into this-

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Now, I wish to connect the ends of this diode with a conducting wire and resistance like this-

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Thus, I expect the electric field in this space to be aligned as follows (Indicated din green)-

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This will make the charges in the wire accumulate in the following way-

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And finally, this system will end up neutralizing all the charges so that no electric field remains inside and outside the diode; creating equilibrium state for the free charges. So, we are going to be back on a simple p-n junction diode with no depletion region and no electric fields.

However, this will again create a difference in electron concentration between n and p sides; these high-speed free electron will naturally flow from n-side to p-side creating an electric field which would later be balanced by the conducting wire.

I thus expect this cycle to go on and on leading to continuous charge flow through the resistance. Overall, the diode will be taking up heat from the surroundings, while the resistance would be releasing heat there.

Obviously I expect this analysis to be wrong, but I am not able to figure out where did I made any mistake?

Qmechanic
  • 220,844

1 Answers1

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The p side of a p-n junction is not at a higher potential with respect to the n side.

p only indicates the presence of free to move positive charges. It is still neutral(due to the presence of fixed negative charges) and charges won't suddenly start flowing when it is connected to the n side.

Edit:

The potential difference does not act like a standalone battery. Think of it this way. The $V_{diff}=0.7 V$ for a Si diode. Now when we apply a potential of 0.6V, No Current flows through the diode. So the $V_{diff}$ is actually a variable quantity which is equal to the applied voltage for upto a fixed value and then remains a constant.