Understanding Vacuum Photocell: Explanation, Polarities, and Cut-off Potential

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Discussion Overview

The discussion revolves around the functioning of a vacuum photocell, focusing on the effects of polarity on its operation, the concept of cut-off potential, and the behavior of electrons in this context. Participants explore theoretical aspects, practical implications, and clarify terminology related to the photocell's operation.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested

Main Points Raised

  • One participant describes the basic setup of a vacuum photocell, noting the roles of the plate and ring in relation to the applied voltage.
  • Another participant confirms that reversing the polarity will reduce the sensitivity of the photocell but suggests it should still function.
  • A participant questions where the electrons would go if the polarities are reversed and seeks clarification on the concept of cut-off potential.
  • It is noted that reversing polarity increases the effective work function, making it harder for electrons to escape from the positively charged electrode.
  • Some participants discuss the relationship between the area of the plate and its likelihood of photon interaction, suggesting this affects sensitivity.
  • There is a suggestion that the term "cut-off" may refer to "saturation" or "stopping potential," but this remains unclear.
  • One participant posits that if electrons return to the anode when polarities are reversed, it could still be considered a current flow.

Areas of Agreement / Disagreement

Participants express varying interpretations of the effects of reversing polarity on the photocell's operation, particularly regarding electron behavior and the meaning of cut-off potential. No consensus is reached on these points.

Contextual Notes

Participants have not fully defined the cut-off potential or stopping potential, and there are unresolved questions regarding the implications of reversed polarities on current flow and electron behavior.

Karimz
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Hello. This is actually my first post in these forums and I've never really thought of posing my questions online but I've decided to give it a try.

Well about the Vacuum Photocell. I know what the setup looks like and all, but there's one thing I don't get. I'm going to say everything I know in here, so please feel free to correct me: There's a plate and a ring in the photocell surrounded by vacuum. Now if the plate is connected to the -ve terminal of a generator, it will be the -vely charged cathode while the ring becomes relatively positively charged. Supposing the UV radiation is of enough energy to extract the electrons from the plate, these electrons which leave the plate will be absorbed by the +vely charged ring and a complete circuit is achieved. What if the polarities are reversed though? What happens? The plate becomes +vely charged while the ring is now -vely charged. So now the radiation will extract electrons from this +ve plate which will be attracted/absorbed again by the plate when they leave it? Moreover, I don't really get the "cut-off potential" concept. What is really going on in the photocell, in other words? Have I misunderstood the whole concept?

Thanks in advance
 
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Welcome to PF.

You've got it about right. Reversing the polarity will make the cell much less sensitive, but it should still work.

The electrons near the surface are held in a potential well which defines the photoelectric 'work function'. To free the electron requires a certain minimum energy, called the work function ( I think ). Any energy left over will contribute to the electrons kinetic energy outside the material.

It's explained here
en.wikipedia.org/wiki/Work_function

and

en.wikipedia.org/wiki/Photoelectric_effect
 
Well yea I know about the work function and Kinetic energy left and all.. but my question is when the polarities are reversed, the electrons leaving the plate would go where? How is the cut-off potential reached? Can you define it for me please?
 
When the polarity is reversed, you are trying release electrons from a postively charged electrode , so the effective work function is greater.

A released electron will fall back to the anode unless it has enough energy to escape.

I don't know what 'cut-off' voltage you mean.
 
If you reverse the power source, like Mentz says, "will make the cell much less sensitive". The plate on which the light falls on has a larger area which will give it a greater chance of being struck by an incoming photon. As to 'cut-off' could you be meaning saturation?
 
I'm not sure but perhaps it's also called the "stopping potential" ? Also, when polarities are reversed, wouldn't it be a good thing if the electron comes back to the anode? The polarities are reversed so the flow of the current should also be opposite to what it was, meaning into that +ve plate. The ring would reject the electron since it repels it anyway, no ?
 
Karimz is right.
If the electron can't leave the anode, no current will flow. In fact I don't think it will work at all unless light falls on the cathode.
 
Well at some point an electron does leave the anode but it's attracted back to it when it leaves. But the idea that the polarities were reversed makes the anode a cathode now since it's role would be to receive electrons not lose them. So when it does lose them and attracts them again that's considered as a current flow no ?
 

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