Stopping Potential in Photoelectric Effect Experiment

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Discussion Overview

The discussion revolves around the concept of stopping potential in the photoelectric effect experiment, exploring its implications on electron flow and current measurement. Participants examine the conditions under which electrons emitted from a cathode can be stopped from reaching an anode and the effects of potential differences in the system.

Discussion Character

  • Exploratory
  • Technical explanation
  • Debate/contested
  • Mathematical reasoning

Main Points Raised

  • Some participants question whether the stopping potential should be equal to the cathode potential, suggesting that if equal, there would be no potential difference and current would stop.
  • Others argue that the stopping potential must be more negative than the cathode potential to repel even the fastest electrons, preventing them from reaching the anode.
  • A participant notes that if the cathode is grounded, making the anode at the same potential would mean everything is grounded, allowing electrons to reach the anode and register a current.
  • There is a discussion about the behavior of emitted electrons when a stopping potential is applied, with some suggesting that they become motionless while others clarify that they are pushed away from the anode and do not become motionless due to the external field.
  • One participant introduces the concept of an insulated plate next to the photoelectron emitter, discussing how electrons would accumulate on that plate and affect its potential, leading to a stopping condition.
  • Another participant mentions that both emission and recombination of electrons occur simultaneously, leading to a maximum space charge around the emitter.
  • Concerns are raised about the introduction of insulators complicating the understanding of the photoelectric effect, with a suggestion to focus on the straightforward physics of the standard experiment.

Areas of Agreement / Disagreement

Participants express differing views on the nature of stopping potential and its effects on electron behavior, indicating that multiple competing views remain without a consensus on the implications of these concepts.

Contextual Notes

There are unresolved assumptions regarding the definitions of stopping potential and the behavior of electrons in various configurations, such as grounded versus insulated plates. The discussion also highlights the complexity introduced by insulators in the photoelectric effect context.

Molar
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In the photoelectric effect experiment..it says - the stopping potential should be more negative (-V) than the cathode plate to stop the current...but
i) should not it be equal to the potential of the cathode plate...?? i mean if it is equal, the there would be no potential difference between the plate and currrent flow should stop...and the electron flow would stop..
 
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The Potential you need has to be negative enough with respect to the photo-electrode to repel even the fasted electrons. That means it has to be lower than the plate potential. If the potentials are equal (your suggestion) then electrons will find themselves on the 'catcher' and they will not return across the gap but find their way round the circuit because that's the 'easiest path'.
The Kinetic Energy from the photo electrons will actually be dissipated in the resistance of the connecting wire and components.
 
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ohh thanks for helping...
 
Initially, I was going to leave it as it is, since the OP appears to "understand" the answer that was given. However, I still think that what was written is rather unclear, and a couple of important points might have been missed here.

1. The cathode is usually grounded, so it is at zero potential. So making the anode to be at the same potential as the cathode means that everything is grounded.

2. The photoelectrons are "born" with a range of kinetic energy, i.e. they are already moving! If everything is at the same potential, there will be nothing to stop these electrons from reaching all parts of the system, including the anode, and thus, registering a current. So how would this be the "stopping potential"?

Zz.
 
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Thanks for your explanation ZapperZ.

I have another question..if I apply stopping potential..the electrons emitted from cathode stops "reaching" anode...but still they are generating from cathode...right...?? So,what happens...??
They are just emitted from the surface and become motionless ??
 
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Molar said:
Thanks for your explanation ZapperZ.

I have another question..if I apply stopping potential..the electrons emitted from cathode stops "reaching" anode...but still they are generating from cathode...right...?? So,what happens...??
They are just emitted from the surface and become motionless ??

They get pushed away from the anode. Where they end up depends on their initial directions and energies. They don't become motionless. Remember, there is an external field due to the anode being at a certain potential. So these electrons can't just sit there.

Zz.
 
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If you put an insulated plate next to the photoelectron emitter, the photoelectrons will accumulate on that plate, making its potential more and more negative (wrt the emitter) when the potential reaches a 'stopping potential', electrons will not hit the plate (repelled) and may just return to the emitter plate. that's ok but there is no way of telling when this condition has been reached and measuring a zero current using a variable bias potential will tell you when it has.
Same 'automatic' thing happens for an insulated photo electron emitter. Electrons are kicked off, leaving the emitter with a positive potential. Eventually, an equilibrium condition will be reached when the space charge, around the emitter reaches a maximum value.
 
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sophiecentaur said:
Eventually, an equilibrium condition will be reached when the space charge, around the emitter reaches a maximum value.

As long as the incident photons have the sufficient energy,electron will come out. Now they cannot go near the insulated plate. So the electrons come back to the emitter (positive potetial). That means both emission and recombination goes on simultaneouly at a constant rate and thus space charge reaches the maximum value...?
 
Molar said:
As long as the incident photons have the sufficient energy,electron will come out. Now they cannot go near the insulated plate. So the electrons come back to the emitter (positive potetial). That means both emission and recombination goes on simultaneouly at a constant rate and thus space charge reaches the maximum value...?

I've done photoemission experiments on insulators, and so have others if one judges by the number of papers published on this. There are ways to minimize such charging effects, depending on the nature of the insulator. I suggest you not follow or extend this line of discussion. The introduction of insulators in all of this is an unnecessary complication, and from what I can tell already, it is distracting you from understanding the straightfoward physics in a standard and simple photoelectric effect experiment.

Zz.
 
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Molar said:
As long as the incident photons have the sufficient energy,electron will come out. Now they cannot go near the insulated plate. So the electrons come back to the emitter (positive potetial). That means both emission and recombination goes on simultaneouly at a constant rate and thus space charge reaches the maximum value...?
Yes. That will be the equilibrium state.
 
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