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So, I understand that the intensity should be the only factor increasing the current as the answer to a similar question (Photoelectric Effect - Dependence of current on frequency) wisely explained, assuming that the Cathode, from which the electrons are leaving, is kept at a lover or same potential as the anode. If it was the opposite case However, as far as I know and the simulator shows, current would depend on the voltage because not every released electron would reach the anode because of the braking electric field.

My actual question however is: Can anybody explain me why does the PhET simulator (http://phet.colorado.edu/en/simulation/photoelectric) show that current does depend on frequency, but not seemingly linearly. The current on a constant intensity seems to reach its peak at the wavelength of 196nm corresponding the frequency of 1,53 x 10^15 Hz, which is UV.

I even made some rough measurements on the amount of electrons leaving the cathode in 20 second interval. My result was: At the wavelength of 196nm 21 electrons were released. At 345nm only 13 electrons were released.

So my point here is that we are told that the current doesn't depend on the frequency, furthermore the amount of electrons released from cathode doesn't depend on frequency. Is there something wrong in my measurements or does the simulator take something into account that a basic school book doesn't tell?

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Although the intensity may be the same the lower wavelength photons have more energy and so can give more energy to an electron.
An electron with more energy has more chance of escaping from the metal.
So although more electrons per second may be given energy by the higher wavelength photons their chances of escape are less that the fewer electrons per second given by the lower wavelength photons.
Overall more electrons per second, which have acquired a greater amount of energy, escape.
So the saturation current does depend on the wavelength of the incident radiation but in a non-linear way.

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Update

There are some tips for teachers available but if you cannot register here are the relevant three paragraphs:

  • Electrons are emitted with a range of energies because photons can eject electrons with a range of binding energies. If more of a photon’s energy is used to release an electron, the emitted electron will have less kinetic energy. Note that this behaviour is different from the simplified model used by some textbooks, in which all electrons are emitted with the same kinetic energy. If you want to use this simplified model, you can check the “show only highest energy electrons” option. This option does not change the graphs because current is still calculated based on all the electrons.
  • Not every photon emits an electron, even if the photons have enough energy to emit electrons. If a photon is absorbed by an electron with binding energy greater than the photon energy, the electron will not be released. Photons with higher energies are more likely to release electrons because a greater proportion of the electrons in the metal have binding energy less than the photon energy. Therefore, as you increase the frequency, the number of emitted electrons (and therefore the current) will increase until all photons are emitting electrons. Note that this behaviour is different from the simplified model used by many textbooks, in which every photon with frequency greater than the threshold frequency releases an electron, so the current is constant above the threshold frequency.

  • In the default setting, since the intensity of light is proportional to the number of photons times the frequency, if you increase the frequency while holding the intensity constant, the number of photons will decrease. Therefore, if you increase the frequency past the point where all photons are emitting electrons (see previous bullet), the number of emitted electrons (and therefore the current) will start to decrease. Note that this is different from the simplified model used by many textbooks, in which current is constant above the threshold frequency. If you want to be able to change the frequency without changing the number of photons, select “Control photon number instead of intensity” in the Options menu.

The last bullet point gives you a way of finding out for the Phet simulation the average number of electrons emitted by a photon as a function of the wavelength of the photon.

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The greater the frequency of the light the greater the amount of energy per photon. The threshold frequency has just barely enough energy per photon to eject electrons, and can only eject the electrons in the metal that have the highest amount of energy. (Imagine the electrons in a valance shell or the top of a valence band, although that's too simplistic as electrons are being given energy by the collisions of the atoms and being "excited" a bit.) The main thing is that photons with a higher frequency have more energy and therefore can eject electrons that were a little lower in energy as well. So these photons have a higher probability of ejecting electrons. It's like lowering a rope down from a window to pull people up. There's a minimum length that will work, but a longer rope can reach not only the tallest people but some of the shorter ones too. So the odds that each photon (rope) can "pull up" an electron goes up as the frequency and therefore energy per photon goes up.

In the simulation, with the intensity at 100% the number of photons emitted each second goes DOWN as the frequency increases. The intensity staying constant means the energy emitted per second is the same. So, since higher frequency photons have more energy each, then the number of photons being emitted each second must be less. If you go to Options and select "Control photon number instead of intensity" then the current won't drop when the frequency goes above ~196 nm. (It does seem to reach a maximum, though, and a higher frequency doesn't affect the current. I can only assume the "rope" is now so long that it's hitting the ground and so a longer rope isn't helping anyone.)

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