How do I solve for voltage in a phototube with multiple figures and connections?

  • Thread starter dimpledur
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In summary, the values found for figure 1 are as follows: Vc1=1.51V, Vc2=1.61V, Vc1c2=-0.1V, Vc1a1=1.51V, Vc2a2=1.61V, Vc1a2=1.51V, Va1=Va2=Va1a2=0. The potential difference between Vc1 and Vc2 in figure 1 is due to the initial voltage from the photon hitting each cathode, but eventually they reach an equilibrium potential of 1.56V. In figure 2, since Vc1 and Vc2 are not connected,
  • #1
dimpledur
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Homework Statement


yes-1.jpg




The Attempt at a Solution


What I am wondering is if I found all of the answers for figure 1, wouldn't I just be repeating those same answers for figure 2 and 3? Or is the way it arranged important?

Here are the values I found:
Vc1=1.51V
Vc2=1.61V
Vc1c2=-0.1V
Vc1a1=1.51V
Vc2a2=1.61V
Vc1a2=1.51V
Va1=Va2=Va1a2=0

Thanks for your help
 
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  • #2
all arrangements are different. In fig. 1, C1 and C2 are connected, so are at same potential, but in fig.2, this is the case with A1 and A2. In fig. 3, C1 and C2 are at same potential, and A1 and A2 are also at same potential (different from C1 and C2).
 
  • #3
How do you determine what potential they are at if they are at the same potential. For example, for figure one if Vc2=1.61 V and Vc1= 1.51V, would Vc1c2 just be an average of the two?
 
  • #4
i think you calculated wrong. Vc1 = Vc2 (should be), and Vc1c2 = 0, as Vc1c2 = Vc1 - Vc2 (potential difference).
 
  • #5
But the cathode at the bottom is struck with a different energy than the cathode at the top. Hence the difference in potentials. V=(Wf-Ephoton)V/eV
 
  • #6
So if I calculated Vc1=1.51 and Vc2=1.61 would I assume they reach the same potential in figure one so Vc1=Vc2=1.56?
 
  • #7
Ephoton - Wf = Eelectron, not V.
 
  • #8
my textbook labels the frequency with v, which is units cycles/s
 
  • #9
i am a bit unsure about Vc1 and Vc2 part, will need some time to think about it.
 
  • #10
I think I got it. For figure one, Vc1 has an initial voltage due to the energy of the photon that hits it. Additionally, Vc2 has an initial voltage due to the photon that hits it as well. However, after the initial potential difference, they reach an "equilibirum" potential of 1.56. That way Vc1c2=0, Vc1=Vc2=1.56. Also, Vc1a1=Vc2a2=Vc1a2=Vc2a1=1.56 and Va1=Va2=Va1a2=0.
 
  • #11
Perhaps for figure 2 Vc1=1.51 and Vc2=1.61, but since they are not connected they don't reach the same potential and Vc1c2=-0.1 Va1=Va2=Va1a2. Wouldn't the potentials of the anode in all the figures be zero?
 
  • #12
but as far as i know, we never take average of potentials of two points if they are connected. so i am do not agree with above.
 
  • #13
Well then I am very confused. However, wouldn't it make sense for that to occur? If there is excess charge at one point, and a conductor between two ponts, wouldn't the charge flow till eventually there was no potential difference?
 
  • #14
Suppose for a moment that both cathodes were made of the same material and that they were connected as in figure 1. Further suppose that only one source of light is involved. What would be the difference between a photon hitting c1 and then a photon hitting c2, and two photons hitting either c1 or c2?
 
  • #15
I don't really see a difference. If electrons are leaving c1 due to a single photon hitting it, more electrons from c2 would flow via the conductor so eventually both cathodes would reach the same potential. Or am I completely off?
 
  • #16
dimpledur said:
I don't really see a difference. If electrons are leaving c1 due to a single photon hitting it, more electrons from c2 would flow via the conductor so eventually both cathodes would reach the same potential. Or am I completely off?

Precisely. The two cathodes are essentially one cathode when they are connected, so the work done removing the charges by the photons is "shared". The potential is the same.
 
  • #17
One last question before I go. Is it true that all of the anodes have a potential of 0 regardless of the set up? for example, Vca=0, but I don't really see how Va1a2 would equal zero for figure two, because wouldn't the anodes have a different charge?
 
  • #18
If only the anode is connected via a wire, wouldn't they eventually have the same charge and consequently the potential on the cathodes would change?
 
  • #19
Actually, I think all the Va's will. Equal zero except for the Va1Va2 in which they're not connected. Does it make sense to say for this set up that Va1Va2=Va1c1-Va2c2
 

FAQ: How do I solve for voltage in a phototube with multiple figures and connections?

1. What is a phototube?

A phototube is a device used in scientific experiments and instruments, such as photometers and spectrophotometers, to measure the intensity of light. It consists of a vacuum tube containing electrodes and a photosensitive material that produces an electric current when exposed to light.

2. How does a phototube work?

A phototube works by converting light energy into electrical energy. When light enters the tube, it strikes the photosensitive material, causing it to emit electrons. The electrodes within the tube then collect these electrons, creating an electric current. The amount of current produced is proportional to the intensity of the light.

3. What is the voltage range of a phototube?

The voltage range of a phototube can vary, but most commonly it is between 100 to 1000 volts. The specific voltage used depends on the type of phototube and the intensity of the light being measured.

4. What are some applications of phototubes?

Phototubes have a wide range of applications in scientific research and technology. They are commonly used in photometers and spectrophotometers to measure the intensity of light in various experiments. They are also used in astronomy to detect and study light from distant objects and in photography to capture images.

5. Can phototubes be used to measure other forms of radiation?

Yes, phototubes can also be used to measure other forms of radiation, such as X-rays and gamma rays. In these cases, the photosensitive material within the tube is replaced with a material that is sensitive to the specific type of radiation being measured. The basic principle remains the same, with the radiation causing the emission of electrons and the electrodes collecting them to create an electric current.

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