Accelerating electrons in a cathode ray tube

In summary, the electron gun in a CRT tube allows the electrons to be accelerated to a high energy before they are allowed to strike the phosphor screen.
  • #1
snath_98
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I have a question which has intrigued me for quite some time. If the electrons are accelerated using a potential difference in a cathode ray tube, the electrons should get accelerated till the time they reach the anode only. Once they cross over (ie. move to the other side of the anode), they should begin to slow down, now being attracted by the anode. Hence, on the whole, I suppose there should be no net gain in energy for the electrons, unless the anode is placed very close to the front glass screen of the CRT, in which case there's not enough time available to the electron to be slowed down appreciably. This is a conundrum for me. Can anyone explain this?
Thanks
 
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  • #2
greetings
Welcome to PF :)

snath_98 said:
Once they cross over (ie. move to the other side of the anode), they should begin to slow down, now being attracted by the anode

what do you mean by that ?

Do you understand how a CRT tube works and what/where the anode in a CRT is ?Dave
 
  • #3
davenn said:
greetings
Welcome to PF :)
what do you mean by that ?

Do you understand how a CRT tube works and what/where the anode in a CRT is ?Dave
Yes, I do. Please refer to the diagram here: http://design.osu.edu/carlson/history/images/crt.gif
 
  • #4
snath_98 said:
Yes, I do. Please refer to the diagram here: http://design.osu.edu/carlson/history/images/crt.gif
Cross over to the other side means go through the anode. Coming from the left they are naturally attracted/accelerated by the positive anode. However, once they go through the anode in the diagram, they should begin to be slowed down (the same attraction forces still operate).
 
  • #5
snath_98 said:
Cross over to the other side means go through the anode. Coming from the left they are naturally attracted/accelerated by the positive anode.

OK ... you do have a misunderstanding of how a CRT works

neither of those anodes are the main anode for the tube
The main High Voltage anode isn't shown in that pic as it is the front of the screen
depending on the size of the screen, that HT voltage will vary ... Small Oscilloscopes may be ~ 1-5 kV
the old large 26 inch colour TV CRT's had up to 25 kV on them

This HT voltage is what allows the to continue on to the screen and strike the phosphor dots

( There may be CRT's that don't have an HT voltage on the front, instead use some other method, but I'm not personally aware of them)

The Crookes tube is a bit of a really basic version ... but not really a CRT as we know. It only showed one thing on the front of the display
http://en.wikipedia.org/wiki/Crookes_tube
cheers
Dave
 
  • #6
I suppose my question is not clear to you. To put it in a simpler manner. if I have electrons (low energy), and wish to accelerate them before allowing the high energy electrons to strike something, how do I do it?
 
  • #7
snath_98 said:
Once they cross over (ie. move to the other side of the anode), they should begin to slow down, now being attracted by the anode
Your point is absolutely fine, in principle. In an electron gun, the electrons are attracted by the 'First' Anode (Which is part of the electron gun assembly, initially and there is a strong field between them (Many Volts, small distance). The ballistics of the situation could take those electrons far beyond the first Anode, before they slow down and head back to it, if that Anode Potential were all that counted. But there is also a potential difference between Anode and Screen (that's also an anode), so the electrons carry on towards the (highly positive) back of the screen. In practice, the whole of the Electron source (back end) is kept at a 'safe' voltage so that you can supply the grids and deflection coils / plates with reasonable voltages from video amplifiers etc. That big fat wire that goes to the front, side of the tube, carries the EHT from the diode stack and is the hairiest part of the setup.

The reason for having an electron gun at all is to produce the narrow, steerable electron beam which, once formed, will carry on to the screen phosphors. The energy from this acceleration is what produces the light output from the screen. A Crooke's tube has no focussed beam and no electron gun. You can make a crook's tube work with the sort of vacuum that you can get with a hand cranked school vacuum pump. A round bottomed flask with an anode, fed through a sealed hole in the bottom is not hard to make and to get results with. But be careful with kV power supplies!
 
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  • #8
snath_98 said:
I suppose my question is not clear to you. To put it in a simpler manner. if I have electrons (low energy), and wish to accelerate them before allowing the high energy electrons to strike something, how do I do it?

You haven't asked anything different, the answer remains the same :)
As already discussed, you use a high voltage positive plate/screen etc to attract them

Dave
 
  • #9
davenn said:
As already discussed, you use a high voltage positive plate/screen etc to attract them

Dave

If the object you are trying to bombard is a conductor, you put it at a high potential. If it is not, then you can put an anode behind it or, even better, use an electron gun to focus your beam at it. Your original point about the electrons 'going past' an anode and still having energy, is a valid one.
What actually do you (the OP) want to do with these electrons?

PS there can be a problem with an insulator charging up and then repelling electrons from the beam.
 
  • #10
snath_98 said:
Cross over to the other side means go through the anode. Coming from the left they are naturally attracted/accelerated by the positive anode. However, once they go through the anode in the diagram, they should begin to be slowed down (the same attraction forces still operate).

Usually the electrodes are shaped to focus the fields with the anode at the effective ground potential of the circuit.
http://www4.nau.edu/microanalysis/microprobe-sem/images\Electron_Gun.jpg
 
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  • #11
nsaspook said:
Usually the electrodes are shaped to focus the fields with the anode at the effective ground potential of the circuit.
http://www4.nau.edu/microanalysis/microprobe-sem/images\Electron_Gun.jpg
It will depend upon what sort of CRT you are dealing with. A TV CRT certainly needs the Grids to be at around Ground potential so that relatively low video voltage drivers can be used. In any case, the accelerating potential, to produce high energy will have to be at the 'front end (call it a second anode, because that is its function) because it is not convenient to produce modulating signals, sat down at lots of -kV. The absolute potential has no relevance except for practicality and it is by far the easiest system to have the EHT supply taken to the front of the tube, away from all the other electronics.
That diagram is of the electron gun section and the supply is only 'high voltage' and not EHT. It doesn't seem to include the focussing electrodes, which are needed for spot forming.
 
  • #12
sophiecentaur said:
It will depend upon what sort of CRT you are dealing with. A TV CRT certainly needs the Grids to be at around Ground potential so that relatively low video voltage drivers can be used. In any case, the accelerating potential, to produce high energy will have to be at the 'front end (call it a second anode, because that is its function) because it is not convenient to produce modulating signals, sat down at lots of -kV. The absolute potential has no relevance except for practicality and it is by far the easiest system to have the EHT supply taken to the front of the tube, away from all the other electronics.
That diagram is of the electron gun section and the supply is only 'high voltage' and not EHT. It doesn't seem to include the focussing electrodes, which are needed for spot forming.

Correct. I was just trying to show that the potentials and fields would be focused to accelerate the electrons past the (at effective ground potential IRT the electron) anode but after the anode the potentials and fields from that circuit would be much less and not slow the electron as it moved into space past it.
 
  • #13
snath_98 said:
I have a question which has intrigued me for quite some time. If the electrons are accelerated using a potential difference in a cathode ray tube, the electrons should get accelerated till the time they reach the anode only. Once they cross over (ie. move to the other side of the anode), they should begin to slow down, now being attracted by the anode. Hence, on the whole, I suppose there should be no net gain in energy for the electrons, unless the anode is placed very close to the front glass screen of the CRT, in which case there's not enough time available to the electron to be slowed down appreciably. This is a conundrum for me. Can anyone explain this?
Thanks

The acceleration of the electrons is caused, not by the potential of the first anode, but by the potential gradient between anode and cathode. Once the electrons pas the anode, the potential gradient is much reduced. There may be a second anode to help.
 
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1. What is a cathode ray tube?

A cathode ray tube (CRT) is a specialized vacuum tube used to create images on screens for televisions and computer monitors. It works by accelerating electrons to create a beam of electrons that can be directed onto a phosphorescent surface to produce images.

2. How are electrons accelerated in a cathode ray tube?

Electrons are accelerated in a cathode ray tube by using a high voltage electrical field. This field is created by applying a strong negative charge to the cathode (negative electrode) and a positive charge to the anode (positive electrode). This creates a potential difference, causing the electrons to accelerate towards the anode.

3. What is the purpose of accelerating electrons in a cathode ray tube?

The purpose of accelerating electrons in a cathode ray tube is to create a focused beam of electrons that can be directed onto a screen to produce images. The speed and intensity of the electrons can be controlled to create different shades and colors on the screen.

4. How is the direction of the electron beam controlled in a cathode ray tube?

The direction of the electron beam is controlled by using a series of electromagnets. These magnets can be adjusted to change the direction of the beam, allowing for precise control over the image displayed on the screen.

5. What are some common applications of cathode ray tubes?

Cathode ray tubes were commonly used in televisions and computer monitors before the advent of LCD and LED screens. They are also used in oscilloscopes, which are instruments used to measure and display electronic signals. Some older medical imaging equipment, such as X-ray machines, also use cathode ray tubes.

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