Coldie said:
Our Physics review sheet includes two questions involving "accelerating voltage", "deflecting voltage", and "screen deflection", which are involved with Cathode Ray Tubes. The chapter on this in the book basically outlined what one was and how it worked, but it did not make use of any of these terms and I'm at a loss at how to solve the problems.
One of them is:
An accelerating voltage of 750 V produces a screen deflection of 4.2 cm on a CRT. If the deflecting voltage is kept constant but the accelerating voltage is increased to 1000 V, what will the deflection become?
There appear to be two voltages to keep track of, and so none of my equations seem to apply here. Would someone please explain to me what to do?
Much of the intent seems almost clear to me. The accelerating voltage determines the velocity of the electrons.
Most CRT's use magnetic deflection, but because the textook talks about "deflecting voltage", I'd assume that there is some constant E-fiield that deflects the electrons.
The deflection distance is just how far the electrons move on the scrreen due to the deflection voltage, i.e. you measure the distance the spot on the screen moves when you remove the deflection voltage.
Now, when you boost the accelerating voltage, you speed up the electrons, so they deflect less.
The problem is that we don't know the region of space in which the E-fields are located that cause the deflection. Two different approximations come to mind
1) The E-field is contant everywhere - this leads to a quadratic dependence of deflection on transit time. (Transit time is inversely proportional to velocity).
2) The E-field is only present during the first part of the flight. The lateral velocity imparted will be inversely proportional to the time it takes to traverse the electrodes. If we ignore the deflection that occurs during the acutal transit of the electrodes and assume that it's small, the deflection will be proportional to the lateral velocity the electron has when it leaves the electrode region (we multiply the lateral velocity times the distance the electron travels after it leaves the deflection area.)
I'd guess they problably want you to use case 2, and igonre the quadratic nature of the deflection that happens when th electron is actually moving between the charged deflecting plates. But this is just a guess.