Charge to mass ratio of an electron shot through a cathode-ray oscilloscope

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SUMMARY

The charge-to-mass ratio of an electron projected through a cathode-ray oscilloscope can be derived using the equation e/m = hv^2/(ELd). The problem involves an electron with charge -e and mass m, projected at speed v in a uniform electric field directed negatively along the y-axis. The analysis shows that the displacement h of the electron when it hits the screen is influenced by the length d of the electric field and the distance L traveled after exiting the field. The derivation requires understanding of kinematics and the relationship between acceleration, velocity, and displacement.

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jordanl122
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I've been working on this problem for awhile but I just can't seem to hack it. (This is problem 76 from Serway 3rd for the first electricity chapter if you happen to have that book and want a visualization)
Given: an electron with charge, -e, and mass, m, is projected with speed v, at a right angle to a uniform electric field that is flowing in the negative y direction. The oscilloscope has length d, and after the particle exits the field it travels a length, L, and smacks a screen. It was displaced in the positive y direction to a height of h when it has hit the screen. Assuming d is much less than L in magnitude, and ignoring gravity, show the charge-to-mass ratio is given by:
e/m = hv^2/(ELd)

First, I set Ee = ma and divide through to get e/m = a/E

Solving for a in terms of L, d, and h, I know the electron is traveling with constant horizontal velocity, and it travels a distance of (L + d) in time t, or

v = (L+d)/t so t = (L+d)/v

I also know that it is accelerating in the y direction, so

h = vyt + 1/2at^2 (there is no initial y component to the velocity so...)

h = .5at^2

plugging in for t and solving for a I get...

2h/(L+d)^2/v^2 = a which simplifies to 2hv^2/(L^2+2dL+d^2) = a

I then plug it into the original ratio equation

e/m = 2hv^2/(E(L^2+2dL+d^2) which assuming d is much less than L,

e/m = 2hv^2/(E(L^2 +2dL) which is close but not the answer

If anyone can help me I would be greatly appreciative. I know I have probably made a stupid mistake somewhere, but for the life of me, I can't find it. Thank you.
 
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Realize that the electron is only accelerated during its travel across d, not d + L.

Try this: Find the impulse given to the electron, then the change in its vertical speed. Then use that to find the angle the electron is traveling when it leaves the field. (Ignore the change in height during the acceleration; assume the electron starts its straight line journey at y = 0.)
 
thanks

Thank you so much, I was killing myself over this problem
 

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