Calculate Charge to Mass Ratio from J.J. Thomson's Experiment

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Homework Help Overview

The discussion revolves around calculating the charge to mass ratio of charged particles in a setup inspired by J. J. Thomson's experiment. The problem involves charged particles moving through a magnetic field and the introduction of an electric field to alter their path.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning, Assumption checking

Approaches and Questions Raised

  • Participants explore various equations related to the motion of charged particles in magnetic and electric fields. There is discussion about the role of kinetic energy and whether it can be applied in this context. Some participants question the use of the distance between the capacitor plates in the calculations.

Discussion Status

There is an ongoing exploration of different interpretations of the problem. Some participants have provided alternative approaches to calculating the charge to mass ratio, while others have pointed out potential oversights in the original calculations. Guidance has been offered regarding the use of the distance between the plates and its relevance to the problem.

Contextual Notes

Participants note that the charge is traveling along an equipotential and discuss the implications of this on the forces acting on the particles. There is also mention of the specific values given in the problem, such as the voltage and the separation distance between the plates.

Linday12
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Homework Statement


In an experiment similar to J. J. Thomson's, charged particles are observed to travel through a magnetic field of 0.040 T with a radius of curvature of 0.20 m. The path of these particles is made straight again when an electric field is introduced by two parallel plates.

V=200 V
distance between plates=10cm=0.10m
radius=0.20m
B=0.040T (assuming its parallel)


Homework Equations


r=mv/qB
ek=1/2(mv^2)=qV
v=[tex]\sqrt{2qV/m}[/tex]
r[tex]^{2}[/tex]=m2V/qB[tex]^{2}[/tex]
q/m=2V/r[tex]^{2}[/tex]B[tex]^{2}[/tex]

The Attempt at a Solution


=2(200V)/(0.20m)[tex]^{2}[/tex](0.040T)[tex]^{2}[/tex]
=6.3 x 10^6 C/kg

Does this look to be correct? I wasn't sure if I could do it all at once if the force was exerted at two different times (although it seems to make sense).

Thanks.
 
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r=mv/qB
ek=1/2(mv^2)=qV
v=[tex]\sqrt{2qV/m}[/tex]
r[tex]^{2}[/tex]=m2V/qB[tex]^{2}[/tex]
q/m=2V/r[tex]^{2}[/tex]B[tex]^{2}[/tex]
I don't think you can use kinetic energy here because it seems that the charge is traveling along an equipotential, i.e. not in the direction of the E field of the capacitor plates.

In the first case you found

mv2/R = qv*B

Then the E-Field is applied so there is no net force. This results in

qv*B = q*E

where E = V/d

v = E / B = V/(d*B)

If you apply this result to the first equation you should arrive at

q/m = V/(B2*R*d)

In this case since it happens that d = R it calculates to half of your result ...

q/m = V/(B*R)2
 
Last edited:
In the relevant equation, the ek is the kinetic energy acquired be the charged particle before it enters the magnetic field. In the problem the given voltage is the voltage across the parallel plates which deflects the the beam of charged particles. In the calculation you have not used the distance between the plates which is given in the problem.
 
Wow, I can't believe I didn't notice that I hadn't used the plate separation. The problem makes complete sense now. Thank you both for your help, it was exactly what I needed!
 

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