Angle of Deflection for a Moving Charge Passing a Fixed Charge

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Homework Help Overview

The problem involves a charged particle moving along the x-axis and its interaction with a fixed charge, focusing on the angle of deflection as the moving charge passes the stationary charge. The context is within the realm of electrostatics and dynamics.

Discussion Character

  • Exploratory, Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • Participants discuss the derivation of the electric field and its implications for the motion of the charged particle. There are attempts to relate mass to the electric field and force, with some questioning the correctness of the calculations and assumptions made.

Discussion Status

The discussion is ongoing, with participants providing insights and questioning each other's reasoning. Some guidance has been offered regarding the need for integrals in the calculations, and there is an exploration of the implications of using physical units in the equations.

Contextual Notes

There are indications of confusion regarding the application of Gauss's law and the treatment of the electric field as non-constant. Participants are also addressing the need for consistency in units across the equations being discussed.

Graham1
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Homework Statement



A Particle of mass m and chargeq oves at high speed along the x axis. It is initially near x=-infinity and it ends up near x=+infinity. A second charge Q is fixed at the point x=0, y=-d. As the moving charge passes the stationary chrge, its x component o velocity does not change appreciably, but it acquires a small velocity in the y direction. Determine the angle angle through which the moving charge is deflected. suggestion: The integral you encounter in determining v_y can be evaluated by applying Gauss's law to a long cylinder of radius D, centred on the stationary charge.


Homework Equations



[tex]\Phi[/tex] = ∮EdA


The Attempt at a Solution



So Far, I have managed to get to E=Q/2[tex]\pi[/tex]md([tex]\epsilon[/tex]_0)
and ended up with a= Qq/(2[tex]\pi[/tex]md([tex]\epsilon[/tex]_0)
by using electric force and F=ma equations

I know the answer I should get is [tex]\Theta[/tex]=Qq/(2[tex]\pi[/tex]md([tex]\epsilon[/tex]_0}[/tex)v[tex]^{2}[/tex]

can anybody help me with the method between these two points, or correct me if my method is wrong?
 
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How did you manage to bring mass into the formula for electric field?
Anyway, your calculation of electric field is wrong, since E is not constant. What you need in this exercise is an integral of Er(radial component of electric field) over x, which can be easily obtained from Gauss law (since the same integral also appears in Gauss law).
 
getting mass into the equation was easy enough - use the field E to get a force F.
then simply take F=ma and rearrange
 
Physical units are a usefull thing. Especially if they are the same on both sides of the equation.
 

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