Electromagnetism - particle moving in magnetic field

  • #51


v(t)=\frac{D(t)}{r} where D(t) is some polynomial in t?
 
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  • #52


If the radial part is zero, doesn't that mean \frac{mv^2-Bvqr}{qr}=0...solve that for v
 
  • #53


refer to the feyman lectures on physics Vol 2 chapter17-3
 
  • #54


for a non trivial solution v(t)=\frac{B(r,t)q^2r^2}{m}

i still don't really see what to do next though?
 
  • #55


latentcorpse said:
for a non trivial solution v(t)=\frac{B(r,t)q^2r^2}{m}

i still don't really see what to do next though?

First, check your algebra because this result is a little off...second calculate dv/dt and hence find the tangential component of E...then check to see if E satisfies Gauss' Law (use the differential form) and Faraday's law (use the integral form).
 
  • #56


v(t)=\frac{B(r,t)qr}{m}

\Rightarrow \frac{d v(t)}{dt}=\frac{qr}{m} \frac{\partial{B(r,t)}}{\partial{t}}

therefore the tangential component of E is E_{\phi}=r\frac{\partial{B(r,t)}}{\partial{t}}


shall i just take a gaussian pillbox to test both Gauss and Faraday?
 
  • #57


latentcorpse said:
shall i just take a gaussian pillbox to test both Gauss and Faraday?

Why use the integral form of Gauss' law? Since you now know E (or at least have made a guess at what E is), just take the divergence of it.

And Faraday's law requires a loop, not a surface.
 
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