Capacitor Exercise (part 2)

A non-relativistic charged particle flies through the electric field of a cylindrical capacitor and gets into a uniform transverse magnetic field with induction B B as shown in figure. In the capacitor the particle moves along the arc of a circle, in the magnetic field, along a semicircle of radius r r . The potential applied to the capacitor is equal to V V , the radii of the electrodes are equal to a a and b b with a < b a<b . Find the specific charge q m \frac{q}{m} of the particle. q m = h V i c r d B e l n ( b f a g ) \frac{q}{m}=\frac{hV^{i}}{cr^{d}B^{e}ln(\frac{b^{f}}{a^{g}})} Find h + i + c + d + e + f + g = ? h+i+c+d+e+f+g=?
This problem is not original


The answer is 9.

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1 solution

Motion through the capacitor :

q V r ln ( b a ) = m u 2 r u 2 = q V m ln ( b a ) \dfrac{qV}{r\ln (\frac{b}{a})}=\dfrac{mu^2}{r}\implies u^2=\dfrac{qV}{m\ln (\frac{b}{a})} .

Motion through the magnetic field :

B q u = m u 2 R u = B q R m Bqu =\dfrac{mu^2}{R}\implies u=\dfrac{BqR}{m} .

So, q V m ln ( b a ) = B 2 q 2 R 2 m 2 q m = V B 2 R 2 ln ( b a ) \dfrac{qV}{m\ln (\frac{b}{a})}=\dfrac{B^2q^2R^2}{m^2}\implies \dfrac{q}{m}=\dfrac{V}{B^2R^2\ln (\frac{b}{a})} .

Hence the required sum is 1 + 1 + 1 + 2 + 2 + 1 + 1 = 9 1+1+1+2+2+1+1=\boxed 9 .

@Alak Bhattacharya now it is clearly stated, so please delete the problem

A Former Brilliant Member - 1 year, 1 month ago

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