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Physics 8 Online
OpenStudy (anonymous):

See attachment below

OpenStudy (anonymous):

OpenStudy (nincompoop):

this is a nice problem. do you know how to start?

OpenStudy (anonymous):

In equilibrium, the cord is stretched in the direction of resultant force of G =mg and F = q E, where E stands for the electric field strength of the ring on the axis in distance x from the plane of the ring

OpenStudy (anonymous):

how about you @nincompoop ??

OpenStudy (anonymous):

|dw:1429083397346:dw|

OpenStudy (anonymous):

Using the triangle similarity, one can write \[\frac{ x }{ R } = \frac{ E q }{ mg }\]

OpenStudy (anonymous):

For the calculation of the electric field strength let us divide the ring to n identical parts, so as every part carries the charge \(Q/n\)

OpenStudy (anonymous):

The electric field strength magnitude of one part of the ring is given by \[\Delta E = \frac{ Q }{ 4 \pi \epsilon_0 l^2 n}\]

OpenStudy (michele_laino):

Hint: here, for symmetry reason, the electric force is directed along the z-axis, and the magnitude of its x-component, is: \[\Large {F_x} = \frac{1}{{4\pi {\varepsilon _0}}}\frac{{Qq}}{{{l^3}}}\sqrt {{l^2} - {R^2}} \]

OpenStudy (michele_laino):

now in order to find l, we have to reire that the subsequent condition is checked: \[\Large mg = {F_x}\tan \theta \] where \[\theta \] is sulike in the figure below: |dw:1429096060848:dw|

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