An infinitely long cylinder of radius R has its axis along z-axis. It has a uniform volume charge density and it is rotating with constant angular velocity. Find the magnetic field produced by it everywhere.
Infinite long cylinder
∫Bo.dl=μ0Σi\smallint B_o.dl =\mu_0\Sigma i∫Bo.dl=μ0Σi
Bo=μoI2πrB_o=\frac{\mu_oI}{2\pi r}Bo=2πrμoI
I=wq2π,q=ρvI=\frac{wq}{2 \pi},q=\rho vI=2πwq,q=ρv
I=ρvw2πI=\frac{\rho v w}{2 \pi}I=2πρvw
B0=μ02πr×ρvw2π=μ04π2rρvwB_0=\frac{\mu_0 }{2 \pi r}\times \frac{\rho vw}{2 \pi}=\frac{\mu_0 }{4\pi ^2r}\rho vwB0=2πrμ0×2πρvw=4π2rμ0ρvw
Similarly surface r=R
Bs=μ02πR×ρvw2π=μ04π2RρvwB_s=\frac{\mu_0 }{2 \pi R}\times \frac{\rho vw}{2 \pi}=\frac{\mu_0 }{4\pi ^2R}\rho vwBs=2πRμ0×2πρvw=4π2Rμ0ρvw
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