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Consider a toroid with rectangular cross section, of inner radius a, outer radius be and height h, carrying n number of turns. Then the self-inductance of the toroidal coil when current I passing through the toroid is |
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Answer» `(mu_(0)n^(2)h)/(2pi)In((b)/(a))` Magnetic field inside a rectangular toroid is given by `B=(mu_(0)nI)/(2pir)""......(i)` usind the INFINITESIMAL cross-sectinoal area element. `dx=hdr` `:.` Flux passing through the cross-section of toroid. `phi=intB.dx=int_(a)^(b)(mu_(0)nI)/(2pir).(hdr)` `phi=(mu_(0)nIh)/(2pi)int_(a)^(b)(1)/(r)dr` `impliesphi=(mu_(0)nhI)/(2pi)[logr]_(a)^(b)` `impliesphi=(mu_(0)nhI)/(2pi)(logb-loga)` `phi=(mu_(0)nhI)/(2pi)In((b)/(a))` Now, self inductance of rectangular toroid, `L=(nphi)/(I)` PUTTING the value of `phi` we get `L=(mu^(2)nh)/(2pi)In((b)/(a))` |
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