single circular loop of wire , radius = r , with a resistance , R , sits above a series of moving magnets . The magnets pass underneath the stationary loop of wire creating a periodic magnetic field given by the function : B=B0 (sin( omega t))2 B0 is the maximum magnetic field , and w is the angular frequency . Derive the function for induced current in the circular loop of wire as a function of time
single circular loop of wire , radius = r , with a resistance , R , sits above a series of moving magnets . The magnets pass underneath the stationary loop of wire creating a periodic magnetic field given by the function : B=B0 (sin( omega t))2 B0 is the maximum magnetic field , and w is the angular frequency . Derive the function for induced current in the circular loop of wire as a function of time
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A single circular loop of wire , radius = r , with a resistance , R , sits above a series of moving magnets . The magnets pass underneath the stationary loop of wire creating a periodic magnetic field given by the function : B=B0 (sin( omega t))2 B0 is the maximum magnetic field , and w is the angular frequency . Derive the function for induced current in the circular loop of wire as a function of time
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