Showing Faraday's Law with an Oscilloscope
Showing Faraday's Law with an Oscilloscope
According to Faraday's law of electromagnetic induction, an electromotive force (emf) is induced in a conducting coil by a time-varying magnetic flux through the coil. This can be written , where the magnetic flux through the coil is given by . For a circular search coil of radius wound with turns of wire, , where is the angle of the coil to the magnetic induction , which is assumed uniform over its cross section, although variable over time. The function generator varies the voltage through the Helmholtz coils, which produces a time-dependent magnetic induction mirroring the signal profile. The induced signal is then proportional to the time derivative of the input signal, thus depending linearly on both its amplitude and frequency. Both the function generator and oscilloscope show stroboscopic plots of voltage versus time. The dual-trace oscilloscope can show both signals simultaneously, and we have taken the liberty of coloring the search-coil signal red.
ℰ=-
Φ
t
Φ=∫B·dσ
R
N
Φ=πNBcosθ
2
R
θ
B
B(t)