A square coil is placed in a magnetic field. The coil is composed of 450 turns of wire. As the coil is wound around, the magnetic field changes at a constant tempo from 0,2 T to 0,42 T in 6 x 10-2 seconds. The induced emf is – 15 V.
Faraday's law of induction can be expressed as:
"\\epsilon=-N\\dfrac{d\\Phi_B}{dt}=-NA\\dfrac{dB}{dt}=-Nl^2\\dfrac{dB}{dt}"
where "\\epsilon" is the induced emf, N is the number of turns for the coil, and since it is a squared coil we also have A=l2 (length of a side to the square), and dB/dt is the rate of change for the magnetic field on the coil.
For the first par, we define and substitute for "\\frac{d\\Phi_B}{dt}" :
"\\dfrac{d\\Phi_B}{dt}=-\\dfrac{\\epsilon}{N}=-(\\dfrac{-15\\,V}{450\\,turns})=(\\dfrac{1\\,V}{30})=0.0\\overline{3}\\frac{Wb}{s}"
After that, we use again the definition for Faraday's law and we find the square length l:
"\\epsilon=-Nl^2\\dfrac{dB}{dt} \\iff l= \\sqrt{\\dfrac{-\\epsilon}{N\\dfrac{dB}{dt}}}\n\\\\ \\implies l= \\sqrt{\\dfrac{-(-15\\frac{Wb}{s})}{(450)\\dfrac{(0.42-0.20)T}{6\\times10^{-2}s}}}\n\\\\ l=\\sqrt{\\dfrac{(15\\,m^2)}{(450)\\dfrac{(0.42-0.20)}{6\\times10^{-2}}}}=0.0953\\,m"
In conclusion, we find that the change in magnetic flux in the coil "\\dfrac{d\\Phi_B}{dt}=0.0\\overline{3}\\,\\cfrac{Wb}{s}", and the length of the side of the coil "l=0.0953\\,m=9.53\\,{cm}".
Reference:
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