# Faraday's Application on a Magnetic Dipole

Consider a closed loop wire with current flowing through it:

Consider along the wire a battery $$V$$, a resistance $$R$$ and a capacitor $$C$$.

We know the integral form of Faraday's law:

$$\oint\limits_{\partial S} \vec E\cdot d\vec l = -\frac {d\Phi_B}{dt}=-\frac d {dt} \int\limits_S \vec B\cdot d\vec A$$

Because of the capacitor, the current through the wire will exponentially decay, therefore the magnetic field $$B$$ will also decay, therefore the right side of Faraday's law won't be 0.

However, in his lecture https://www.youtube.com/watch?v=6w3SzI_s5Sg&list=PLyQSN7X0ro2314mKyUiOILaOC2hk6Pc3j&index=26 at 5.15 Walter Lewin says that $$\oint\vec E\cdot d\vec l=0$$

What am I doing wrong?

At 1:26 Lewin assumes that it is an $$RC$$ circuit, in other words he ignores any and all magnetic effects. Since the subject is "lumped" circuit theory, when speaking of magnetic effects he would have had to include in it some inductor, but he confined the problem to an $$R$$ and a $$C$$ and that is why he could write $$\oint \mathbf E \cdot d{\ell}=0$$. The magnetic moment of a closed loop of area $$A$$ is $$\approx IA$$ that usually carries quite small magnetic energy when compared to normal size capacitors and their electric energy. As you increase the local number of kinks, loops thereby making an inductor, the situation changes.