B Why does an inductor discharge?

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An inductor discharges when connected to a capacitor due to the relationship between current and magnetic fields. When current flows through the inductor, it creates a magnetic field, storing energy as described by E = ½·L·i². Upon connecting to a capacitor, the inductor begins to transfer energy, charging the capacitor while the inductor current decreases. This process creates an oscillation of energy between the inductor and capacitor, described by harmonic motion equations. The interaction continues until the energy is fully exchanged, illustrating the dynamic behavior of inductors and capacitors in an electrical circuit.
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A capacitor will discharge because once a path is created there is a potential difference $V=Q/C$. But for an inductor it's $L\frac{di}{dt}$. Why would an inductor want to discharge once you connect it to a capacitor?
 
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If there was no current flowing through the inductor, then there is no energy stored, and no magnetic field.
E = ½·L·i² ;

If a current is flowing through the inductor when it is connected to a zero volt capacitor, the current will begin to charge the capacitor.
Q = I·t ; v = Q / C ; E = ½·C·v² ;

As the capacitor voltage increases, the inductor voltage will also increase, that will reduce the inductor current, until it stops, reverses, and repeats, circulating the energy between L and C.
v = L·di/dt ;
 
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Just write down the equation from Kirchhoff's rule:
$$L \dot{i}+Q/C=0$$
Since ##i=\dot{Q}## this means
$$L \ddot{Q}+Q/C=0$$
The general solution of this "harmonic-oscillator equation of motion" is
$$Q(t)=A \cos(\omega t) + B \sin(\omega t) \quad \text{with} \quad \omega=\sqrt{\frac{1}{LC}}$$
and
$$i(t)=-A\omega \sin(\omega t) + B \omega \cos(\omega t).$$
For ##Q(0)=Q_0## and ##i(0)=0##, i.e., having some charge on the capacitor and then at ##t=0## connect it to the coil, then you get ##A=Q_0## and ##B=0##. So the final solution reads
$$Q(t)=Q_0 \cos(\omega t), \quad i(t)=-Q_0 \omega \sin(\omega t).$$
 
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