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Answer #2

To see why, apply Kirchoff's loop rule. With the switch opened we have:

IR + L dI/dt = 0

or dI/dt = -IR/L

Solving this for current gives I(t) = Io e-t/t

The potential difference across the resistor has a similar form:

DVR = e e-t/t

The potential difference across the inductor is negative because it's acting like a battery hooked up in the opposite direction:

DVL = -e e-t/t

Once again, the graph of current as a function of time in the RL circuit has the same form as the graph of the capacitor voltage as a function of time in the discharging RC circuit, while the graph of the inductor voltage as a function of time in the RL circuit has the same form as the graph of current vs. time in the discharging RC circuit.

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