Solution:
The electric field in a discharging capacitor drops as \(E = E_0 e^{-t/RC}\). Given \(E = E_0/3\), we have \(RC = \frac{t}{\ln 3}\). Solving for \(R = \frac{4.4 \times 10^{-6}}{2.0 \times 10^{-6} \times 1.1} = 2~\Omega\).
The electric field in a discharging capacitor drops as \(E = E_0 e^{-t/RC}\). Given \(E = E_0/3\), we have \(RC = \frac{t}{\ln 3}\). Solving for \(R = \frac{4.4 \times 10^{-6}}{2.0 \times 10^{-6} \times 1.1} = 2~\Omega\).
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