Step 1: Model the discharge
When the plates are shorted by a wire of resistance \(R\), the capacitor (capacitance \(C=1.5\,\mu\text{F}\)) discharges through \(R\) with time constant \(\tau=RC\). The voltage (and hence the electric field between the plates) decays exponentially:
\[
E(t)=E_0\,e^{-t/(RC)}.
\]
Given that the electric field drops to one third in \(t=6.6\,\mu\text{s}\):
\[
\frac{E(t)}{E_0}=\frac{1}{3}=e^{-t/(RC)} \quad\Longrightarrow\quad \frac{t}{RC}=\ln 3.
\]
Step 2: Solve for the resistance
\[
R=\frac{t}{C\,\ln 3}.
\]
Insert the values \(t=6.6\times 10^{-6}\,\text{s}\), \(C=1.5\times 10^{-6}\,\text{F}\), and (as given) \(\ln 3\approx 1.1\):
\[
R=\frac{6.6\times 10^{-6}}{(1.5\times 10^{-6})\times 1.1}
=\frac{6.6}{1.65}
=4\,\Omega.
\]
Step 3: Note on the logarithm
The problem’s “log 3 = 1.1” is intended as the natural logarithm \(\ln 3\approx 1.1\) (not base-10). Using base-10 would give an incorrect value.
Final answer
4