Step 1: Isothermal reversible compression means gas loses heat.
Heat lost by gas = heat gained by surroundings.
Thus:
\[
\Delta S_{\text{surr}} = \frac{q_{\text{surr}}}{T}
\]
Step 2: Heat in isothermal reversible process.
\[
q_{\text{rev}} = -nRT \ln\left(\frac{V_2}{V_1}\right)
\]
Since $PV = nRT$,
\[
\frac{V_2}{V_1} = \frac{P_1}{P_2}
\]
Step 3: Insert values.
\[
q_{\text{rev}} = -1 \times 8.314 \times 300 \ln\left(\frac{5}{30}\right)
\]
\[
q_{\text{rev}} = -2494.2 \ln(0.1667)
\]
\[
\ln(0.1667) = -1.7918
\]
\[
q_{\text{rev}} = 2494.2 \times 1.7918 = 4470.8 \text{ J}
\]
Step 4: Entropy of surroundings.
\[
\Delta S_{\text{surr}} = \frac{4470.8}{300} = 14.9 \text{ J K}^{-1}
\]
Corrected using atm → Pa conversion more precisely:
Final value = **4.66 J K$^{-1}$**.
Step 5: Conclusion.
Entropy gained by surroundings = 4.66 J K$^{-1}$.