Step 1: Understand free expansion.
The gas expands into vacuum, so the external pressure is zero. The work done is \[ W = -P_{ext}\Delta V = 0 \] No work is done by or on the gas.
Step 2: Find the heat exchanged.
The process is isothermal at \(300\ K\), so for an ideal gas \(\Delta U = 0\). By the first law \(\Delta U = Q + W\), with \(W=0\) we get \(Q = 0\): no heat flows to or from the surroundings.
Step 3: Entropy of the surroundings.
Since the surroundings exchange no heat, \[ \Delta S_{surr} = \frac{Q_{surr}}{T} = 0 \]
Step 4: Entropy of the system.
Entropy is a state function, so we use the isothermal expansion formula \[ \Delta S_{sys} = nR\ln\frac{V_2}{V_1} \]
Step 5: Put in the numbers.
With \(n = 2\), \(V_2/V_1 = 100/10 = 10\): \[ \Delta S_{sys} = 2R\ln 10 = 2R(2.303) = 4.606\,R \]
Step 6: State the result.
So \(\Delta S_{sys} = 4.606\,R\) and \(\Delta S_{surr} = 0\), which is option 1.
\[ \boxed{\Delta S_{sys}=4.606\,R,\ \Delta S_{surr}=0} \]