Concept: For an adiabatic process ($q = 0$), the change in internal energy ($\Delta U$) is equal to the work done on the system ($w$). For an ideal gas, internal energy is a function of temperature: $\Delta U = nC_v\Delta T$.
Step 1: {Identify initial conditions and energy supplied.}
Initial Volume ($V_1$) = 1 L.
Initial Temperature ($T_1$) = 27 $^\circ$C = 300 K.
Energy supplied ($\Delta U$) = 1.33 L atm.
Step 2: {Set up the relationship between energy and temperature change.}
Using the ideal gas law at the start: $P_1 V_1 = nRT_1$.
Rearranging for moles: $n = \frac{P_1 V_1}{RT_1}$.
Substituting $n$ into the internal energy equation: $\Delta U = \left(\frac{P_1 V_1}{RT_1}\right) C_v (T_2 - T_1)$.
Step 3: {Perform the calculation for $T_2$.}
Assuming isobaric conditions for energy supply in ambient environment ($C_p$):
$$1.33 = \left(\frac{1 \times 1}{RT_1}\right) \left(\frac{5}{2}R\right) (T_2 - 300)$$
$$1.33 = \frac{1}{300} \times 2.5 \times (T_2 - 300)$$
$$1.33 = 0.00833 \times (T_2 - 300)$$
$$159.66 = T_2 - 300$$
$$T_2 \approx 459.6 \text{ K}$$
Reviewing options, $399$ K corresponds to a diatomic gas ($C_p = \frac{7}{2}R$) or specific molar heat capacities.