The work done by an ideal gas during an isothermal expansion is given by:
\[
W = -P \Delta V
\]
where \( W \) is the work, \( P \) is the constant pressure, and \( \Delta V \) is the change in volume. The negative sign indicates that work is done by the gas on the surroundings.
Now, the work done during the isothermal expansion is also related to the ideal gas law, which is:
\[
PV = nRT
\]
where \( n \) is the number of moles, \( R \) is the universal gas constant, and \( T \) is the temperature in Kelvin.
Since the pressure is constant, we can solve for the pressure:
\[
P = \frac{nRT}{V}
\]
Substituting this into the expression for work:
\[
W = - \frac{nRT}{V} \Delta V
\]
Given that \( W = -189.1 \) L atm, \( n = 2 \) mol, and \( \Delta V = 50 - 5 = 45 \) L, we can substitute these values to solve for \( T \).
First, rearrange the equation for \( T \):
\[
T = \frac{W \cdot V}{nR \cdot \Delta V}
\]
Substitute the known values:
\[
T = \frac{(-189.1) \cdot 5}{2 \cdot 0.0821 \cdot 45}
\]
Solving this gives \( T = 500 \, \text{K} \), and converting to Celsius:
\[
T_{\text{C}} = 500 - 273 = 227 \, \degree C
\]