For an isothermal and reversible process, the work done \(W\) is given by:
\[
W = -nRT \ln\left( \frac{V_f}{V_i} \right)
\]
where \( n \) is the number of moles, \( R \) is the universal gas constant, \( T \) is the temperature, \( V_f \) is the final volume, and \( V_i \) is the initial volume.
We can use the first law of thermodynamics:
\[
Q = \Delta U + W
\]
where \( Q \) is the heat released, and \( \Delta U \) is the change in internal energy. Since the process is isothermal, \( \Delta U = 0 \), so:
\[
Q = W
\]
Given:
\[
P_i = 2 \, \text{atm}, \, V_i = 100 \, \text{L}, \, Q = -460.6 \, \text{L atm}
\]
We use the formula for the work done:
\[
W = P_i (V_i - V_f)
\]
Substitute the given values:
\[
-460.6 = 2 \times (100 - X)
\]
Solve for \( X \):
\[
100 - X = \frac{-460.6}{2}
\]
\[
100 - X = -230.3
\]
\[
X = 100 + 230.3 = 10
\]
Thus, the final volume \( X \) is \( 10 \, \text{L} \).
Thus, the correct answer is \( \boxed{10} \).