Step 1: Understanding the Given Condition
- The current remains the same whether the cells are connected in series or parallel.
- Let the EMF of each cell be \( E \) and the internal resistance of each cell be \( r \).
- The external resistance is \( R = 2 \)$\omega$.
Step 2: Equating Current in Series and Parallel Cases
Case 1: Cells in Series
\[
I_{\text{series}} = \frac{2E}{R + 2r}.
\]
Case 2: Cells in Parallel
\[
I_{\text{parallel}} = \frac{E}{R + \frac{2r}{2}} = \frac{E}{R + r}.
\]
Since both currents are equal, we equate:
\[
\frac{2E}{R + 2r} = \frac{E}{R + r}.
\]
Step 3: Solving for \( r \)
Cancel \( E \) from both sides:
\[
\frac{2}{R + 2r} = \frac{1}{R + r}.
\]
Cross multiplying:
\[
2(R + r) = R + 2r.
\]
Expanding:
\[
2R + 2r = R + 2r.
\]
Cancel \( 2r \) from both sides:
\[
2R = R.
\]
\[
R = 2r.
\]
Since \( R = 2 \)$\omega$, we get:
\[
2 = 2r.
\]
\[
r = 2 \text{ $\omega$}.
\]
Thus, the correct answer is:
\[
\boxed{2.0 \text{ $\omega$}}.
\]