For parallel cells with emf \( E_1 = 4 \, \text{V} \), \( r_1 = 1 \, \Omega \), \( E_2 = 2 \, \text{V} \), \( r_2 = 2 \, \Omega \), equivalent emf:
\[
E_{\text{eq}} = \frac{E_1 r_2 + E_2 r_1}{r_1 + r_2} = \frac{4 \times 2 + 2 \times 1}{1 + 2} = \frac{8 + 2}{3} = \frac{10}{3} \, \text{V}.
\]
Equivalent internal resistance:
\[
\frac{1}{r_{\text{eq}}} = \frac{1}{r_1} + \frac{1}{r_2} = \frac{1}{1} + \frac{1}{2} = \frac{3}{2} \quad \Rightarrow \quad r_{\text{eq}} = \frac{2}{3} \, \Omega.
\]
Total resistance: \( r_{\text{eq}} + R = \frac{2}{3} + 5 = \frac{17}{3} \, \Omega \).
Current through external resistance:
\[
I = \frac{E_{\text{eq}}}{r_{\text{eq}} + R} = \frac{\frac{10}{3}}{\frac{17}{3}} = \frac{10}{17} \, \text{A} \approx 0.588 \, \text{A}.
\]
Answer: \( \frac{10}{17} \, \text{A} \).