Using the principle of continuity for incompressible fluids, the mass flow rate must remain constant. This is given by the equation:
\[
A_1 v_1 = A_2 v_2
\]
Where:
- \( A_1 = 1 \, \text{m}^2 \) is the cross-sectional area at point A,
- \( v_1 = 2 \, \text{m/s} \) is the velocity at point A,
- \( A_2 \) is the cross-sectional area at point B,
- \( v_2 = 4 \, \text{m/s} \) is the velocity at point B.
Substitute the known values:
\[
1 \times 2 = A_2 \times 4
\]
\[
A_2 = \frac{2}{4} = 0.5 \, \text{m}^2
\]
Thus, the cross-sectional area at point B is \( 0.5 \, \text{m}^2 \).