According to the principle of continuity for incompressible fluids, the flow rate (volume per unit time) must remain constant. This is expressed as:
\[
A_1 v_1 = A_2 v_2
\]
Where:
- \( A_1 = \pi r_1^2 \) is the cross-sectional area at the wider end,
- \( A_2 = \pi r_2^2 \) is the cross-sectional area at the narrower end,
- \( v_1 = 5 \, \text{m/s} \) is the velocity at the wider end,
- \( v_2 \) is the velocity at the narrower end.
Now, substitute the values:
\[
A_1 v_1 = A_2 v_2
\]
\[
\pi (2)^2 \times 5 = \pi (1)^2 \times v_2
\]
\[
4 \times 5 = 1 \times v_2
\]
\[
v_2 = 20 \, \text{m/s}
\]
Thus, the velocity of the water at the narrower end is \( 20 \, \text{m/s} \).