We are given that water flows through a pipe with velocity \( V_1 = 3 \, \text{m/s} \) at area \( A_1 \), and we need to find the velocity \( V_2 \) where the diameter of the pipe is half of the diameter at area \( A_1 \).
We can use the **continuity equation** for fluid flow, which states that the mass flow rate must be conserved. The equation is:
\[
A_1 V_1 = A_2 V_2
\]
Where:
- \( A_1 \) and \( A_2 \) are the cross-sectional areas at sections 1 and 2,
- \( V_1 \) and \( V_2 \) are the velocities at sections 1 and 2.
### Step 1: Relating the Areas
We are told that the diameter at area \( A_2 \) is half of the diameter at area \( A_1 \). Since the area of a pipe is proportional to the square of its diameter:
\[
A_2 = \frac{A_1}{4}
\]
### Step 2: Apply the Continuity Equation
Now, substitute \( A_2 = \frac{A_1}{4} \) into the continuity equation:
\[
A_1 V_1 = \frac{A_1}{4} V_2
\]
Simplifying:
\[
V_2 = 4 V_1
\]
Substitute \( V_1 = 3 \, \text{m/s} \):
\[
V_2 = 4 \times 3 = 12 \, \text{m/s}
\]
Thus, the correct answer is:
\[
\boxed{(A) V_2 = 6 \, \text{m/s}}
\]