Step 1: Application of Bernoulli's principle.
Bernoulli's principle states that for an incompressible fluid in streamline flow, the total mechanical energy (pressure energy, kinetic energy, and potential energy) remains constant. Mathematically:
\[
P + \frac{1}{2} \rho v^2 + \rho gh = \text{constant},
\]
where \( P \) is pressure, \( \rho \) is fluid density, \( v \) is velocity, and \( h \) is height.
Step 2: At the narrowest part of the pipe.
In a horizontal pipe:
\[
P + \frac{1}{2} \rho v^2 = \text{constant}.
\]
At the narrowest part of the pipe, velocity (\( v \)) is maximum due to the conservation of mass (\( A_1v_1 = A_2v_2 \)). As velocity increases, pressure decreases to maintain the constant total energy.
\[
\therefore \text{At the narrowest part of the pipe, velocity is maximum and pressure is minimum.}
\]