According to the Bernoulli's principle, the total mechanical energy per unit volume along a streamline remains constant. The equation for Bernoulli's principle is:
\[
P + \frac{1}{2} \rho v^2 + \rho gh = \text{constant}
\]
where:
- \( P \) is the pressure,
- \( \rho \) is the density of the fluid,
- \( v \) is the velocity of the fluid,
- \( g \) is the acceleration due to gravity (which is ignored in this case as the pipe is horizontal),
- \( h \) is the height (also ignored in this case, as we are dealing with a horizontal pipe).
At two points along the streamline, we have:
\[
P_1 + \frac{1}{2} \rho v_1^2 = P_2 + \frac{1}{2} \rho v_2^2
\]
The velocity of the water is related to the cross-sectional area by the continuity equation:
\[
A_1 v_1 = A_2 v_2
\]
Given that the areas are \( A_1 = 10 \, \text{cm}^2 = 10^{-4} \, \text{m}^2 \) and \( A_2 = 5 \, \text{cm}^2 = 5 \times 10^{-5} \, \text{m}^2 \), and the velocity at \( A_1 \) is \( v_1 = 1 \, \text{m/s} \), we can find \( v_2 \):
\[
v_2 = \frac{A_1 v_1}{A_2} = \frac{10^{-4} \times 1}{5 \times 10^{-5}} = 2 \, \text{m/s}
\]
Now, using Bernoulli’s equation, we can solve for \( P_2 \):
\[
P_1 + \frac{1}{2} \rho v_1^2 = P_2 + \frac{1}{2} \rho v_2^2
\]
\[
2000 + \frac{1}{2} \times 1000 \times (1)^2 = P_2 + \frac{1}{2} \times 1000 \times (2)^2
\]
\[
2000 + 500 = P_2 + 2000
\]
\[
P_2 = 500 \, \text{Pa}
\]
Thus, the pressure at the second point is \( 2000 \, \text{Pa} - 1800 \, \text{Pa} = 200 \, \text{Pa} \).