To solve this problem, we can use the Bernoulli's principle which states that the total mechanical energy of a fluid flowing along a streamline is constant, ignoring dissipative forces like friction. Mathematically, this can be expressed as:
P1 + (1/2)ρv1^2 = P2 + (1/2)ρv2^2
where P1 and v1 are the pressure and speed at one place, P2 and v2 are the pressure and speed at another place, and ρ is the density of the fluid.
We can rearrange the equation to solve for P2:
P2 = P1 + (1/2)ρ(v1^2 - v2^2)
Substituting the given values, we get:
P2 = 130 kPa + (1/2)(1.2 kg/m^3)(0.6 m/s)^2 - (1/2)(1.2 kg/m^3)(9 m/s)^2
P2 = 130 kPa + 0.216 kPa - 5.832 kPa
P2 = 124.384 kPa
Therefore, the pressure at the other place in the same pipe where the speed is 9 m/s is approximately 124.384 kPa.