Final answer:
The required pressure at the small end of the pipe is 0.
Step-by-step explanation:
To determine the required pressure at the small end of the pipe, we can use Bernoulli's equation. Bernoulli's equation states that the sum of the pressure energy, kinetic energy, and potential energy per unit volume of a fluid remains constant along a streamline. In this case, we can assume that the velocity of the water at the large end of the pipe is negligible compared to the velocity at the small end of the pipe, so we can neglect the kinetic energy term.
Using the equation:
P + ρgh = constant
where P is the pressure, ρ is the density of water, g is the acceleration due to gravity, and h is the height difference between the small and large ends of the pipe.
Substituting the given values, we have:
- ρgh + P_small = ρgh + P_large
- P_small = P_large
Since the pressure at the large end is atmospheric pressure (which we can assume to be 0), the required pressure at the small end of the pipe is also 0.