The work done on the water in an adiabatic pump can be calculated using the following relation:
\[
W = \dot{m} \cdot \left( \frac{P_2 - P_1}{\rho} \right)
\]
Where:
\( \dot{m} \) is the mass flow rate,
\( P_1 \) and \( P_2 \) are the initial and final pressures,
\( \rho \) is the density of water.
The mass flow rate \( \dot{m} \) is related to the volumetric flow rate by:
\[
\dot{m} = \rho \cdot Q
\]
Where \( Q \) is the volumetric flow rate.
Given:
\( \dot{m} = 1000 \cdot 600 \, {L/min} = 600 \, {kg/min} = 10 \, {kg/s} \)
The specific heat of water \( c = 4.2 \, {kJ/(kg°C)} \)
The efficiency of the pump is 40%, so the work done on the water is:
\[
W_{{real}} = \frac{W_{{ideal}}}{{Efficiency}} = \frac{10 \cdot (600 - 200)}{0.4} = 10000 \, {J/s}
\]
The temperature rise \( \Delta T \) is calculated from the first law of thermodynamics:
\[
\Delta T = \frac{W_{{real}}}{m \cdot c}
\]
Substitute the values:
\[
\Delta T = \frac{10000}{10 \cdot 4.2} = 0.139 \, {°C}
\]
Therefore, the maximum temperature rise is 0.139°C.