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:
\( \dot{m} = \rho \cdot Q = 1000 \cdot \frac{600}{60} \, {kg/s} = 10 \, {kg/s} \),
\( P_2 - P_1 = 600 \, {kPa} - 200 \, {kPa} = 400 \, {kPa} = 400 \times 10^3 \, {Pa} \),
\( \rho = 1000 \, {kg/m³} \).
The real work done on the water is:
\[
W_{{real}} = \frac{W_{{ideal}}}{\eta} = \frac{10 \cdot 400 \times 10^3}{0.4} = 10^7 \, {J/s}
\]
The temperature rise \( \Delta T \) is given by:
\[
\Delta T = \frac{W_{{real}}}{\dot{m} \cdot c}
\]
Substitute the values:
\[
\Delta T = \frac{10^7}{10 \cdot 4.2 \cdot 10^3} = 38.5 \, {°C}
\]