The power dissipated by the jump is given by the formula:
\[
\Delta P = \rho g Q \Delta E
\]
where:
\(\Delta E\) is the change in specific energy,
\(\rho\) is the density of water,
\(g\) is the acceleration due to gravity,
\(Q\) is the discharge.
From the energy equation,
\[
\Delta E = \frac{(y_2 - y_1)^3}{4 y_1 y_2}
\]
For Froude number at upstream:
\[
Fr_1^2 = \frac{V_1^2}{g y_1} - \frac{q^2}{g y_1^3}
\]
\[
Fr_1^2 = \frac{3^2}{9.81 \times 0.5} = 7.34
\]
Now,
\[
y_2 = y_1 \left( -1 + \sqrt{1 + 8 Fr_1^2} \right) = 0.5 \left( -1 + \sqrt{1 + 8 \times 7.34} \right) = 1.68 \, {m}
\]
Next, calculate the change in specific energy:
\[
\Delta E = \frac{(1.68 - 0.5)^3}{4 \times 1.68 \times 0.5} = 0.49 \, {m}
\]
Now, from the power equation:
\[
\Delta P = 1000 \times 9.81 \times 15 \times 0.49 = 72.10 \, {kW} \quad {(rounded to the nearest integer)}.
\]
Thus, the power dissipated by the jump is \( \boxed{72} \, {kW} \) (rounded to the nearest integer).