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Use complex amplitudes with time dependence $e^{i\omega t}$, so the outgoing two-dimensional Helmholtz equation kernel has phase $e^{-i{k}_{0}r}$. Dividing the harmonic form of Lighthill acoustic analogy by $c_0^2$ and integrating the two source derivatives by parts gives an amplitude proportional toOnly the magnitude is needed here; the specified kernel omits its constant phase and normalization. In the acoustic compact-source approximation, $\int {\tilde{T}}_{ij}{d}^{2}y=O({\rho }_0{U}^2{\ell }^2)$. With $\omega =O(U/\ell )$, hence $k_0\ell =O(m)$, the two-dimensional compact quadrupole scaling isThe half-power difference from three dimensions comes from cylindrical spreading, including its $k_0^{-1/2}$ factor. As in part (i), the Mach number power is stated with the geometrical range factor separated; $k_{0}r\gg 1$ is still required.