I. Introduction
The equation that describes the complete wave nature of sound in the time and space domain is called the acoustic wave equation and it is given by\begin{equation*} \frac{\partial^{2}p(\mathrm{x},t)}{\partial t^{2}}-c^{2}\nabla^{2}p(\mathrm{x},\ t)=f(\mathrm{x},\ t) \tag{1} \end{equation*}
where the operator is the Laplacian in the three dimensional space, is the sound pressure in the space and time domain, the speed of sound is and is the forcing term corresponding to an acoustic source present in the scene. This equation explains wave phenomena such as interference and diffraction that are observed in the reality [1]. Analytic solutions of the wave equation exist in few problems in physical acoustics hence solutions require assumptions and simplifications [2], [3]. If the sound field is too complicated to handle in an analytic way, then a numerical approach would be effective.