I. Introduction
High-Power ultrasonic systems are commonly used in many applications such as food processing [1], water treatment [2], microbe inactivation [3], cleaning [4], and cutting [5]. It is a particularly application-focused technology, although recently a large degree of interest has developed in the research community pertaining to more efficient systems [6], in-process applications [7], and system qualification methods [8]. At the heart of many of these applications is the generation of cavitation within the high-power cell [9]. The phenomenon of cavitation produces a series of dramatic effects that have a powerful effect on the liquid media in which it is induced, effects such as extremely high local temperatures (3000K) and pressures (10 GPa) [10]. These effects create a local environment that can directly influence chemical reactions, material properties, and even chemical structures [11]. Cavitation itself is likely to occur within regions of a test cell that exhibit higher intensities. Therefore, accurate knowledge of spatial pressure distribution within such cells can be valuable when attempting to optimize the location of such regions.