Low pressure setups (up to 150 psi) for creating hydrodynamic cavitation are investigated in this study. The decomposition of chloroform in water is used as a model reaction. The effects of upstream pressure, fluid velocity, Cavitation number, C v , and b 0 on the conversion are compared with regard to the effectiveness (conversion per pass) with changing flow conditions and scale-up terms within three different setups. The values of C v and b 0 are seen to be significant parameters in optimizing the hydrodynamic cavitation. Moreover, the optimal values of these parameters shift to smaller values with increasing pipe diameter. The influence of a new orifice plate specific parameter, d, on the collapse conditions, is also described.
IntroductionCavitation can potentially be used for a wide range of applications [1][2][3]. It is most commonly generated by ultrasonic transducers (acoustic cavitation), but there are problems associated with ultrasonic transducers concerning energy requirements and scale-up potential [4]. An alternative for generating cavitation events is hydrodynamic cavitation, where the bubbles are created due to pressure losses caused by an increasing fluid velocity (Bernoulli principle) and/or boundary layer separation [5,6]. This technology has been described as being more energy efficient and offers better scale-up possibilities [7][8][9]. A number of pipe flow systems with varying integrated restrictions, i.e., valve, venturi, and orifice plates, have been investigated [10,11]. The hydrodynamic cavitation has been studied extensively including parameter studies [5,6,9,10,[12][13][14][15], various applications [7,[16][17][18][19][20][21], energy efficiency assessments [8,16,21,22] and theoretical work [5,6,9,13,[23][24][25][26].Overall, a significant number of parameters exists that affect hydrodynamic cavitation, in particular, the numbers of generated (reactive) bubbles and the collapse conditions. An overview of the effective parameters in hydrodynamic cavitation, is shown in Fig. 1. The collapse conditions are defined as the temperatures/pressures reached at the bubble collapse [5]. In acoustic cavitation, this term is described for an adiabatic collapse by the following expressions, Eqs. (1) and (2) [27,28] 1) :(1)where T 0 is the liquid temperature, P m is the acoustic pressure at initiation of collapse, c is the ratio of specific heats of the dissolved gas or vapor and p v is the vapor pressure of the solvent. Several parameters have been introduced to characterize hydrodynamic cavitation systems. The dimensionless Cavitation number, C v , is defined by Eq. (3):where p d is the measured downstream pressure, p v is the vapor pressure (0.023 bar), q l is the density of the solution (1000 kg m -3 ), and v is the measured fluid velocity. These terms describe the ability of a system to generate cavitation, where smaller values are preferred. Moreover, C v can be correlated with the number of cavitation events and the collapse intensity [14,29]. The dimensionless number, b 0 , which character...