Experimental investigation of the influences of different liquid types on acoustic emission energy levels during the bubble formation process
- 3k Downloads
Bubble formation phenomena in a two-phase gas/liquid system occur in many industries that involve boiling; such as desalination stations, nuclear reactors, chemical plants, and fluid piping transportation and processes. Bubble formation phenomena cause problems, such as a decrease in equipment efficiency, vibration, noise, and solid surface erosion. Applications of the acoustic emission (AE) technique for monitoring bubble formation and burst stages in boiling processes are marginal in terms of extension in comparison to other applications of the AE technique. The use of the AE technique in this experimental investigation covers the frequency range between 100 and 1000 kHz, showing that the AE sensor can detect acoustic emissions from an occurrence of bubble formation. Statistically, it was found that the best AE parameter indicator for bubble formation was AE-RMS (root mean square).
KeywordsAcoustic emission Bubble formation Pool boiling vessel
List of symbols
Frequency of the bubble
Polytrophic constant of the gas inside the bubble
Bubble formation and cavitation are common phenomena in many industrial processes that include gas–liquid systems or just liquid flow, such as manufacturing processes, which use gas or water jets that are blown into a liquid to provide energising processes, and in gas–liquid flows that commonly occur in chemical processing plants. However, while cavitation may not affect the surface integrity of a liquid, the collapse of cavitation bubbles close to the wall or other surfaces can cause active surface erosion, known as cavitation damage. In liquid transportation industries, the cavitation phenomenon is a contributor to the failure and inefficiency of pumps and valves that leads to a decrease in the life of the equipment . For liquid power systems, such as in gas-lift pumps, cavitation will cause vibration, noise, reduced efficiency, pitting, and erosion of the surfaces in contact with collapsing bubbles . Weninger et al.  noted that the bubble collapse generates an amount of energy in the form of a shockwave and that transducers can measure its pressure pulse. It is possible to correlate pressure pulses from bubble activity with bubble size; in other words, through measuring the size of the bubble using an acoustic technique. It is well known that bubble activities are potential sources of AE, and that the acoustic energy released from the bubble formation can be used to determine certain properties of the surrounding liquid . This paper starts with the definition of cavitation, which is followed by a general presentation of bubble occurrence phenomena, and of the acoustic techniques that are suitable for monitoring and detection of bubble formation at the early stages of the boiling processes.
Cavitation is a phenomenon that occurs in rotating machines and flow process, which is characterised by the collapse of voids in the flow with an explosive effect generating localised high pressures and temperatures. Cavitation occurs when the liquid is subjected to a drop in pressure, which is equal or lower than the saturated vapour pressure at a given temperature [5, 6]. To reduce the damage caused by cavitation, bubble formation must be monitored and detected in rotating machines and valves . Acoustic emission is a physical phenomenon that occurs within or on the surface of the material. It is defined as elastic waves generated by the rapid release of energy from localised sources within a material due to a deformation or fracture process [8, 9]. Application of the acoustic emission technique is not limited to detection and diagnosis of cavitation in hydraulic systems, such as centrifugal pumps and valves; it can be used as a monitoring tool for different types of industries, such as petroleum engineering using gas–liquid pumps, mechanical processes, and chemical processing plants. Furthermore, the AE technique can be applied to the monitoring and diagnosis of bubble formation in boiling processes.
Alhashan et al.  used the AE technique in the monitoring of bubble formation during the boiling process. They found a clear association between increasing AE levels and bubble formation. Benes and Uher  found that the parameters of the AE signal have a correlation with overheating during heat transfer. It was established that the AE signal could be used to predict the boiling phenomena. Carmi et al.  used the AE technique in a flow boiling experiment to detect bubble transit, noting the possibility of using AE in the detection of bubble dynamic events at the early stages in the boiling process. The AE technique has been used to diagnose the bubble formation process and monitor bubble departure from the heating surface of the boiler to the surface of the liquid container during pool boiling . In another investigation, centring on two-phase flows, Addali  found that the gas void fraction (GVF) can be determined by measurement of the acoustic emission. Moreover, it was concluded that there is a direct correlation between the AE energy and GVF. It was also noted that an increase in superficial gas and liquid velocities caused an increase in AE energy levels. Husin et al.  found that AE was a suitable technique for the detection of a single bubble formation and burst, with AE being used to measure the velocity of the acoustic wave. Jaubert et al.  used AE as the method for the detection of cavitation phenomena in pumps and valves at an early stage, which makes it possible to study incipient cavitation occurrences. Husin  found that when the bubble size and liquid viscosity increase, the level of AE signals also increases. One particular item of interest in this programme was the investigation of AE energy radiated from the bubble formation. The bubble formation phenomena have potential energy that depends on the pressure within the bubbles and their volume.
The sound created by bubble formation, oscillation and burst at the free surface is dependent on the bubble size. The period of stress pulse due to bubble collapse and burst is very short (ms) . Acoustic emission of bubble burst is correlated to the size of the bubble . For pool boiling, the bubble dynamics are divided into five stages: (1) bubble formation at the bottom of the boiler wall, (2) bubble rising, (3) bubble coalescence, (4) splitting of bubbles, and (5) bubble burst at the free surface  . When the bubble cavities collapse, it causes sound and dissipation of energy in the water . It is known that the pressure pulses associated with the bubble formation and burst at the surface of the liquid also act as sources of acoustic emission  . Blanchard and Woodcock  observed that the bubbles coalesce in tap water more than in sea water. Additionally, the bubbles produced in sea water are smaller and continue longer than in pure water. Ceccio et al.  concluded that there is a significant difference between bubble occurrence in salt water and fresh water. It was observed that the acoustic emission of the bubble cavitation in fresh water was lower than that produced in salt water. Moreover, they noted that small bubbles produce higher acoustic emission compared to large bubbles.
Use of AE to monitor the process.
Study of the effect of different liquid types (tap water, demoralise water, and salt water) on AE signals.
Investigation of the influence of the input power-supply (2.5-3 kW) on AE levels.
Study of the effect of threshold levels on AE signals.
Experimental procedures of boiler test
Water Level (mm)
Salt water (5 g/L) concentration
A commercially available piezoelectric AE sensor (Physical Acoustic Corporation type “PICO”) with an operating range of 100–1000 kHz was used. Two acoustic sensors were attached to the external surface of the boiler using superglue. The two AE channels were distanced at 200 mm, vertically apart. The first channel was connected to the bottom of the boiler, 100 mm from the bottom surface, to detect the initiation of bubble formation, while channel 2 was positioned 200 mm above channel 1 to monitor bubble burst, and oscillations when the bubbles depart towards the surface at high water levels (see Fig. 1). The acoustic sensors were linked to a data acquisition system by a preamplifier, set at 40 dB gain. The system was continuously set to acquire AE waveforms at a sampling rate of 2 MHz. The software (signal processing package “AEWIN”) was incorporated within a PC to monitor AE parameters, such as AE-RMS and AE-Energy (recorded at a time constant of 10 ms and a sampling rate of 100 Hz).
Results, observations, and discussions
Observation of the effect of salt water (5 g/L) concentration on AE signals
Figure 3: Observation of boiling test at salt water (5 g/L) level of 200 mm.
At the beginning of the process, there was initial bubble formation on the bottom wall of the pool boiling vessel. Moreover, the bubbles formed on cavity, scratches and grooves on the heated surface of the boiler. This process is called heterogeneous nucleation. Then the bubbles detach from the heating surface and rise to the surface of the water; at an early stage at about 22 °C. Bubbling happens on the boundary between the salt water (5 g/L) and the solid wall of the boiler. In addition, the bubbles also occur between the water and small parts of salt suspended in the water. For this reason, the bubbles detach from the heating element at an early stage.
The value of AE-RMS ranked the highest for both channels, between 495 and 825 s. During this stage, the temperature rises and the bubbles start to form at a faster rate. Then the bubbles grow and depart towards the free surface, where they burst and release the vapour. As a result, the heat flux attains its maximum value. However, the value of AE-RMS in channel 1 is higher than that of channel 2, with 0.0009 volts and 0.0005 volts, respectively, because the position of channel 2 is further from the water surface. The value of AE signal decreases slowly to approximately 0.0007 volts in channel 1, between 60 and 75 °C. During this period, the bubbles start to detach from the heating surface into the surrounding water, some of which rise from the heating wall of the boiler to the water surface, while others combine with adjacent bubbles and then stick to the internal wall of the boiler, causing an isolated layer. This layer is responsible for attenuation of AE signals. Obviously, there is a constant in the value of AE signal for channel 2, between 55 and 95 °C, because the position of channel 2 is further from the water surface. It was noted that when the salt water (5 g/L) approaches the boiling stage, between 90 and 100 °C, the value of AE increases in both channels. These temperatures cause a rise in the heat flux and more bubbles form and increase whilst travelling towards the free surface, where large bubbles start to burst on the water surface at the end of the test. Also, the size and internal energy of the bubbles increased.
Observation of the difference between bubble formation in tap water and demineralized water
For the demineralized water, the bubbles start to detach from the heating surface of the boiler at approximately 570 s, between 50 and 60 °C. In this type of water, there are considerably fewer small particles in the liquid from heterogeneous nucleation can occur between the liquid and small particles suspended in the liquid. Furthermore, the thermal motions inside the demineralized water form temporary, microscopic gaps which by themselves can produce nuclei cavitation, which is necessary for the rupture and growth of micro-bubbles. This phenomenon is called homogeneous nucleation.
It can be seen that the detachment of bubbles from the heating surface in the tap water is faster than that of demineralized water because there is a much lower concentration of mineral ions and small particles inside the water.
Observation of the difference between bubble formation in tap water and salt water (5 g/L)
For the tap water, the bubbles start to form on the heating element of the boiler where these bubbles were stuck on the bottom surface of the vessel, which is between 10 and 245 s. At 245 s, the bubbles start to detach from the bottom surface of the boiler into the surrounding water. A sharp transition in the AE movement occurs in tap water, as shown in Fig. 5. This dramatic change indicates the start of the boiling process during pool boiling. More bubbles are formed and depart towards the surface between 30 and 50 °C, due to the heat transferring from the boiler’s heating element to the water as the temperature increases. In the salt water (5 g/L), the bubbles start to detach from the heating wall of the vessel into the surrounding water at an early stage, between 22 and 45 °C. It was detected that the rate average of bubble detachment from the heating surface in salt water (5 g/L) is faster than that of tap water. This is due to the surface tension of salt water (5 g/L) being higher than that of tap water. Additionally, bubble gaps appear between the water and small parts of salt suspended in the water, which is responsible for the rupture and growth of micro-bubbles.
In the tap water, many large bubbles appeared and disappeared in a short time. However, there are no large individual bubbles in the salt water. The mechanism of bubble formation in tap water is the same as in salt water but there is a difference in the size of the bubbles. Moreover, the acoustic emission of the bubble formation in tap water was less than that of salt water, between 10 and 330 s, as shown in Fig. 5. Overall, it can be concluded that the bubbles form and rise to the water surface between 30 and 50 °C in tap water, and between 22 and 45 °C in salt water.
Observation of the difference between bubble formation in demineralized water and salt water (5 g/L)
For demineralized water, there is a stable AE signal from 0 to around 660 s because the bubbles start to form on the bottom surface of the vessel and then stick on the heating surface between 20 and 45 °C. At around 660 s, the bubbles begin to detach from the boiler’s heating wall and rise to the water surface between 50 and 60 °C. This is because the thermal motions inside the liquid create temporary, microscopic gaps that can produce nuclei cavitation, which is necessary for the rupture and growth of micro-bubbles. This process is called homogeneous nucleation. In addition, the value of the AE significantly increases to reach 0.0014 volts, when more bubbles form. The value of the AE signal decreases gradually to approximately 0.00075 volts, between 60 and 78 °C. During this stage, when the bubbles form due to increasing temperature, some of which rise from the heating boiler wall into the surrounding water, others combine with adjacent bubbles and stick to the internal wall of the vessel, causing an isolated layer. This layer is responsible for attenuation of AE signals. When the water approaches the boiling phase, between 82 and 100 °C, a slight increase in the value of AE signal from 0.00075 volts to approximately 0.0015 volts in demineralized water was observed, as shown in Fig. 6. This rise can be attributed to the heat gained by the water. This heat caused more bubbles to form and depart towards the water surface, where finally large bubbles burst on the water surface at the end of the test; and when the bubbles’ size and their internal energy increased.
For salt water (5 g/L), the bubbles start to detach from the heating element at 22 °C, where more bubbles form and depart from the bottom of the boiler into the surrounding water. During this stage, gas voids occur on the boundary between the liquid and small parts of salt inside the liquid, being suspended in the liquid. For this reason, the bubbles are detached at an early stage from the heating element in the salt water (5 g/L). These bubbles combine with each other and then start to split to produce more bubbles.
It can be seen that bubbles detaching from heating surface travelling towards the water surface in the salt water (5 g/L) are faster than that of demineralized water. This is because there are small particles of salt within the water that can produce nuclei cavitation, which is necessary for the rupture and growth of micro-bubbles. This event is called hydrophilic surface.
Influence of threshold levels on AE signals
The value of AE-hits was ranked the highest with 160,000 hits for a water level of 350 mm, at 36 dB. Furthermore, the threshold parameters have an effect on AE signal levels. When the threshold levels increase, the number of hits decreases, as shown in Fig. 7.
Influence of power-supply on AE signals
For a power-supply of 2.5 kW, the bubbles start to detach from the heating surface into the surrounding water at around 33 °C. The levels of AE signal increase between 33 and 50 °C, where more bubbles form caused by heat flux increases. With a power-supply of 3 kW, the bubbles start to detach from the boiler wall bottom travelling towards the water surface directly, at around 22 °C. There is a significant increase in the level of AE signals between 22 and 50 °C. The increase in the power supply causes a high temperature and heat flux during pool boiling.
The value of AE signal decreases slowly between 50 and 80 °C for a power-supply of 2.5 kW. For a power-supply of 3 kW, the level of AE signal decreases gradually between 50 and 90 °C. It was observed that the power-supply has a significant effect on AE levels and bubble formation behaviour, where the bubbles start to detach from the heating surface at an early stage with a power-supply of 3 kW compared with the bubble detachment with a power-supply of 2.5 kW. This is because more heat flux and energy are obtained from a 3 kW power-supply.
This paper focuses on monitoring and diagnosis of bubble occurrence in boiling processes using AE technology and depends on previous analysis and its investigation. It was observed that AE parameters, such as AE-RMS and threshold levels, are sensitive, robust and reliable in the monitoring and detection of bubble activity and the movement towards the surface of the water. It was observed that the presence of bubble formation in pool boiling is detectable with the AE technique by applying standard analysis techniques, such as RMS, hits and threshold levels. Furthermore, there is a relationship between bubble formation and temperature during the boiling process. The monitoring of bubble formation using AE technology can complement other condition monitoring methods, all of which are aimed at reducing energy losses and improving life cycle costs. AE technology is capable of detecting the dynamic formation and bursting of bubbles. This technique is necessary for predicting the incidence of boiling in nuclear reactors. This is also the case for observing heat exchanger systems in industrial chemical processes, detecting bubble occurrence in the petrochemical industry, detecting gas layers in oil drilling, and monitoring and detection of cavitation phenomena in centrifugal pumps and valves. It was concluded that the different liquid types have an influence on AE energy levels and bubble formation. In addition, the power supply has a significant effect on AE levels; as the power-supply increases, the levels of AE signals increase during the bubble formation process.
Finally, this paper provides an early investigation of ongoing research in the application of the AE technique to detect bubble formation in pool boiling. The authors are also working on another study of bubble formation and collapse in valves that will be published in the near future. Expectantly, the following investigation will contribute to distinguishing the differences between bubble formation and bubble collapse due to cavitation using the AE technique. It is aimed to use waveform analysis for this approach.
- 2.Rydberg, K.E.: Energy efficient water hydraulic systems. In: The fifth international conference on fluid power transmission and control, HangZhou, China, 2001, pp 44–46Google Scholar
- 4.Naveen N. Sinha, Los Alamos N. Characterization of liquids using gas bubbles. United States (12), Patent Application Publication (10). 2004; 1(19). http://file:///C:/Users/s218245/Downloads/US20040144175.pdfGoogle Scholar
- 5.Brennen, C.E.: Cavitation and bubble dynamics, pp. 145-185. Oxford University Press, Oxford, (1995). doi: 10.1017/CBO9781107338760
- 7.Brennen, C.: Hydrodynamics of Pumps. NREC, Oxford University Press (1994). doi: 10.1017/CBO9780511976728
- 8.Alssayh, M.A.: Slug velocity measurement and flow regime recognition using acoustic emission technology. PHD Thesis. Cranfield University; 2013Google Scholar
- 9.FDIS ISO. International Standards Organization Documents 22096. Documents. ISO, Generic, R.T. (eds.) Condition monitoring and diagnosis of machines. Acoust Emiss; 2007Google Scholar
- 10.Alhashan, T., Elforjani, M., Addali, A., Teixeira, J.: Monitoring of bubble formation during the boiling process using acoustic emission signals. Int J Eng Res Sci. 2(4), 66–72 (2016)Google Scholar
- 11.Benes, P., Uher, M.: Identification of liquid boiling by acoustic emission. Fundam Appl Metrol. 1, 1396–1401 (2009)Google Scholar
- 12.Carmi, R., Bussiba, A., AI and HI. Detection of transient zones during water boiling by acoustic emission. Acoust Emiss. 2011; 29: 89–97Google Scholar
- 14.Addali, A.: Monitoring gas void fraction in two-phase flow with acoustic emission. PHD Thesis. Cranfield University; 2010Google Scholar
- 15.Husin, S., Mba, D.: Acoustic emission of a single bubble activities. In: Proceedings of the World Congress on Engineering 2010 Vol. II. London UK; 2010. pp. 0–5Google Scholar
- 16.Jaubert, L., Maillard, S., Sulis, V.: Monitoring of fluidic systems by acoustic emission. In: European conf. AE Testing. France; 2008. pp. 334–339Google Scholar
- 17.Husin, S.: An experimental investigation into the correlation between Acoustic Emission (AE) and bubble dynamics. Cranfield University (2011). ISBN: 9789881821072Google Scholar
- 20.Pumphrey, H. C., Crum, L.: Sources of ambient noise in the ocean and experimental investigation. PhD thesis. University of Mississippi (1989)Google Scholar
- 21.Leighton, T.G.: The acoustic bubble: Oceanic bubble acoustics and ultrasonic cleaning. In: Proceedings of Meetings on Acoustics. 2015; 24: 1–5. doi: 10.1121/2.0000121
- 23.Plesset, M. S.: Shockwaves from cavity collapse. Philosophical Transactions of the Royal Society of London, vol. 260, pp. 241–244. Royal Society (1966)Google Scholar
- 27.Derakhshan, J.O., Houghton, R.R.J.K.: Cavitation monitoring of hydro turbines with RMS acoustic emission measurements. Proc. World Meet. On Acoust. Emiss. 15, 305 (1989)Google Scholar
- 28.Blanchard, D.C., Woodcock, A.H.: Bubble formation in modification in the sea and its meteorological signifcance. Tellus 9, 145–158 (1957)Google Scholar
Open AccessThis article is distributed under the terms of the Creative Commons Attribution 4.0 International License (http://creativecommons.org/licenses/by/4.0/), which permits unrestricted use, distribution, and reproduction in any medium, provided you give appropriate credit to the original author(s) and the source, provide a link to the Creative Commons license, and indicate if changes were made.