Evaluating an ultrasonic magnetostrictive transducer with conical nickel core: performance and application

Evaluating an ultrasonic magnetostrictive transducer with conical nickel core: performance and application | Research Square window.SnipcartSettings = { analytics: { enabled: false } }; (function() { var accessVector = localStorage.getItem('access_vector') || ''; window.dataLayer = window.dataLayer || []; if (accessVector) { window.dataLayer.push({ user: { profile: { profileInfo: { snid: accessVector } } } }); } })(); (function(w,d,s,l,i){w[l]=w[l]||[];w[l].push({'gtm.start':new Date().getTime(),event:'gtm.js'});var f=d.getElementsByTagName(s)[0],j=d.createElement(s),dl=l!='dataLayer'?'&l='+l:'';j.async=true;j.src='https://www.googletagmanager.com/gtm.js?id='+i+dl;f.parentNode.insertBefore(j,f);})(window,document,'script','dataLayer','GTM-K279D39R'); Browse Preprints In Review Journals COVID-19 Preprints AJE Video Bytes Research Tools Research Promotion AJE Professional Editing AJE Rubriq About Preprint Platform In Review Editorial Policies Our Team Advisory Board Help Center Sign In Submit a Preprint Cite Share Download PDF Research Article Evaluating an ultrasonic magnetostrictive transducer with conical nickel core: performance and application Danial Gandomzadeh, Mohammad Hossein Abbaspour-Fard, Yeganeh Sabeghi, and 1 more This is a preprint; it has not been peer reviewed by a journal. https://doi.org/ 10.21203/rs.3.rs-2009995/v1 This work is licensed under a CC BY 4.0 License Status: Under Review Version 1 posted 4 You are reading this latest preprint version Abstract In recent years, ultrasonic machining has been developing rapidly and it is used in areas such as abrasive machining, cleaning, and welding. In this research, a magnetostrictive device with pure nickel conical core with cone angle of 30 degrees was constructed. The observed sound pressure level was used as a measure of transducer performance. Also the ability of the device to reduce the residual pesticide on cucumber surface due to cavitation was evaluated. The results showed that the sound pressure from simulation by JMAG-Designer software is almost the same as the sound pressure produced in the constructed transducer. To assess the performance of the device in removing residual pesticide from cucumber surface and evaluate the changes in peel texture of cucumber, the GC and SEM methods were used, respectively. The GC results showed that with 20 min treatment, the removal of pesticide based on height and chromatogram area were 75% and 83%, respectively. The SEM results showed that by increasing the treatment time, the stomatal pore area reduced from 144.74 \({\mu m}^{2}\) (reference) to 30.56 \({\mu m}^{2}\) (20 min treatment). This results are promising, hence further research is suggested towards enhancing the device for commercial use in biomaterials processing operations such as cleaning and removing pesticides from fruits and vegetables. Magnetostrictive ultrasonic transducer Residual Pesticide Cleaning GC SEM Figures Figure 1 Figure 2 Figure 3 Figure 4 Figure 5 Figure 6 Figure 7 Figure 8 Figure 9 1. Introduction In recent years, ultrasonic machining has developed rapidly. It has been used in applications such as ultrasonic abrasive machining, cleaning and welding. Fruits and vegetables contain important nutrients that are essential for human health. But agricultural pesticides are widely used to protect products against insects, diseases and maximizing crop yields. Residual pesticides have been considered in terms of their effects on human health as well as environmental effects. Because these pesticides cause diseases such as cancer and reproductive endocrine disorders [ 1 ]. In general, different methods are used for peeling and cleaning agricultural products including: manual, mechanical, chemical, enzymatic, and thermal [ 2 ]. Conventional, mechanical, chemical methods and immersion in hot water cause adverse effects on the product [ 3 ]. Alkaline solution or steam pressure can also be used for this purpose. However, these methods have some disadvantages such as excessive water and chemical consumptions, high cost, as well as problems related to peeling waste [ 4 ]. In addition, infrared (IR) [ 5 ] and ultraviolet (UV) radiations [ 6 ], [ 7 ] can be used for peeling and cleaning agricultural products. Chemical methods use natural acids such as aceticacid, benzoicacid, citricacid, malicacid, sorbicacid, succinicacid, and tartaricacid [ 2 ] as well as antimicrobial agents such as peroxyacetic acid, chlorine dioxide, ozone, electrolyzed water, chlorine [ 8 ], and Essential Organic Oils (EOS) [ 9 ]. These compounds, have some benefits such as antiseptic properties and reasonable price, but raise concerns about the reaction of chlorine with organic matter and toxic properties [ 10 ]. Alternative methods such as ultrasound can be used to remove residual chemicals from agricultural products with high performance [ 11 ]. Piezoelectric ultrasound transducers have been used for this purpose, but to amplify the amplitude of the generated waves, a horn, which causes power loss, must be used [ 12 ]. Magnetostrictive materials are good alternatives to convert electrical energy to ultrasound and used in various fields such as cleaning [ 13 ], sonochemistry, industrial processes, and medicine, because they have high energy density and high response speed [ 14 ]. In order to optimize the design of these transducers at a lower cost their performance should be examined in software environments with applied effective parameters. These parameters included the number of coil turns, electrical frequency, permanent magnets position and core geometry. In fact, the fluctuations of magnetostrictive force in the longitudinal direction of the transducer are very important in the generation of ultrasonic waves. It has been shown that conical cores with an angle of 30 degrees are able to generate the maximum fluctuations along the longitudinal axis [ 15 ]. The contamination level of products should be controlled in order to assure consumer health, improve the management of agricultural resources and prevent economic losses. This evaluation is performed by the MRL (Maximum Residue Limits) index. This parameter actually determines the maximum allowable concentration of residual pesticides inside or outside food products in terms of \({\mu }g/\text{k}\text{g}\) [ 1 ]. Many methods are used to detect residual pesticides on agricultural products. These methods include gas chromatography (GC), high-performance liquid chromatography (HPLC), HPLC / GC, mass spectra (MS) [ 16 ], and enzyme-linked immunoassay (ELISA), GC-MS, liquid chromatography/ mass spectra (LC-MS) and Quadrupole Time-of-Flight Mass Spectrometry (Q-TOF MS) [ 17 ]. In order to evaluate changes in the surface quality of biological materials due to ultrasonic application, a wide range of special tools and equipment are required. One of these common methods is the scanning electron microscope (SEM). In this study, the ability of a magnetostrictive transducer equipped with a conical core, made of pure nickel in generating ultrasonic wave, to create turbulence in liquid for cleaning fruits and vegetables was evaluated. Due to the limitations of the existing load cells in measuring high-frequency forces, the performance of this transducer was evaluated by measuring its created sound pressure, using a decibel meter. The decibel meter data were then compared with the results of numerical simulation using the JMAG-Designer software. In addition, the performance of the device in creating cavitation to disperse waterproof paints in aqueous solvents was investigated by image processing. On the other hand, cucumber is one of the most widely consumed products among fruits and vegetables, widely used in salads and cold soups. Few studies have been performed on the effect of ultrasonic treatment time on cucumber washing. In this study, the amount of residual pesticide on cucumber and also the textural changes in its peel after ultrasonic treatment were investigated by GC and SEM methods, respectively. Because these changes affect the digestibility of cucumber peel and also its shelf life. 2. Materials And Methods 2.1. Manufacturing the mechanical parts of ultrasonic transducer Nickel plates with 99.99% purity (Vale Inco, Canada) were purchased and used to make the magnetostrictive core. Pure metals, have high melting temperatures which is 1455°C for nickel [ 18 ]. By some modifications on the existing induction furnace (Ferdowsi University of Mashhad, Nano Laboratory), the pure nickel was cast in the prepared mold. After casting the pure nickel in the induction furnace, the cast specimen was machined to achieve the desired dimensions of the core. The housing and cap of the device were made of 316L austenitic stainless steel. Among the characteristics of this steel are high resistance to corrosion, higher strength in high temperatures, good forming ability and high tolerance to stress [ 19 ]. The housing and its cap are responsible for compressing the inside components of transducer (core and winding). According to Fig. 1 , in order to tighten the housing cap and compress the internal parts of the transducer, a head was built on the top of the cap. As shown in this figure, polyethylene material was used to make the coil spool of device. The thickness of this spool was considered to be 5 mm to ensure enough mechanical strength in the coil during the winding process and also when applying high electrical power (due to relatively high heat) to the coil. 2.2. Electrical specifications of coil and driver circuit The operating frequency of the magnetostrictive ultrasonic transducer was set to 20 kHz [ 15 ]. In this study the inductance of the coil was compared in two different modes. Because at high frequencies, based on the skin effect, the current through the coil tends to move away from the center of the wire. Therefore, the number of parallel strands of wire should be increased as much as possible in order to increase the cross section to pass high frequency current [ 20 ]. For this purpose, a bundle of 100-strand wire with a length of 10 meters was prepared (known as Litz wire). The litz wire consisted of 0.2 wires. Then the coil was wound with the same number of turns by ordinary wire and litz wire and the results were compared. While winding the wires, insulation paper (Presspahn Limited) and air drying varnish were used to create electrical insulation and eliminate the vibrations of the wires, respectively. In pure induction circuits, the source power is used to create a magnetic field. Also in RLC circuits, if resistive, inductive and capacitive loads are in series, the resonance frequency ( \({f}_{\text{r}}\) ) is achieved when the magnetic resistance of the inductor load is equal to the capacitive resistance of the capacitive load. These circuits are called series resonant circuits. For this purpose and as seen in Fig. 2 , the driver circuit designed by Mahbodtronics Company, Iran. This circuit has a half bridge consisting of two IGBTs and also a capacitive bank which was placed in series with the magnetostrictive transducer coil. The features of this circuit include switching high currents (more than 30 amps) with high operating frequency (more than 100 kHz). The driver is powered by a 12-volt power supply to switch IGBTs and supply the required voltage to the microcontroller and the other electronic components via an LM7805 regulator. Also, a variable transformer was used to provide the required power of the magnetostrictive transducer. The operating frequency of the driver is adjusted by an ATMega8 microcontroller. As previously stated, given that the operation frequency of the transducer was considered equal to 20 kHz and the circuit inductance was equal to 74 \(\mu H\) , the capacitor bank capacitance was calculated equal to 1 \(\mu F\) . Because the resonant frequency of the driver circuit must be close to the desired operating frequency. However, due to the fact that the required current of the transducer is infinite in the resonant frequency, the operating frequency of the microcontroller should be shifted as much as 10 to 20% to the inductive area. Therefore, by using the capacitor bank, the resonant frequency of the driver circuit was adjusted to approximately 18 kHz, and to move away from the resonance zone, the operating frequency of the microcontroller, which is the operating frequency of the transducer, was set at 20 kHz. 2.3. Sound pressure measurement In magnetostrictive transducers, the fluctuations of the magnetostrictive force along the longitudinal axis is the key parameter affecting the cavitation phenomenon. Also according to the Nyquist law, the sampling rate of the generated ultrasound must be at least twice the operating frequency [ 21 ]. Due to the high operating frequency in this study (20 kHz) and the other hand, low sampling rate of the existing load cells, it was not possible to directly measure the magnetostrictive force. So the performance of the transducer was evaluated as its sound created, and the sound pressure measured from the real transducer was compared with the simulation model. So according to Fig. 2 , the ultrasonic generated by the device was measured by a decibel meter (TES-1358). The decibel meter was placed horizontally in front of the device. The electrical parameters of the transducer, were measured using a multimeter, clamp ammeter and oscilloscope which are given in Table (1). The decibel value was measured in two different modes, i.e. when the driver circuit is turned off (solely surrounding sound with no sound from transducer) and when the magnetostrictive transducer is on (surrounding sound + transducer sound). The sound level in the first and second mode was 35.6 and 66.5 decibels, respectively. In other words, by turning on the driver circuit, the decibel increased by 30.9 decibels. Table 1 Electrical specifications of coil used in the magnetostrictive transducer Wire Specification Wire Strands No. 100 Coil Specification Frequency 20 kHz Wire Diameter/Gauge 32/0.2 mm Current 5 A Wire Resistance 1.7 Ohm Voltage 78 V Inductance 74 µH 2.4. Image processing procedure to evaluate the dispersion effect of transducer In order to evaluate the performance of the device, a waterproof paint dispersion test was used. In this test, the dispersion rate of waterproof paint in water was evaluated. Image processing is a technique to monitor various processes, including monitoring the ripening of agricultural products such as mango, banana and apple in the ripening room to achieve the desired conditions [ 22 ]. In this test a drop of waterproof paint was poured at the bottom of a 50 cc glass bottle and subsequently by turning on the ultrasonic transducer, the paint dispersion process in aqueous solvent was filmed. In order to evaluate the dispersion effect of the transducer by image processing, color snapshots were captured after 10, 20, 30, 40, 50 and 60 seconds, since the paint dispersion was negligible before 10 seconds. Red, green and blue channels of the images were extracted using MATLAB software. Histogram adjustment was used to create more distinction between the background and the paint dispersed in the water. In other words, multiplication operations were used to increase color intensity [ 23 ]. After reading the images in MATLAB software environment, a suitable coefficient was selected to increase the color intensity by trial and error method, and this coefficient was applied to color images and the extracted channels. 2.5. Cucumber sampling In order to ensure the concentration of residual pesticides on the crop, cucumbers prepared from a local greenhouse located in Fariman city, where biological pesticides were used to grow this product. The variety of these cucumbers was DIVA. Their average physical dimensions, which include diameter, length and mass, were 14.1 and 27.3 mm and 70.8 gr, respectively. In this study, Diazinon pesticide was used to investigate the effects of ultrasonic treatment on reducing the residual pesticides on cucumber samples. This pesticide that is frequently used against insects on fruits and vegetables such as cucumbers, tobacco, forage as well as soil nematodes. It is also used to protect greenhouses and mushroom farms from winged insects. In addition, Diazinon is one of the organophosphorus pesticides that affects human health and is easily absorbed through the gastrointestinal tract, skin, and respiratory tract [ 24 ]. For this purpose, considering the concentration of 2 \(ml/L\) [ 24 ], the solution of Diazinon was spread evenly on the samples. The solution was sprayed by a hand sprayer with a tank capacity of 70 cc. 2.6. Ultrasonic treatment Since this transducer equipped with a nickel core with low magnetostriction effects, its ultrasonic output power is low. For this purpose, in order to increase the effect of ultrasound waves on cucumber samples, a 250 cc lab beaker was used to place two cucumbers with the ultrasonic horn. Then, each sample was treated separately by ultrasound. The ultrasonic treatment time was variable and equal to 5, 10, and 20 minutes [ 25 ]. However, due to the fact that more than 50% of the input power of these transducers is converted to heat, the propagation time of ultrasonic waves was such that every 1 minute of propagation, the power supply was cut off for 2 minutes. This time pattern was considered for cooling the nickel core and the Teflon coil spool. 2.7. Sample preparation for GC Gas chromatography was used to evaluate the changes in the amount of residual pesticide on cucumber samples. To perform this test, 4 samples including reference, 5 min, 10 min, and 20 min treatments were selected. Each sample was first crushed separately in a blender at 9000 rpm for 5 minutes and then placed in a variable-speed homogenizer. However, in order to ensure that all the cucumber pulps were crushed and prevent remaining pulps between the homogenizer blades, the blended samples were first completely crushed in a laboratory mortar and passed through filter paper. In the homogenizer, the samples were completely uniform for 2 minutes at variable speeds. The homogenized samples were transferred separately to the GC laboratory of Ferdowsi University of Mashhad in glass containers. Samples were evaluated by QuEChERS method [ 26 ]. 2.8. Sampling for SEM SEM images were used to investigate the textural changes of cucumber peel caused by the application of ultrasonic waves. To perform this test, 4 samples including reference, 5 min, 10 min, and 20 min treatments were selected. Samples were prepared biologically [ 27 ] and then SEM images were taken in Central Laboratory of Ferdowsi University of Mashhad. 3. Results And Discussion Sound pressure level was used as a measure of transducer performance. The performance of transducer was also investigated as its ability to disperse waterproof paints in aqueous solvents by image processing. Then Diazinon pesticide, which is widely used in agricultural applications including the production of cucumber, was used. After spreading Diazinon pesticide solution on cucumber products, ultrasonic treatment was applied on the samples for 5, 10 and, 20 minutes. To determine the residual pesticide and evaluate the peel texture of cucumber product, the GC and SEM methods were used respectively. 3.1. Sound pressure level test As previously stated, in order to reduce heat loss and select a suitable conductor for applying the high frequency current through the coil, the spool was wound by an ordinary wire and also Litz wire with the same number of coil turns. The purpose was to compare the performance of these two types of wirings. The results showed that the inductance of the coil with 100 turns for the coil with ordinary wire and Litz wire was 112.9 and 74 microhenry, respectively. Thus, by increasing the number of strands in the Litz wire, the resistance created at high frequencies decreases [ 28 ]. In order to compare the real transducer with the simulation model, the sound pressure was measured. This parameter has been used to evaluated the performance of ultrasonic transducers [ 29 ], [ 30 ]. The sound pressure produced is affected by the size of transducer. This increase is about three to five decibels [ 29 ]. However, due to the small size of the transducer in this study, this effect can be ignored. Figure 3 shows the sound pressure distribution of the simulated transducer using the JMAG-Designer software. In Fig. 4 the sound pressure level diagrams in three different modes is presented (simulated, real model and ambient + real model). As seen the average sound pressure level in the simulated model, the absolute sound pressure level (solely from transducer) of the real transducer and the sound pressure level of real transducer with ambient sound were 33.98, 35.6 and 66.5 dB, respectively. A slight difference (4.5%) between the sound pressure level in the simulated model and the real transducer is seen. This is mainly due to the way of calculating the sound pressure. The sound pressure in the software environment was calculated on a spherical shell with a diameter of 100 mm, while in the real transducer this was done by connecting the decibel meter directly in front of the core horn. Moreover, due to the mismatch of different properties of transducer in simulation and real model, some error is expected. Generally, in ultrasonic transducers the transmitted power and sound pressure level increase with decreasing probe distance [ 31 ]. 3.2. Evaluating dispersion ability of the magnetostrictive device By dropping the waterproof paint at the bottom of a glass bottle and applying the magnetostrictive transducer and filming the process, the color images and red, green and blue channels were extracted in the MATLAB software environment. Because high-speed imaging can determine the formation of cavitation phenomenon and the growth of cavitation clouds [ 32 ]. However, as mentioned, the scaling method was used to improve the image contrast and increase the pixel intensity. Considering that the effective coefficients can be obtained by trial and error [ 33 ], in this section a coefficient of 2 was selected to scale the images. In Fig. 5, the elapsed times are displayed in the first column and the other columns are the images extracted from different color channels. According to this figure, the right column shows the status of paint dispersion as control i.e. the glass bottle that was not treated with the ultrasonic transducer is shown. As seen, in this case after 60 seconds, the waterproof paint on the bottom of the glass bottle does not disperse and only the paint on the top of the bottle moves down. By using RGB color channels, the image features can be extracted [ 22 ]. As can be seen in this figure, and comparing the images of different color channels at 10, 40, and 60 seconds, it is observed that the images of the red color channel are clearer than the other channels and also more consistent with the RGB image. Since the images extracted from red channel were more consistent with the RGB images, the histogram of this channel was drawn for different elapsed times as shown in Fig. 6 . At 10 and 20 seconds elapsed times, which are shown in Fig. 6 .a and 6.b respectively, it is observed that the higher gray scales have a small number of pixels and the lower gray scales have less than 400 pixels, implying less dispersion of the paint. But over time at 40, 50 and, 60 seconds, which are shown in Fig. 6 .d, 6.e, and 5.f, respectively, it is observed that the number of pixels with higher gray scales has decreased to zero, but the number of pixels with lower gray scales increased to values above 1000. The evolution of pixel’s grayscale over time shows the paint dispersion process. This indicates that turbulence has occurred in the liquid due to the operation of the magnetostrictive ultrasonic transducer, which has caused the paint to spread. For further investigation and eliminating the color effects of the transducer probe in the achieved images, the space around the transducer probe was divided into 6 parts, because depending on the type of research, parts of the image that are fixed or variable can be cut and deleted or processed [ 34 ]. In other words, according to Fig. 7 , 3 parts on the right side and 3 parts on the left side of the transducer probe with the same dimensions (60 pixels wide by 50 high) were selected. The Red channel histograms data were extracted at 60 seconds and the mean value was calculated for all gray scales. By analyzing this data, it was found that the mean value (72) is related to the gray scale 41. Therefore, to calculate the percentage of surface occupied by the waterproof paint in each of the 6 parts, all pixels whose gray scale was less than 73 were counted. Because by counting the number of pixels that have a special property, the amount of the surface and its changes can be achieved [ 22 ]. Then at different elapsed times, the number of pixels was introduced as a percentage of the occupied area. According to this figure, since the dispersion of waterproof paint at the bottom of the glass bottle is non-uniform, it is observed that the cropped image at the lower end of the left side has an occupancy level of 62% at 10 seconds and at the end of 60 seconds the occupied area reaches 81%. But at the lower right side, the occupied area is initially 28% and at the end about 100%. But in the middle parts, the paint dispersion speed increases from 20 to 40 seconds, so that in 40 seconds, more than 80% of these areas are occupied by blue paint. At the upper parts, up to 40 seconds, the dispersion speed is very low (less than 40%), but it is observed that between 40 to 60 seconds, this increases rapidly so that more than 90% of these areas are occupied by blue paint. In other words, the cavitation phenomenon created by mechanical waves of the ultrasonic transducer initially creates bubbles at the lower parts. But over time, these bubbles burst and move upward to dissolve the blue paint in the middle and then the upper layers. Because over time and increasing the radius of the bubbles and reaching their critical radius and pressure, the bubbles become unstable and their density decreases, so the bubbles begin to move upwards. Also, by increasing the Reynolds number, which indicates turbulence in the fluid, tails are created on the new bubbles, which intensifies the cavitation phenomenon and increases the tendency to last longer after the disappearance of the main bubbles [ 35 ]. As a result, the magnetostrictive ultrasonic transducer causes the complete dispersion of the blue paint in the glass bottle for 60 seconds by creating the cavitation phenomenon. In general, employing image processing method is useful in studying the dynamic behavior of clouds created by cavitation phenomenon in aqueous solvents [ 36 ]. So that by using gray images, dimensional parameters such as the length of the created cavitation clouds can be measured [ 37 ]. 3.3. GC test Microorganisms are among the natural contaminants of fresh products. Observance of hygienic principles of such products is done by washing in tap water to remove residual pesticides, contaminants, plant residues and reduce the microbial load on the peel of fruits [ 38 ]. The effects of ultrasonic cleaning for 5, 10 and 20 minutes on the residual pesticide are shown in Table (2). Ultrasonic waves in water cause cavitation. Therefore, in the medium, micron-sized bubbles are formed quickly and burst. In such conditions, small explosions are created that provide the power of cleaning. According to this table, the Diazinon residue decreases with increasing time. Ultrasonic cleaning in 20 minutes has significantly reduced this pesticide. In other words, by using external standard method in GC test, the results showed that the residual pesticide based on the height of the chromatogram for the reference, 5, 10 and, 20 minutes were 1, 0.27, 0.26 and 0.25, respectively. Also, the residual pesticide based on the area under the chromatogram for the reference, 5, 10, and 20 minutes were 1, 0.21, 0.18, and 0.17, respectively. In other words, using the magnetostrictive ultrasonic transducer for 20 minutes, the residual pesticide based on the height and chromatogram area were 25% and 17%, respectively. For ultrasonic cleaning, it is assumed that the sound bubbles created by the cavitation phenomenon oscillate over the peel products at a distance of several tens of nanometers. The flow created by the bursting of the bubble can lead to tensile and shear forces over the peel. This flow will cause cleaning [ 39 ]. In a study that used ultrasonic treatment for 20 min to remove pesticides from cucumber product, the residual pesticides for Trichlorfon, Dimethoate, Dichlorvos, Fenitrothion and, Chlorpyrifos were reported 17.1%, 47.8%, 50.2%, 15.6%, and, 37%, respectively [ 25 ]. Also, in another study that used piezoelectric transducers with variable powers and times for tomato product, the results showed that by considering 300 watts and 15 minutes, the residual pesticide for DDVP was 89% [ 40 ]. Probably, the small volume of the lab beaker and also considering the 2-minute interval for each one-minute treatment are the main reasons that have improved the results of this study compared to other studies. Because according to table (1), by applying ultrasonic waves for 5 minutes, the reduction of Diazinon pesticide was more than 73%. On the other hand, in the ultrasonic bath, the power level is not high enough because the transducer vibrations enter the tank through a metal wall. Therefore, sound waves form a sustainable wave pattern in the tank and the distribution of the ultrasonic field is not uniform. But the uniformity of this distribution in a probe system is less than in an ultrasonic bath. So that intense vibrations occur at the tip of the probe, causing a hole or corrosion in the metal probe [ 39 ]. Table 2 GC test results for different treatment times on cucumber Sample Elapsed Time (min) HBR * Reduction (%) ABR ** Reduction (%) Reference - 1 - 1 - No. 1 5 0.27 73 0.21 79 No. 2 10 0.26 74 0.18 82 No. 3 20 0.25 75 0.17 83 * Height Based Results ** Area Based Results 3.4. SEM imaging The micro-images of the middle part of the cucumber were selected for measuring the dimensions of the peel features. All SEM images were taken at 2500 magnification and working distance of 8 mm. According to Fig. 8, the peel features of the cucumber product such as stomatal pores were observed by SEM images. In other words, the stomatal pores and their guard cells that are elliptic were evaluated. Stomatal pores are involved in the gas exchange of many fruits and vegetables such as cucumber, and are embedded in the epidermis for several microns [ 27 ]. As can be seen in this figure, by increasing the time of ultrasonic treatment, the opening area of stomatal pores decreases so that the highest opening area is related to the reference (Fig. 8.a) and the lowest opening area is related to the 20 min treatment (Fig. 8.d). The results of a study showed that by applying ultrasound for 2 min on the surface of the recalcitrant squash cotyledon, the stomatal pores and Ridges of the guard cells were still in place. But after 10 min, the edges of the guard cells and the surrounding areas were smoothed. After 30 minutes, Severe peel damage was observed so that epidermal cells and stomatal pores were damaged, and also large cracks were observed on the peel surface [ 41 ]. As mentioned, ultrasonic waves not only clean the cucumber product, but also close the stomatal pores, and this will probably increase the shelf life of the product without affecting the content of organic and mineral materials as well as mechanical properties. Because according to the researches, the ultrasonic treatment of cherry tomatoes, strawberries and palm fruits has almost doubled the shelf life without affecting their contents [ 42 ]. Also, according to Fig. 8, it is observed that with increasing treatment time, the peel texture of the cucumber product has been worn. So that by increasing this time, the depth of cavities on the cucumber peel has decreased and the pitting wall thickness has increased. The color uniformity in the 20 min treatment (Fig. 8.d) compared to the 5 min treatment (Fig. 8.b) justifies this peel erosion. The results of a study showed that by applying ultrasound for 2 min on the surface of the recalcitrant squash cotyledon, the surface of the epidermal cell in the reference was higher than the cell junctions. By applying ultrasonic treatment for 2 minutes, the surface of the epidermal cell and the cell junctions were disproportionately worn. By increasing the treatment time for 10 minutes, this erosion increased so that the surface of the epidermal cell was approximately equal to the cell junctions [ 41 ]. Ultrasound produces intense pressure, shear force and temperature gradient in the material, which cause mechanical rupture in the texture. In other words, by propagation sound energy, which is mechanical oscillations, through the medium, three types of waves are created, which are: (1) longitudinal waves that move in the direction of displacement (2) shear waves that are perpendicular to the wave main motion (3) Rayleigh waves that travel very close to the material surface. Therefore, these three types of waves create alternating expansions and contractions. During these cycles, millions of small bubbles form that grow by absorbing energy from the medium, and when they cannot absorb more energy, they become unstable and burst violently. This releases a large amount of energy known as cavitation. A bubble can burst at or near the top of a cell wall. When this happens above the cell surface, it can potentially cause cavities in the cell wall [ 42 ]. On the other hand, the bursting of bubbles created by transient cavitation causes serious physical conditions. These conditions include high temperature (up to 5000 K), high pressure (up to 1000 atm), high rate of cooling and heating (up to 1010 \(K/s\) ), shock waveforms, and high-speed water jet (156 \(km/h\) ) [ 39 ]. Photoshop software was used to investigate the effects of ultrasonic mechanical waves on the peel texture of cucumber products accurately. In other words, the dimensions of the stomatal pores, the Guard cell wall thickness, and pitting wall thickness were calculated using the scaling method. Since the stomatal pores are ellipsoid, the area of these pores can be calculated using the ellipsoid area equation. where in this equation, A, a, and b are the stomatal pore area, the major diameter of the ellipse, the minor diameter of the ellipse [ 27 ]. Based on the effects of the cavitation phenomenon and what was mentioned above, according to Fig. 9 by increasing the treatment time, the stomatal pore area reduced from 144.74 \({\mu m}^{2}\) (reference) to 30.56 \({\mu m}^{2}\) (20 min treatment). Also, the guard cell wall thickness increased from 1.49 µm (reference) to 4.16 µm. But according to this figure, the increasing trend of guard cell wall thickness is ascendant for 10 minutes and then is almost constant. This trend may be due to the higher location of guard cells relative to the epidermis and also the lower thickness of the guard cell walls relative to the wall thickness of the epidermis cells. This increases the erosion process speed in the early minutes. Then the guard cell wall thickness increases due to erosion and the cell height become equal to epidermis cells and as a result, the increasing trend of the guard cell wall thickness or erosion speed decreases. In addition, the epidermis wall thickness increased from 2.20 µm (reference) to 4.78 µm (20 min treatment). According to this figure, the increasing trend of the Epidermis cell wall thickness is still ascendant. Therefore, by increasing ultrasonic treatment time, significant peeling will be done in the cucumber samples. Conclusion In this research a magnetostrictive ultrasonic transducer was built and its ability in creating cavitation in fluid (for cleaning of delicate fruits and vegetables) due to its generated mechanical waves was evaluated. Based on the previous finding, a conical core made of pure nickel (as an abundantly available, less expensive, less hazardous material) with a cone angle of 30 degrees was used. The results showed that the sound pressure of the simulated model and the real transducer are almost the same. In addition, the ability of the transducer to disperse waterproof paints in aqueous solvent was evaluated by image processing method. Comparing the red, green and blue channels with the RGB image, it was observed that the red channel is able to display more details of the RGB image. The results showed that the transducer is able to disperse more than 90% of waterproof paints in the glass bottle after 60 seconds. It was also observed that the cavitation phenomenon initially moves the paint at the bottom of the glass bottle and then causes to spread the paint towards the middle layers and finally in the upper layers. In addition, the GC test results showed that the residual pesticide based on the height and chromatogram area were 75% and 83%, respectively. Also, by increasing the treatment time, the stomatal pore area decreases so that the maximum opening area was observed in the reference and the minimum area for the sample of 20 min treatment time. By increasing the treatment time, the peel texture of cucumber is worn so that the epidermis cell depth decreased and the epidermis wall thickness. This erosion can be justified by comparing the color uniformity in the 20 min treatment and the 5 min treatment. However, as mentioned, one of the challenges of this study is the low effect of magnetostrictive nickel core. So a small lab beaker (250 cc) was selected to place two cucumbers with the ultrasonic horn. For future research, it is suggested that the effects of increasing the number of transducers and increasing the horn length in large container be investigated. Declarations Acknowledgements The authors acknowledge and appreciate the funding and technical supports provided by the Ferdowsi University of Mashhad, Iran for this project. Funding: This study was funded by Ferdowsi University of Mashhad (FUM), (grant number 46420). Conflict of Interest: The authors declare that they have no conflict of interest. Data Availability Statement: All data generated or analysed during this study are included in this published article. Also, more information is available from the corresponding author on request. Author Contributions Statement: Dr. Danial Gandomzadeh and Mrs. Yeganeh Sabeghi conceived the presented idea. Mr. Soheil Movahed Fakhr developed the theory and performed the computations. Prof. Mohammad Hossein Abbaspour-Fard verified the analytical methods. All authors discussed the results and contributed to the final manuscript. References T. M. Mac Loughlin et al. , “Pesticide residues in fruits and vegetables of the argentine domestic market: Occurrence and quality,” Food Control, vol. 93, pp. 129–138, Nov. 2018, doi: 10.1016/j.foodcont.2018.05.041 . M. R. Tapia et al. , “Washing, peeling and cutting of fresh-cut fruits and vegetables,” in Food Engineering Series , Springer, 2015, pp. 57–78. B. Wang, C. Venkitasamy, F. Zhang, L. Zhao, R. Khir, and Z. Pan, “Feasibility of jujube peeling using novel infrared radiation heating technology,” LWT - Food Sci. 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Fava, K. Hodara, A. Nieto, S. Guerrero, S. M. Alzamora, and M. A. Castro, “Structure (micro, ultra, nano), color and mechanical properties of Vitis labrusca L. (grape berry) fruits treated by hydrogen peroxide, UV-C irradiation and ultrasound,” Food Res. Int. , vol. 44, no. 9, pp. 2938–2948, Nov. 2011, doi: 10.1016/j.foodres.2011.06.053 . H. Lee, B. Zhou, and H. Feng, “Power Ultrasound Treatment of Fruits and Fruit Products,” in Food Engineering Series , Springer, 2018, pp. 311–333. A. Heshmati and F. Nazemi, “Dichlorvos (Ddvp) residue removal from tomato by washing with tap and ozone water, a commercial detergent solution and ultrasonic cleaner,” Food Sci. Technol., vol. 38, no. 3, pp. 441–446, Jul. 2018, doi: 10.1590/1678-457x.07617 . G. Ananthakrishnan et al. , “Ultrasonic treatment stimulates multiple shoot regeneration and explant enlargement in recalcitrant squash cotyledon explants in vitro,” Plant Cell Rep. , vol. 26, no. 3, pp. 267–276, Mar. 2007, doi: 10.1007/s00299-006-0235-1 . E. Montalvo-González, L. M. Anaya-Esparza, J. Abraham Domínguez-Avila, and G. A. González-Aguilar, “Ultrasonic Processing Technology for Postharvest Disinfection,” in Postharvest Disinfection of Fruits and Vegetables , Elsevier, 2018, pp. 101–119. Additional Declarations No competing interests reported. Supplementary Files GraphicalAbstract.jpg Highlights.docx Cite Share Download PDF Status: Under Review Version 1 posted Editorial decision: Major revision 05 Sep, 2022 Editor assigned by journal 05 Sep, 2022 Submission checks completed at journal 04 Sep, 2022 First submitted to journal 29 Aug, 2022 You are reading this latest preprint version Research Square lets you share your work early, gain feedback from the community, and start making changes to your manuscript prior to peer review in a journal. As a division of Research Square Company, we’re committed to making research communication faster, fairer, and more useful. We do this by developing innovative software and high quality services for the global research community. Our growing team is made up of researchers and industry professionals working together to solve the most critical problems facing scientific publishing. Also discoverable on Platform About Our Team In Review Editorial Policies Advisory Board Help Center Resources Author Services Accessibility API Access RSS feed Manage Cookie Preferences © Research Square 2026 | ISSN 2693-5015 (online) Privacy Policy Terms of Service Do Not Sell My Personal Information {"props":{"pageProps":{"initialData":{"identity":"rs-2009995","acceptedTermsAndConditions":true,"allowDirectSubmit":false,"archivedVersions":[],"articleType":"Research Article","associatedPublications":[],"authors":[{"id":134067159,"identity":"cf2e83f5-2089-459a-9f69-d24225a4f707","order_by":0,"name":"Danial Gandomzadeh","email":"","orcid":"","institution":"Ferdowsi University of Mashhad","correspondingAuthor":false,"prefix":"","firstName":"Danial","middleName":"","lastName":"Gandomzadeh","suffix":""},{"id":134067161,"identity":"d3ebef05-21fd-4420-8364-5cfac3215c37","order_by":1,"name":"Mohammad Hossein 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transducer\u003c/p\u003e","description":"","filename":"F1.png","url":"https://assets-eu.researchsquare.com/files/rs-2009995/v1/aad530c131f95279b9839540.png"},{"id":26211804,"identity":"76bac61e-fa88-4bba-af4e-b701f3adbb1f","added_by":"auto","created_at":"2022-09-08 14:44:41","extension":"png","order_by":2,"title":"Figure 2","display":"","copyAsset":false,"role":"figure","size":170588,"visible":true,"origin":"","legend":"\u003cp\u003eSound pressure measurement setup including the driver circuit and measuring devices\u003c/p\u003e","description":"","filename":"F2.png","url":"https://assets-eu.researchsquare.com/files/rs-2009995/v1/289024b815ef1ca0618a605f.png"},{"id":26210325,"identity":"1fe93ba0-4cc7-4000-8f8d-c4562bab1c9d","added_by":"auto","created_at":"2022-09-08 14:34:41","extension":"png","order_by":3,"title":"Figure 3","display":"","copyAsset":false,"role":"figure","size":48370,"visible":true,"origin":"","legend":"\u003cp\u003eThe generated sound pressure level on a spherical 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dispersion evolution, extracted from different color channels\u003c/p\u003e","description":"","filename":"F5.png","url":"https://assets-eu.researchsquare.com/files/rs-2009995/v1/1126a9ae86d393846e8651d3.png"},{"id":26210332,"identity":"13f63f06-85a8-4150-95e0-790279c434cf","added_by":"auto","created_at":"2022-09-08 14:34:42","extension":"png","order_by":6,"title":"Figure 6","display":"","copyAsset":false,"role":"figure","size":22361,"visible":true,"origin":"","legend":"\u003cp\u003eRed channel histogram at different elapsed times of applying the paint: (a) 10 seconds, (b) 20 seconds, (c) 30 seconds, (d) 40 seconds, (e) 50 seconds and (f) 60 seconds\u003c/p\u003e","description":"","filename":"F6.png","url":"https://assets-eu.researchsquare.com/files/rs-2009995/v1/45050868753fd815b2da9429.png"},{"id":26211805,"identity":"4493d58f-1bdc-462f-977b-ff83c886cd5a","added_by":"auto","created_at":"2022-09-08 14:44:42","extension":"png","order_by":7,"title":"Figure 7","display":"","copyAsset":false,"role":"figure","size":120799,"visible":true,"origin":"","legend":"\u003cp\u003eCropping the areas around the magnetostrictive ultrasonic probe into 6 parts with the same dimensions (60 pixels wide by 50 high). 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Introduction","content":"\u003cp\u003eIn recent years, ultrasonic machining has developed rapidly. It has been used in applications such as ultrasonic abrasive machining, cleaning and welding. Fruits and vegetables contain important nutrients that are essential for human health. But agricultural pesticides are widely used to protect products against insects, diseases and maximizing crop yields. Residual pesticides have been considered in terms of their effects on human health as well as environmental effects. Because these pesticides cause diseases such as cancer and reproductive endocrine disorders [\u003cspan citationid=\"CR1\" class=\"CitationRef\"\u003e1\u003c/span\u003e].\u003c/p\u003e \u003cp\u003eIn general, different methods are used for peeling and cleaning agricultural products including: manual, mechanical, chemical, enzymatic, and thermal [\u003cspan citationid=\"CR2\" class=\"CitationRef\"\u003e2\u003c/span\u003e]. Conventional, mechanical, chemical methods and immersion in hot water cause adverse effects on the product [\u003cspan citationid=\"CR3\" class=\"CitationRef\"\u003e3\u003c/span\u003e]. Alkaline solution or steam pressure can also be used for this purpose. However, these methods have some disadvantages such as excessive water and chemical consumptions, high cost, as well as problems related to peeling waste [\u003cspan citationid=\"CR4\" class=\"CitationRef\"\u003e4\u003c/span\u003e]. In addition, infrared (IR) [\u003cspan citationid=\"CR5\" class=\"CitationRef\"\u003e5\u003c/span\u003e] and ultraviolet (UV) radiations [\u003cspan citationid=\"CR6\" class=\"CitationRef\"\u003e6\u003c/span\u003e], [\u003cspan citationid=\"CR7\" class=\"CitationRef\"\u003e7\u003c/span\u003e] can be used for peeling and cleaning agricultural products. Chemical methods use natural acids such as aceticacid, benzoicacid, citricacid, malicacid, sorbicacid, succinicacid, and tartaricacid [\u003cspan citationid=\"CR2\" class=\"CitationRef\"\u003e2\u003c/span\u003e] as well as antimicrobial agents such as peroxyacetic acid, chlorine dioxide, ozone, electrolyzed water, chlorine [\u003cspan citationid=\"CR8\" class=\"CitationRef\"\u003e8\u003c/span\u003e], and Essential Organic Oils (EOS) [\u003cspan citationid=\"CR9\" class=\"CitationRef\"\u003e9\u003c/span\u003e]. These compounds, have some benefits such as antiseptic properties and reasonable price, but raise concerns about the reaction of chlorine with organic matter and toxic properties [\u003cspan citationid=\"CR10\" class=\"CitationRef\"\u003e10\u003c/span\u003e]. Alternative methods such as ultrasound can be used to remove residual chemicals from agricultural products with high performance [\u003cspan citationid=\"CR11\" class=\"CitationRef\"\u003e11\u003c/span\u003e]. Piezoelectric ultrasound transducers have been used for this purpose, but to amplify the amplitude of the generated waves, a horn, which causes power loss, must be used [\u003cspan citationid=\"CR12\" class=\"CitationRef\"\u003e12\u003c/span\u003e]. Magnetostrictive materials are good alternatives to convert electrical energy to ultrasound and used in various fields such as cleaning [\u003cspan citationid=\"CR13\" class=\"CitationRef\"\u003e13\u003c/span\u003e], sonochemistry, industrial processes, and medicine, because they have high energy density and high response speed [\u003cspan citationid=\"CR14\" class=\"CitationRef\"\u003e14\u003c/span\u003e]. In order to optimize the design of these transducers at a lower cost their performance should be examined in software environments with applied effective parameters. These parameters included the number of coil turns, electrical frequency, permanent magnets position and core geometry. In fact, the fluctuations of magnetostrictive force in the longitudinal direction of the transducer are very important in the generation of ultrasonic waves. It has been shown that conical cores with an angle of 30 degrees are able to generate the maximum fluctuations along the longitudinal axis [\u003cspan citationid=\"CR15\" class=\"CitationRef\"\u003e15\u003c/span\u003e].\u003c/p\u003e \u003cp\u003eThe contamination level of products should be controlled in order to assure consumer health, improve the management of agricultural resources and prevent economic losses. This evaluation is performed by the MRL (Maximum Residue Limits) index. This parameter actually determines the maximum allowable concentration of residual pesticides inside or outside food products in terms of \u003cspan class=\"InlineEquation\"\u003e\u003cspan class=\"mathinline\"\u003e\\({\\mu }g/\\text{k}\\text{g}\\)\u003c/span\u003e\u003c/span\u003e [\u003cspan citationid=\"CR1\" class=\"CitationRef\"\u003e1\u003c/span\u003e]. Many methods are used to detect residual pesticides on agricultural products. These methods include gas chromatography (GC), high-performance liquid chromatography (HPLC), HPLC / GC, mass spectra (MS) [\u003cspan citationid=\"CR16\" class=\"CitationRef\"\u003e16\u003c/span\u003e], and enzyme-linked immunoassay (ELISA), GC-MS, liquid chromatography/ mass spectra (LC-MS) and Quadrupole Time-of-Flight Mass Spectrometry (Q-TOF MS) [\u003cspan citationid=\"CR17\" class=\"CitationRef\"\u003e17\u003c/span\u003e]. In order to evaluate changes in the surface quality of biological materials due to ultrasonic application, a wide range of special tools and equipment are required. One of these common methods is the scanning electron microscope (SEM).\u003c/p\u003e \u003cp\u003eIn this study, the ability of a magnetostrictive transducer equipped with a conical core, made of pure nickel in generating ultrasonic wave, to create turbulence in liquid for cleaning fruits and vegetables was evaluated. Due to the limitations of the existing load cells in measuring high-frequency forces, the performance of this transducer was evaluated by measuring its created sound pressure, using a decibel meter. The decibel meter data were then compared with the results of numerical simulation using the JMAG-Designer software. In addition, the performance of the device in creating cavitation to disperse waterproof paints in aqueous solvents was investigated by image processing. On the other hand, cucumber is one of the most widely consumed products among fruits and vegetables, widely used in salads and cold soups. Few studies have been performed on the effect of ultrasonic treatment time on cucumber washing. In this study, the amount of residual pesticide on cucumber and also the textural changes in its peel after ultrasonic treatment were investigated by GC and SEM methods, respectively. Because these changes affect the digestibility of cucumber peel and also its shelf life.\u003c/p\u003e"},{"header":"2. Materials And Methods","content":"\u003cdiv id=\"Sec3\" class=\"Section2\"\u003e \u003ch2\u003e2.1. Manufacturing the mechanical parts of ultrasonic transducer\u003c/h2\u003e \u003cp\u003eNickel plates with 99.99% purity (Vale Inco, Canada) were purchased and used to make the magnetostrictive core. Pure metals, have high melting temperatures which is 1455\u0026deg;C for nickel [\u003cspan citationid=\"CR18\" class=\"CitationRef\"\u003e18\u003c/span\u003e]. By some modifications on the existing induction furnace (Ferdowsi University of Mashhad, Nano Laboratory), the pure nickel was cast in the prepared mold. After casting the pure nickel in the induction furnace, the cast specimen was machined to achieve the desired dimensions of the core. The housing and cap of the device were made of 316L austenitic stainless steel. Among the characteristics of this steel are high resistance to corrosion, higher strength in high temperatures, good forming ability and high tolerance to stress [\u003cspan citationid=\"CR19\" class=\"CitationRef\"\u003e19\u003c/span\u003e]. The housing and its cap are responsible for compressing the inside components of transducer (core and winding). According to Fig.\u0026nbsp;\u003cspan refid=\"Fig1\" class=\"InternalRef\"\u003e1\u003c/span\u003e, in order to tighten the housing cap and compress the internal parts of the transducer, a head was built on the top of the cap. As shown in this figure, polyethylene material was used to make the coil spool of device. The thickness of this spool was considered to be 5 mm to ensure enough mechanical strength in the coil during the winding process and also when applying high electrical power (due to relatively high heat) to the coil.\u003c/p\u003e \u003cp\u003e \u003c/p\u003e \u003c/div\u003e \u003cdiv id=\"Sec4\" class=\"Section2\"\u003e \u003ch2\u003e2.2. Electrical specifications of coil and driver circuit\u003c/h2\u003e \u003cp\u003eThe operating frequency of the magnetostrictive ultrasonic transducer was set to 20 kHz [\u003cspan citationid=\"CR15\" class=\"CitationRef\"\u003e15\u003c/span\u003e]. In this study the inductance of the coil was compared in two different modes. Because at high frequencies, based on the skin effect, the current through the coil tends to move away from the center of the wire. Therefore, the number of parallel strands of wire should be increased as much as possible in order to increase the cross section to pass high frequency current [\u003cspan citationid=\"CR20\" class=\"CitationRef\"\u003e20\u003c/span\u003e]. For this purpose, a bundle of 100-strand wire with a length of 10 meters was prepared (known as Litz wire). The litz wire consisted of 0.2 wires. Then the coil was wound with the same number of turns by ordinary wire and litz wire and the results were compared. While winding the wires, insulation paper (Presspahn Limited) and air drying varnish were used to create electrical insulation and eliminate the vibrations of the wires, respectively.\u003c/p\u003e \u003cp\u003eIn pure induction circuits, the source power is used to create a magnetic field. Also in RLC circuits, if resistive, inductive and capacitive loads are in series, the resonance frequency (\u003cspan class=\"InlineEquation\"\u003e\u003cspan class=\"mathinline\"\u003e\\({f}_{\\text{r}}\\)\u003c/span\u003e\u003c/span\u003e) is achieved when the magnetic resistance of the inductor load is equal to the capacitive resistance of the capacitive load. These circuits are called series resonant circuits. For this purpose and as seen in Fig.\u0026nbsp;\u003cspan refid=\"Fig2\" class=\"InternalRef\"\u003e2\u003c/span\u003e, the driver circuit designed by Mahbodtronics Company, Iran. This circuit has a half bridge consisting of two IGBTs and also a capacitive bank which was placed in series with the magnetostrictive transducer coil. The features of this circuit include switching high currents (more than 30 amps) with high operating frequency (more than 100 kHz). The driver is powered by a 12-volt power supply to switch IGBTs and supply the required voltage to the microcontroller and the other electronic components via an LM7805 regulator. Also, a variable transformer was used to provide the required power of the magnetostrictive transducer. The operating frequency of the driver is adjusted by an ATMega8 microcontroller. As previously stated, given that the operation frequency of the transducer was considered equal to 20 kHz and the circuit inductance was equal to 74\u003cspan class=\"InlineEquation\"\u003e\u003cspan class=\"mathinline\"\u003e\\(\\mu H\\)\u003c/span\u003e\u003c/span\u003e, the capacitor bank capacitance was calculated equal to 1 \u003cspan class=\"InlineEquation\"\u003e\u003cspan class=\"mathinline\"\u003e\\(\\mu F\\)\u003c/span\u003e\u003c/span\u003e. Because the resonant frequency of the driver circuit must be close to the desired operating frequency. However, due to the fact that the required current of the transducer is infinite in the resonant frequency, the operating frequency of the microcontroller should be shifted as much as 10 to 20% to the inductive area. Therefore, by using the capacitor bank, the resonant frequency of the driver circuit was adjusted to approximately 18 kHz, and to move away from the resonance zone, the operating frequency of the microcontroller, which is the operating frequency of the transducer, was set at 20 kHz.\u003c/p\u003e \u003c/div\u003e \u003cdiv id=\"Sec5\" class=\"Section2\"\u003e \u003ch2\u003e2.3. Sound pressure measurement\u003c/h2\u003e \u003cp\u003eIn magnetostrictive transducers, the fluctuations of the magnetostrictive force along the longitudinal axis is the key parameter affecting the cavitation phenomenon. Also according to the Nyquist law, the sampling rate of the generated ultrasound must be at least twice the operating frequency [\u003cspan citationid=\"CR21\" class=\"CitationRef\"\u003e21\u003c/span\u003e]. Due to the high operating frequency in this study (20 kHz) and the other hand, low sampling rate of the existing load cells, it was not possible to directly measure the magnetostrictive force. So the performance of the transducer was evaluated as its sound created, and the sound pressure measured from the real transducer was compared with the simulation model. So according to Fig.\u0026nbsp;\u003cspan refid=\"Fig2\" class=\"InternalRef\"\u003e2\u003c/span\u003e, the ultrasonic generated by the device was measured by a decibel meter (TES-1358). The decibel meter was placed horizontally in front of the device.\u003c/p\u003e \u003cp\u003e \u003c/p\u003e \u003cp\u003eThe electrical parameters of the transducer, were measured using a multimeter, clamp ammeter and oscilloscope which are given in Table\u0026nbsp;(1). The decibel value was measured in two different modes, i.e. when the driver circuit is turned off (solely surrounding sound with no sound from transducer) and when the magnetostrictive transducer is on (surrounding sound\u0026thinsp;+\u0026thinsp;transducer sound). The sound level in the first and second mode was 35.6 and 66.5 decibels, respectively. In other words, by turning on the driver circuit, the decibel increased by 30.9 decibels.\u003c/p\u003e \u003cp\u003e \u003cdiv class=\"gridtable\"\u003e\u003ctable float=\"Yes\" id=\"Tab1\" border=\"1\"\u003e \u003ccaption language=\"En\"\u003e \u003cdiv class=\"CaptionNumber\"\u003eTable 1\u003c/div\u003e \u003cdiv class=\"CaptionContent\"\u003e \u003cp\u003eElectrical specifications of coil used in the magnetostrictive transducer\u003c/p\u003e \u003c/div\u003e \u003c/caption\u003e \u003ccolgroup cols=\"6\"\u003e \u003cdiv align=\"left\" class=\"colspec\" colname=\"c1\" colnum=\"1\"\u003e\u003c/div\u003e \u003cdiv align=\"left\" class=\"colspec\" colname=\"c2\" colnum=\"2\"\u003e\u003c/div\u003e \u003cdiv align=\"left\" class=\"colspec\" colname=\"c3\" colnum=\"3\"\u003e\u003c/div\u003e \u003cdiv align=\"left\" class=\"colspec\" colname=\"c4\" colnum=\"4\"\u003e\u003c/div\u003e \u003cdiv align=\"left\" class=\"colspec\" colname=\"c5\" colnum=\"5\"\u003e\u003c/div\u003e \u003cdiv align=\"left\" class=\"colspec\" colname=\"c6\" colnum=\"6\"\u003e\u003c/div\u003e \u003ctbody\u003e \u003ctr\u003e \u003ctd align=\"left\" colname=\"c1\" morerows=\"3\" rowspan=\"4\"\u003e \u003cp\u003eWire Specification\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c2\"\u003e \u003cp\u003eWire Strands No.\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c3\"\u003e \u003cp\u003e100\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c4\" morerows=\"2\" rowspan=\"3\"\u003e \u003cp\u003eCoil Specification\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c5\"\u003e \u003cp\u003eFrequency\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c6\"\u003e \u003cp\u003e20 kHz\u003c/p\u003e \u003c/td\u003e \u003c/tr\u003e \u003ctr\u003e \u003ctd align=\"left\" colname=\"c2\"\u003e \u003cp\u003eWire Diameter/Gauge\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c3\"\u003e \u003cp\u003e32/0.2 mm\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c5\"\u003e \u003cp\u003eCurrent\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c6\"\u003e \u003cp\u003e5 A\u003c/p\u003e \u003c/td\u003e \u003c/tr\u003e \u003ctr\u003e \u003ctd align=\"left\" colname=\"c2\"\u003e \u003cp\u003eWire Resistance\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c3\"\u003e \u003cp\u003e1.7 Ohm\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c5\"\u003e \u003cp\u003eVoltage\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c6\"\u003e \u003cp\u003e78 V\u003c/p\u003e \u003c/td\u003e \u003c/tr\u003e \u003ctr\u003e \u003ctd align=\"left\" colname=\"c2\"\u003e \u003cp\u003eInductance\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c3\"\u003e \u003cp\u003e74 \u0026micro;H\u003c/p\u003e \u003c/td\u003e \u003ctd align=\"left\" colname=\"c4\"\u003e\u0026nbsp;\u003c/td\u003e \u003ctd align=\"left\" colname=\"c5\"\u003e\u0026nbsp;\u003c/td\u003e \u003ctd align=\"left\" colname=\"c6\"\u003e\u0026nbsp;\u003c/td\u003e \u003c/tr\u003e \u003c/tbody\u003e \u003c/colgroup\u003e \u003c/table\u003e\u003c/div\u003e \u003c/p\u003e \u003c/div\u003e \u003cdiv id=\"Sec6\" class=\"Section2\"\u003e \u003ch2\u003e2.4. Image processing procedure to evaluate the dispersion effect of transducer\u003c/h2\u003e \u003cp\u003eIn order to evaluate the performance of the device, a waterproof paint dispersion test was used. In this test, the dispersion rate of waterproof paint in water was evaluated. Image processing is a technique to monitor various processes, including monitoring the ripening of agricultural products such as mango, banana and apple in the ripening room to achieve the desired conditions [\u003cspan citationid=\"CR22\" class=\"CitationRef\"\u003e22\u003c/span\u003e]. In this test a drop of waterproof paint was poured at the bottom of a 50 cc glass bottle and subsequently by turning on the ultrasonic transducer, the paint dispersion process in aqueous solvent was filmed. In order to evaluate the dispersion effect of the transducer by image processing, color snapshots were captured after 10, 20, 30, 40, 50 and 60 seconds, since the paint dispersion was negligible before 10 seconds. Red, green and blue channels of the images were extracted using MATLAB software. Histogram adjustment was used to create more distinction between the background and the paint dispersed in the water. In other words, multiplication operations were used to increase color intensity [\u003cspan citationid=\"CR23\" class=\"CitationRef\"\u003e23\u003c/span\u003e]. After reading the images in MATLAB software environment, a suitable coefficient was selected to increase the color intensity by trial and error method, and this coefficient was applied to color images and the extracted channels.\u003c/p\u003e \u003c/div\u003e \u003cdiv id=\"Sec7\" class=\"Section2\"\u003e \u003ch2\u003e2.5. Cucumber sampling\u003c/h2\u003e \u003cp\u003eIn order to ensure the concentration of residual pesticides on the crop, cucumbers prepared from a local greenhouse located in Fariman city, where biological pesticides were used to grow this product. The variety of these cucumbers was DIVA. Their average physical dimensions, which include diameter, length and mass, were 14.1 and 27.3 mm and 70.8 gr, respectively. In this study, Diazinon pesticide was used to investigate the effects of ultrasonic treatment on reducing the residual pesticides on cucumber samples. This pesticide that is frequently used against insects on fruits and vegetables such as cucumbers, tobacco, forage as well as soil nematodes. It is also used to protect greenhouses and mushroom farms from winged insects. In addition, Diazinon is one of the organophosphorus pesticides that affects human health and is easily absorbed through the gastrointestinal tract, skin, and respiratory tract [\u003cspan citationid=\"CR24\" class=\"CitationRef\"\u003e24\u003c/span\u003e]. For this purpose, considering the concentration of 2 \u003cspan class=\"InlineEquation\"\u003e\u003cspan class=\"mathinline\"\u003e\\(ml/L\\)\u003c/span\u003e\u003c/span\u003e [\u003cspan citationid=\"CR24\" class=\"CitationRef\"\u003e24\u003c/span\u003e], the solution of Diazinon was spread evenly on the samples. The solution was sprayed by a hand sprayer with a tank capacity of 70 cc.\u003c/p\u003e \u003c/div\u003e \u003cdiv id=\"Sec8\" class=\"Section2\"\u003e \u003ch2\u003e2.6. Ultrasonic treatment\u003c/h2\u003e \u003cp\u003eSince this transducer equipped with a nickel core with low magnetostriction effects, its ultrasonic output power is low. For this purpose, in order to increase the effect of ultrasound waves on cucumber samples, a 250 cc lab beaker was used to place two cucumbers with the ultrasonic horn. Then, each sample was treated separately by ultrasound. The ultrasonic treatment time was variable and equal to 5, 10, and 20 minutes [\u003cspan citationid=\"CR25\" class=\"CitationRef\"\u003e25\u003c/span\u003e]. However, due to the fact that more than 50% of the input power of these transducers is converted to heat, the propagation time of ultrasonic waves was such that every 1 minute of propagation, the power supply was cut off for 2 minutes. This time pattern was considered for cooling the nickel core and the Teflon coil spool.\u003c/p\u003e \u003c/div\u003e \u003cdiv id=\"Sec9\" class=\"Section2\"\u003e \u003ch2\u003e2.7. Sample preparation for GC\u003c/h2\u003e \u003cp\u003eGas chromatography was used to evaluate the changes in the amount of residual pesticide on cucumber samples. To perform this test, 4 samples including reference, 5 min, 10 min, and 20 min treatments were selected. Each sample was first crushed separately in a blender at 9000 rpm for 5 minutes and then placed in a variable-speed homogenizer. However, in order to ensure that all the cucumber pulps were crushed and prevent remaining pulps between the homogenizer blades, the blended samples were first completely crushed in a laboratory mortar and passed through filter paper. In the homogenizer, the samples were completely uniform for 2 minutes at variable speeds. The homogenized samples were transferred separately to the GC laboratory of Ferdowsi University of Mashhad in glass containers. Samples were evaluated by QuEChERS method [\u003cspan citationid=\"CR26\" class=\"CitationRef\"\u003e26\u003c/span\u003e].\u003c/p\u003e \u003c/div\u003e \u003cdiv id=\"Sec10\" class=\"Section2\"\u003e \u003ch2\u003e2.8. Sampling for SEM\u003c/h2\u003e \u003cp\u003eSEM images were used to investigate the textural changes of cucumber peel caused by the application of ultrasonic waves. To perform this test, 4 samples including reference, 5 min, 10 min, and 20 min treatments were selected. Samples were prepared biologically [\u003cspan citationid=\"CR27\" class=\"CitationRef\"\u003e27\u003c/span\u003e] and then SEM images were taken in Central Laboratory of Ferdowsi University of Mashhad.\u003c/p\u003e \u003c/div\u003e"},{"header":"3. Results And Discussion","content":"\u003cp\u003eSound pressure level was used as a measure of transducer performance. The performance of transducer was also investigated as its ability to disperse waterproof paints in aqueous solvents by image processing. Then Diazinon pesticide, which is widely used in agricultural applications including the production of cucumber, was used. After spreading Diazinon pesticide solution on cucumber products, ultrasonic treatment was applied on the samples for 5, 10 and, 20 minutes. To determine the residual pesticide and evaluate the peel texture of cucumber product, the GC and SEM methods were used respectively.\u003c/p\u003e\n\u003cdiv class=\"Section2\" id=\"Sec12\"\u003e\n \u003ch2\u003e3.1. Sound pressure level test\u003c/h2\u003e\n \u003cp\u003eAs previously stated, in order to reduce heat loss and select a suitable conductor for applying the high frequency current through the coil, the spool was wound by an ordinary wire and also Litz wire with the same number of coil turns. The purpose was to compare the performance of these two types of wirings. The results showed that the inductance of the coil with 100 turns for the coil with ordinary wire and Litz wire was 112.9 and 74 microhenry, respectively. Thus, by increasing the number of strands in the Litz wire, the resistance created at high frequencies decreases [\u003cspan class=\"CitationRef\"\u003e28\u003c/span\u003e].\u003c/p\u003e\n \u003cp\u003eIn order to compare the real transducer with the simulation model, the sound pressure was measured. This parameter has been used to evaluated the performance of ultrasonic transducers [\u003cspan class=\"CitationRef\"\u003e29\u003c/span\u003e], [\u003cspan class=\"CitationRef\"\u003e30\u003c/span\u003e]. The sound pressure produced is affected by the size of transducer. This increase is about three to five decibels [\u003cspan class=\"CitationRef\"\u003e29\u003c/span\u003e]. However, due to the small size of the transducer in this study, this effect can be ignored. Figure \u003cspan class=\"InternalRef\"\u003e3\u003c/span\u003e shows the sound pressure distribution of the simulated transducer using the JMAG-Designer software.\u003c/p\u003e\n \u003cp\u003eIn Fig. \u003cspan class=\"InternalRef\"\u003e4\u003c/span\u003e the sound pressure level diagrams in three different modes is presented (simulated, real model and ambient\u0026thinsp;+\u0026thinsp;real model). As seen the average sound pressure level in the simulated model, the absolute sound pressure level (solely from transducer) of the real transducer and the sound pressure level of real transducer with ambient sound were 33.98, 35.6 and 66.5 dB, respectively. A slight difference (4.5%) between the sound pressure level in the simulated model and the real transducer is seen. This is mainly due to the way of calculating the sound pressure. The sound pressure in the software environment was calculated on a spherical shell with a diameter of 100 mm, while in the real transducer this was done by connecting the decibel meter directly in front of the core horn. Moreover, due to the mismatch of different properties of transducer in simulation and real model, some error is expected. Generally, in ultrasonic transducers the transmitted power and sound pressure level increase with decreasing probe distance [\u003cspan class=\"CitationRef\"\u003e31\u003c/span\u003e].\u003c/p\u003e\n\u003c/div\u003e\n\u003cdiv class=\"Section2\" id=\"Sec13\"\u003e\n \u003ch2\u003e3.2. Evaluating dispersion ability of the magnetostrictive device\u003c/h2\u003e\n \u003cp\u003eBy dropping the waterproof paint at the bottom of a glass bottle and applying the magnetostrictive transducer and filming the process, the color images and red, green and blue channels were extracted in the MATLAB software environment. Because high-speed imaging can determine the formation of cavitation phenomenon and the growth of cavitation clouds [\u003cspan class=\"CitationRef\"\u003e32\u003c/span\u003e].\u003c/p\u003e\n \u003cp\u003eHowever, as mentioned, the scaling method was used to improve the image contrast and increase the pixel intensity. Considering that the effective coefficients can be obtained by trial and error [\u003cspan class=\"CitationRef\"\u003e33\u003c/span\u003e], in this section a coefficient of 2 was selected to scale the images. In Fig.\u0026nbsp;5, the elapsed times are displayed in the first column and the other columns are the images extracted from different color channels. According to this figure, the right column shows the status of paint dispersion as control i.e. the glass bottle that was not treated with the ultrasonic transducer is shown. As seen, in this case after 60 seconds, the waterproof paint on the bottom of the glass bottle does not disperse and only the paint on the top of the bottle moves down. By using RGB color channels, the image features can be extracted [\u003cspan class=\"CitationRef\"\u003e22\u003c/span\u003e]. As can be seen in this figure, and comparing the images of different color channels at 10, 40, and 60 seconds, it is observed that the images of the red color channel are clearer than the other channels and also more consistent with the RGB image.\u003c/p\u003e\n \u003cp\u003eSince the images extracted from red channel were more consistent with the RGB images, the histogram of this channel was drawn for different elapsed times as shown in Fig. \u003cspan class=\"InternalRef\"\u003e6\u003c/span\u003e. At 10 and 20 seconds elapsed times, which are shown in Fig. \u003cspan class=\"InternalRef\"\u003e6\u003c/span\u003e.a and 6.b respectively, it is observed that the higher gray scales have a small number of pixels and the lower gray scales have less than 400 pixels, implying less dispersion of the paint. But over time at 40, 50 and, 60 seconds, which are shown in Fig. \u003cspan class=\"InternalRef\"\u003e6\u003c/span\u003e.d, 6.e, and 5.f, respectively, it is observed that the number of pixels with higher gray scales has decreased to zero, but the number of pixels with lower gray scales increased to values above 1000. The evolution of pixel\u0026rsquo;s grayscale over time shows the paint dispersion process. This indicates that turbulence has occurred in the liquid due to the operation of the magnetostrictive ultrasonic transducer, which has caused the paint to spread.\u003c/p\u003e\n \u003cp\u003eFor further investigation and eliminating the color effects of the transducer probe in the achieved images, the space around the transducer probe was divided into 6 parts, because depending on the type of research, parts of the image that are fixed or variable can be cut and deleted or processed [\u003cspan class=\"CitationRef\"\u003e34\u003c/span\u003e]. In other words, according to Fig. \u003cspan class=\"InternalRef\"\u003e7\u003c/span\u003e, \u003cspan class=\"InternalRef\"\u003e3\u003c/span\u003e parts on the right side and 3 parts on the left side of the transducer probe with the same dimensions (60 pixels wide by 50 high) were selected. The Red channel histograms data were extracted at 60 seconds and the mean value was calculated for all gray scales. By analyzing this data, it was found that the mean value (72) is related to the gray scale 41. Therefore, to calculate the percentage of surface occupied by the waterproof paint in each of the 6 parts, all pixels whose gray scale was less than 73 were counted. Because by counting the number of pixels that have a special property, the amount of the surface and its changes can be achieved [\u003cspan class=\"CitationRef\"\u003e22\u003c/span\u003e]. Then at different elapsed times, the number of pixels was introduced as a percentage of the occupied area. According to this figure, since the dispersion of waterproof paint at the bottom of the glass bottle is non-uniform, it is observed that the cropped image at the lower end of the left side has an occupancy level of 62% at 10 seconds and at the end of 60 seconds the occupied area reaches 81%. But at the lower right side, the occupied area is initially 28% and at the end about 100%. But in the middle parts, the paint dispersion speed increases from 20 to 40 seconds, so that in 40 seconds, more than 80% of these areas are occupied by blue paint. At the upper parts, up to 40 seconds, the dispersion speed is very low (less than 40%), but it is observed that between 40 to 60 seconds, this increases rapidly so that more than 90% of these areas are occupied by blue paint. In other words, the cavitation phenomenon created by mechanical waves of the ultrasonic transducer initially creates bubbles at the lower parts. But over time, these bubbles burst and move upward to dissolve the blue paint in the middle and then the upper layers. Because over time and increasing the radius of the bubbles and reaching their critical radius and pressure, the bubbles become unstable and their density decreases, so the bubbles begin to move upwards. Also, by increasing the Reynolds number, which indicates turbulence in the fluid, tails are created on the new bubbles, which intensifies the cavitation phenomenon and increases the tendency to last longer after the disappearance of the main bubbles [\u003cspan class=\"CitationRef\"\u003e35\u003c/span\u003e]. As a result, the magnetostrictive ultrasonic transducer causes the complete dispersion of the blue paint in the glass bottle for 60 seconds by creating the cavitation phenomenon. In general, employing image processing method is useful in studying the dynamic behavior of clouds created by cavitation phenomenon in aqueous solvents [\u003cspan class=\"CitationRef\"\u003e36\u003c/span\u003e]. So that by using gray images, dimensional parameters such as the length of the created cavitation clouds can be measured [\u003cspan class=\"CitationRef\"\u003e37\u003c/span\u003e].\u003c/p\u003e\n\u003c/div\u003e\n\u003cdiv class=\"Section2\" id=\"Sec14\"\u003e\n \u003ch2\u003e3.3. GC test\u003c/h2\u003e\n \u003cp\u003eMicroorganisms are among the natural contaminants of fresh products. Observance of hygienic principles of such products is done by washing in tap water to remove residual pesticides, contaminants, plant residues and reduce the microbial load on the peel of fruits [\u003cspan class=\"CitationRef\"\u003e38\u003c/span\u003e]. The effects of ultrasonic cleaning for 5, 10 and 20 minutes on the residual pesticide are shown in Table\u0026nbsp;(2). Ultrasonic waves in water cause cavitation. Therefore, in the medium, micron-sized bubbles are formed quickly and burst. In such conditions, small explosions are created that provide the power of cleaning. According to this table, the Diazinon residue decreases with increasing time. Ultrasonic cleaning in 20 minutes has significantly reduced this pesticide. In other words, by using external standard method in GC test, the results showed that the residual pesticide based on the height of the chromatogram for the reference, 5, 10 and, 20 minutes were 1, 0.27, 0.26 and 0.25, respectively. Also, the residual pesticide based on the area under the chromatogram for the reference, 5, 10, and 20 minutes were 1, 0.21, 0.18, and 0.17, respectively. In other words, using the magnetostrictive ultrasonic transducer for 20 minutes, the residual pesticide based on the height and chromatogram area were 25% and 17%, respectively. For ultrasonic cleaning, it is assumed that the sound bubbles created by the cavitation phenomenon oscillate over the peel products at a distance of several tens of nanometers. The flow created by the bursting of the bubble can lead to tensile and shear forces over the peel. This flow will cause cleaning [\u003cspan class=\"CitationRef\"\u003e39\u003c/span\u003e]. In a study that used ultrasonic treatment for 20 min to remove pesticides from cucumber product, the residual pesticides for Trichlorfon, Dimethoate, Dichlorvos, Fenitrothion and, Chlorpyrifos were reported 17.1%, 47.8%, 50.2%, 15.6%, and, 37%, respectively [\u003cspan class=\"CitationRef\"\u003e25\u003c/span\u003e]. Also, in another study that used piezoelectric transducers with variable powers and times for tomato product, the results showed that by considering 300 watts and 15 minutes, the residual pesticide for DDVP was 89% [\u003cspan class=\"CitationRef\"\u003e40\u003c/span\u003e]. Probably, the small volume of the lab beaker and also considering the 2-minute interval for each one-minute treatment are the main reasons that have improved the results of this study compared to other studies. Because according to table (1), by applying ultrasonic waves for 5 minutes, the reduction of Diazinon pesticide was more than 73%. On the other hand, in the ultrasonic bath, the power level is not high enough because the transducer vibrations enter the tank through a metal wall. Therefore, sound waves form a sustainable wave pattern in the tank and the distribution of the ultrasonic field is not uniform. But the uniformity of this distribution in a probe system is less than in an ultrasonic bath. So that intense vibrations occur at the tip of the probe, causing a hole or corrosion in the metal probe [\u003cspan class=\"CitationRef\"\u003e39\u003c/span\u003e].\u003c/p\u003e\n \u003cdiv class=\"gridtable\"\u003e\u0026nbsp;\u0026nbsp;\u003ctable border=\"1\" id=\"Tab2\"\u003e\n \u003ccaption language=\"En\"\u003e\n \u003cdiv class=\"CaptionNumber\"\u003eTable 2\u003c/div\u003e\n \u003cdiv class=\"CaptionContent\"\u003e\n \u003cp\u003eGC test results for different treatment times on cucumber\u003c/p\u003e\n \u003c/div\u003e\n \u003c/caption\u003e\n \u003cthead\u003e\n \u003ctr\u003e\n \u003cth align=\"left\"\u003e\n \u003cp\u003eSample\u003c/p\u003e\n \u003c/th\u003e\n \u003cth align=\"left\"\u003e\n \u003cp\u003eElapsed Time (min)\u003c/p\u003e\n \u003c/th\u003e\n \u003cth align=\"left\"\u003e\n \u003cp\u003eHBR\u003csup\u003e*\u003c/sup\u003e\u003c/p\u003e\n \u003c/th\u003e\n \u003cth align=\"left\"\u003e\n \u003cp\u003eReduction (%)\u003c/p\u003e\n \u003c/th\u003e\n \u003cth align=\"left\"\u003e\n \u003cp\u003eABR\u003csup\u003e**\u003c/sup\u003e\u003c/p\u003e\n \u003c/th\u003e\n \u003cth align=\"left\"\u003e\n \u003cp\u003eReduction (%)\u003c/p\u003e\n \u003c/th\u003e\n \u003c/tr\u003e\n \u003c/thead\u003e\n \u003ctbody\u003e\n \u003ctr\u003e\n \u003ctd align=\"left\"\u003e\n \u003cp\u003eReference\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd align=\"left\"\u003e\n \u003cp\u003e-\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd align=\"left\"\u003e\n \u003cp\u003e1\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd align=\"left\"\u003e\n \u003cp\u003e-\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd align=\"left\"\u003e\n \u003cp\u003e1\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd align=\"left\"\u003e\n \u003cp\u003e-\u003c/p\u003e\n \u003c/td\u003e\n \u003c/tr\u003e\n \u003ctr\u003e\n \u003ctd align=\"left\"\u003e\n \u003cp\u003eNo. 1\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd align=\"left\"\u003e\n \u003cp\u003e5\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd align=\"left\"\u003e\n \u003cp\u003e0.27\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd align=\"left\"\u003e\n \u003cp\u003e73\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd align=\"left\"\u003e\n \u003cp\u003e0.21\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd align=\"left\"\u003e\n \u003cp\u003e79\u003c/p\u003e\n \u003c/td\u003e\n \u003c/tr\u003e\n \u003ctr\u003e\n \u003ctd align=\"left\"\u003e\n \u003cp\u003eNo. 2\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd align=\"left\"\u003e\n \u003cp\u003e10\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd align=\"left\"\u003e\n \u003cp\u003e0.26\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd align=\"left\"\u003e\n \u003cp\u003e74\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd align=\"left\"\u003e\n \u003cp\u003e0.18\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd align=\"left\"\u003e\n \u003cp\u003e82\u003c/p\u003e\n \u003c/td\u003e\n \u003c/tr\u003e\n \u003ctr\u003e\n \u003ctd align=\"left\"\u003e\n \u003cp\u003eNo. 3\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd align=\"left\"\u003e\n \u003cp\u003e20\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd align=\"left\"\u003e\n \u003cp\u003e0.25\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd align=\"left\"\u003e\n \u003cp\u003e75\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd align=\"left\"\u003e\n \u003cp\u003e0.17\u003c/p\u003e\n \u003c/td\u003e\n \u003ctd align=\"left\"\u003e\n \u003cp\u003e83\u003c/p\u003e\n \u003c/td\u003e\n \u003c/tr\u003e\n \u003ctr\u003e\n \u003ctd align=\"left\" colspan=\"6\"\u003e\n \u003cp\u003e* Height Based Results\u003c/p\u003e\n \u003cp\u003e** Area Based Results\u003c/p\u003e\n \u003c/td\u003e\n \u003c/tr\u003e\n \u003c/tbody\u003e\n \u003c/table\u003e\n \u003c/div\u003e\n\u003c/div\u003e\n\u003cdiv class=\"Section2\" id=\"Sec15\"\u003e\n \u003ch2\u003e3.4. SEM imaging\u003c/h2\u003e\n \u003cp\u003eThe micro-images of the middle part of the cucumber were selected for measuring the dimensions of the peel features. All SEM images were taken at 2500 magnification and working distance of 8 mm. According to Fig.\u0026nbsp;8, the peel features of the cucumber product such as stomatal pores were observed by SEM images. In other words, the stomatal pores and their guard cells that are elliptic were evaluated. Stomatal pores are involved in the gas exchange of many fruits and vegetables such as cucumber, and are embedded in the epidermis for several microns [\u003cspan class=\"CitationRef\"\u003e27\u003c/span\u003e]. As can be seen in this figure, by increasing the time of ultrasonic treatment, the opening area of stomatal pores decreases so that the highest opening area is related to the reference (Fig.\u0026nbsp;8.a) and the lowest opening area is related to the 20 min treatment (Fig.\u0026nbsp;8.d). The results of a study showed that by applying ultrasound for 2 min on the surface of the recalcitrant squash cotyledon, the stomatal pores and Ridges of the guard cells were still in place. But after 10 min, the edges of the guard cells and the surrounding areas were smoothed. After 30 minutes, Severe peel damage was observed so that epidermal cells and stomatal pores were damaged, and also large cracks were observed on the peel surface [\u003cspan class=\"CitationRef\"\u003e41\u003c/span\u003e]. As mentioned, ultrasonic waves not only clean the cucumber product, but also close the stomatal pores, and this will probably increase the shelf life of the product without affecting the content of organic and mineral materials as well as mechanical properties. Because according to the researches, the ultrasonic treatment of cherry tomatoes, strawberries and palm fruits has almost doubled the shelf life without affecting their contents [\u003cspan class=\"CitationRef\"\u003e42\u003c/span\u003e].\u003c/p\u003e\n \u003cp\u003eAlso, according to Fig.\u0026nbsp;8, it is observed that with increasing treatment time, the peel texture of the cucumber product has been worn. So that by increasing this time, the depth of cavities on the cucumber peel has decreased and the pitting wall thickness has increased. The color uniformity in the 20 min treatment (Fig.\u0026nbsp;8.d) compared to the 5 min treatment (Fig.\u0026nbsp;8.b) justifies this peel erosion. The results of a study showed that by applying ultrasound for 2 min on the surface of the recalcitrant squash cotyledon, the surface of the epidermal cell in the reference was higher than the cell junctions. By applying ultrasonic treatment for 2 minutes, the surface of the epidermal cell and the cell junctions were disproportionately worn. By increasing the treatment time for 10 minutes, this erosion increased so that the surface of the epidermal cell was approximately equal to the cell junctions [\u003cspan class=\"CitationRef\"\u003e41\u003c/span\u003e].\u003c/p\u003e\n \u003cp\u003eUltrasound produces intense pressure, shear force and temperature gradient in the material, which cause mechanical rupture in the texture. In other words, by propagation sound energy, which is mechanical oscillations, through the medium, three types of waves are created, which are: (1) longitudinal waves that move in the direction of displacement (2) shear waves that are perpendicular to the wave main motion (3) Rayleigh waves that travel very close to the material surface. Therefore, these three types of waves create alternating expansions and contractions. During these cycles, millions of small bubbles form that grow by absorbing energy from the medium, and when they cannot absorb more energy, they become unstable and burst violently. This releases a large amount of energy known as cavitation. A bubble can burst at or near the top of a cell wall. When this happens above the cell surface, it can potentially cause cavities in the cell wall [\u003cspan class=\"CitationRef\"\u003e42\u003c/span\u003e]. On the other hand, the bursting of bubbles created by transient cavitation causes serious physical conditions. These conditions include high temperature (up to 5000 K), high pressure (up to 1000 atm), high rate of cooling and heating (up to 1010 \u003cspan class=\"InlineEquation\"\u003e\u003cspan class=\"mathinline\"\u003e\\(K/s\\)\u003c/span\u003e\u003c/span\u003e), shock waveforms, and high-speed water jet (156 \u003cspan class=\"InlineEquation\"\u003e\u003cspan class=\"mathinline\"\u003e\\(km/h\\)\u003c/span\u003e\u003c/span\u003e) [\u003cspan class=\"CitationRef\"\u003e39\u003c/span\u003e].\u003c/p\u003e\n \u003cp\u003ePhotoshop software was used to investigate the effects of ultrasonic mechanical waves on the peel texture of cucumber products accurately. In other words, the dimensions of the stomatal pores, the Guard cell wall thickness, and pitting wall thickness were calculated using the scaling method. Since the stomatal pores are ellipsoid, the area of these pores can be calculated using the ellipsoid area equation.\u003c/p\u003e\n \u003cp\u003ewhere in this equation, A, a, and b are the stomatal pore area, the major diameter of the ellipse, the minor diameter of the ellipse [\u003cspan class=\"CitationRef\"\u003e27\u003c/span\u003e]. Based on the effects of the cavitation phenomenon and what was mentioned above, according to Fig. \u003cspan class=\"InternalRef\"\u003e9\u003c/span\u003e by increasing the treatment time, the stomatal pore area reduced from 144.74 \u003cspan class=\"InlineEquation\"\u003e\u003cspan class=\"mathinline\"\u003e\\({\\mu m}^{2}\\)\u003c/span\u003e\u003c/span\u003e (reference) to 30.56 \u003cspan class=\"InlineEquation\"\u003e\u003cspan class=\"mathinline\"\u003e\\({\\mu m}^{2}\\)\u003c/span\u003e\u003c/span\u003e (20 min treatment). Also, the guard cell wall thickness increased from 1.49 \u0026micro;m (reference) to 4.16 \u0026micro;m. But according to this figure, the increasing trend of guard cell wall thickness is ascendant for 10 minutes and then is almost constant. This trend may be due to the higher location of guard cells relative to the epidermis and also the lower thickness of the guard cell walls relative to the wall thickness of the epidermis cells. This increases the erosion process speed in the early minutes. Then the guard cell wall thickness increases due to erosion and the cell height become equal to epidermis cells and as a result, the increasing trend of the guard cell wall thickness or erosion speed decreases. In addition, the epidermis wall thickness increased from 2.20 \u0026micro;m (reference) to 4.78 \u0026micro;m (20 min treatment). According to this figure, the increasing trend of the Epidermis cell wall thickness is still ascendant. Therefore, by increasing ultrasonic treatment time, significant peeling will be done in the cucumber samples.\u003c/p\u003e\n\u003c/div\u003e"},{"header":"Conclusion","content":"\u003cp\u003eIn this research a magnetostrictive ultrasonic transducer was built and its ability in creating cavitation in fluid (for cleaning of delicate fruits and vegetables) due to its generated mechanical waves was evaluated. Based on the previous finding, a conical core made of pure nickel (as an abundantly available, less expensive, less hazardous material) with a cone angle of 30 degrees was used. The results showed that the sound pressure of the simulated model and the real transducer are almost the same. In addition, the ability of the transducer to disperse waterproof paints in aqueous solvent was evaluated by image processing method. Comparing the red, green and blue channels with the RGB image, it was observed that the red channel is able to display more details of the RGB image. The results showed that the transducer is able to disperse more than 90% of waterproof paints in the glass bottle after 60 seconds. It was also observed that the cavitation phenomenon initially moves the paint at the bottom of the glass bottle and then causes to spread the paint towards the middle layers and finally in the upper layers. In addition, the GC test results showed that the residual pesticide based on the height and chromatogram area were 75% and 83%, respectively. Also, by increasing the treatment time, the stomatal pore area decreases so that the maximum opening area was observed in the reference and the minimum area for the sample of 20 min treatment time. By increasing the treatment time, the peel texture of cucumber is worn so that the epidermis cell depth decreased and the epidermis wall thickness. This erosion can be justified by comparing the color uniformity in the 20 min treatment and the 5 min treatment. However, as mentioned, one of the challenges of this study is the low effect of magnetostrictive nickel core. So a small lab beaker (250 cc) was selected to place two cucumbers with the ultrasonic horn. For future research, it is suggested that the effects of increasing the number of transducers and increasing the horn length in large container be investigated.\u003c/p\u003e"},{"header":"Declarations","content":"\u003cp\u003e\u003cstrong\u003eAcknowledgements\u0026nbsp;\u003c/strong\u003e\u003c/p\u003e\n\u003cp\u003eThe authors acknowledge and appreciate the funding and technical supports provided by the Ferdowsi University of Mashhad, Iran for this project.\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003eFunding:\u003c/strong\u003e This study was funded by Ferdowsi University of Mashhad (FUM), (grant number 46420).\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003eConflict of Interest:\u003c/strong\u003e The authors declare that they have no conflict of interest.\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003eData Availability Statement:\u003c/strong\u003e All data generated or analysed during this study are included in this published article. Also, more information is available from the corresponding author on request.\u003c/p\u003e\n\u003cp\u003e\u003cstrong\u003eAuthor Contributions Statement:\u003c/strong\u003e Dr. Danial Gandomzadeh and Mrs. Yeganeh Sabeghi conceived the presented idea. Mr. Soheil Movahed Fakhr developed the theory and performed the computations. Prof. Mohammad Hossein Abbaspour-Fard verified the analytical methods. All authors discussed the results and contributed to the final manuscript.\u003c/p\u003e"},{"header":"References","content":"\u003col\u003e\u003cli\u003e\u003cspan\u003eT. M. 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Gonz\u0026aacute;lez-Aguilar, \u0026ldquo;Ultrasonic Processing Technology for Postharvest Disinfection,\u0026rdquo; in \u003cem\u003ePostharvest Disinfection of Fruits and Vegetables\u003c/em\u003e, Elsevier, 2018, pp.\u0026nbsp;101\u0026ndash;119.\u003c/span\u003e\u003c/li\u003e\u003c/ol\u003e"}],"fulltextSource":"","fullText":"","funders":[],"hasAdminPriorityOnWorkflow":false,"hasManuscriptDocX":true,"hasOptedInToPreprint":true,"hasPassedJournalQc":"","hasAnyPriority":false,"hideJournal":false,"highlight":"","institution":"","isAcceptedByJournal":true,"isAuthorSuppliedPdf":false,"isDeskRejected":"","isHiddenFromSearch":false,"isInQc":false,"isInWorkflow":false,"isPdf":false,"isPdfUpToDate":true,"isWithdrawnOrRetracted":false,"journal":{"display":true,"email":"[email protected]","identity":"food-and-bioprocess-technology","isNatureJournal":false,"hasQc":true,"allowDirectSubmit":false,"externalIdentity":"","sideBox":"Learn more about [Food and Bioprocess Technology](https://www.springer.com/journal/11947)","snPcode":"11947","submissionUrl":"https://submission.nature.com/new-submission/11947/3","title":"Food and Bioprocess Technology","twitterHandle":"","acdcEnabled":true,"dfaEnabled":true,"editorialSystem":"stoa","reportingPortfolio":"Springer Hybrid","inReviewEnabled":true,"inReviewRevisionsEnabled":false},"keywords":"Magnetostrictive ultrasonic transducer, Residual Pesticide, Cleaning, GC, SEM ","lastPublishedDoi":"10.21203/rs.3.rs-2009995/v1","lastPublishedDoiUrl":"https://doi.org/10.21203/rs.3.rs-2009995/v1","license":{"name":"CC BY 4.0","url":"https://creativecommons.org/licenses/by/4.0/"},"manuscriptAbstract":"\u003cp\u003eIn recent years, ultrasonic machining has been developing rapidly and it is used in areas such as abrasive machining, cleaning, and welding. In this research, a magnetostrictive device with pure nickel conical core with cone angle of 30 degrees was constructed. The observed sound pressure level was used as a measure of transducer performance. Also the ability of the device to reduce the residual pesticide on cucumber surface due to cavitation was evaluated. The results showed that the sound pressure from simulation by JMAG-Designer software is almost the same as the sound pressure produced in the constructed transducer. To assess the performance of the device in removing residual pesticide from cucumber surface and evaluate the changes in peel texture of cucumber, the GC and SEM methods were used, respectively. The GC results showed that with 20 min treatment, the removal of pesticide based on height and chromatogram area were 75% and 83%, respectively. The SEM results showed that by increasing the treatment time, the stomatal pore area reduced from 144.74 \u003cspan class=\"InlineEquation\"\u003e\u003cspan class=\"mathinline\"\u003e\\({\\mu m}^{2}\\)\u003c/span\u003e\u003c/span\u003e (reference) to 30.56 \u003cspan class=\"InlineEquation\"\u003e\u003cspan class=\"mathinline\"\u003e\\({\\mu m}^{2}\\)\u003c/span\u003e\u003c/span\u003e (20 min treatment). This results are promising, hence further research is suggested towards enhancing the device for commercial use in biomaterials processing operations such as cleaning and removing pesticides from fruits and vegetables.\u003c/p\u003e","manuscriptTitle":"Evaluating an ultrasonic magnetostrictive transducer with conical nickel core: performance and application","msid":"","msnumber":"","nonDraftVersions":[{"code":1,"date":"2022-09-08 14:34:39","doi":"10.21203/rs.3.rs-2009995/v1","editorialEvents":[{"type":"communityComments","content":0},{"type":"decision","content":"Major revision","date":"2022-09-05T08:22:21+00:00","index":"","fulltext":""},{"type":"editorAssigned","content":"","date":"2022-09-05T08:21:20+00:00","index":"","fulltext":""},{"type":"checksComplete","content":"","date":"2022-09-05T01:04:28+00:00","index":"","fulltext":""},{"type":"submitted","content":"Food and Bioprocess Technology","date":"2022-08-29T12:51:58+00:00","index":"","fulltext":""}],"status":"published","journal":{"display":true,"email":"[email protected]","identity":"food-and-bioprocess-technology","isNatureJournal":false,"hasQc":true,"allowDirectSubmit":false,"externalIdentity":"","sideBox":"Learn more about [Food and Bioprocess Technology](https://www.springer.com/journal/11947)","snPcode":"11947","submissionUrl":"https://submission.nature.com/new-submission/11947/3","title":"Food and Bioprocess Technology","twitterHandle":"","acdcEnabled":true,"dfaEnabled":true,"editorialSystem":"stoa","reportingPortfolio":"Springer Hybrid","inReviewEnabled":true,"inReviewRevisionsEnabled":false}}],"origin":"","ownerIdentity":"ca75ea10-6c24-4da7-988c-3cacf21e14b6","owner":[],"postedDate":"September 8th, 2022","published":true,"recentEditorialEvents":[],"rejectedJournal":[],"revision":"","amendment":"","status":"under-review","subjectAreas":[],"tags":[],"updatedAt":"2022-11-20T12:44:15+00:00","versionOfRecord":[],"versionCreatedAt":"2022-09-08 14:34:39","video":"","vorDoi":"","vorDoiUrl":"","workflowStages":[]},"version":"v1","identity":"rs-2009995","journalConfig":"researchsquare"},"__N_SSP":true},"page":"/article/[identity]/[[...version]]","query":{"redirect":"/article/rs-2009995","identity":"rs-2009995","version":["v1"]},"buildId":"J0_U0BvcaRcwD8yVFaRlm","isFallback":false,"isExperimentalCompile":false,"dynamicIds":[84888],"gssp":true,"scriptLoader":[]}