This paper presents the design of an instrument for measuring the liquid level. The objective of this proposed work is to measure the level of liquid accurately even with variations in liquid concentration. The designed instrument should also be able to compute the concentration of additives in the liquid. For this purpose, a multisensor model comprising a capacitive level sensor (CLS), ultrasonic level sensor (ULS), and capacitance pressure sensor is used to acquire information of the liquid. The data acquired from all these sensors are processed using Pau’s multisensor data fusion framework to compute the level of liquid along with the concentration of additives added to the solution. Pau’s framework consists of alignment, association function, analysis, and representation functions. The designed multisensor technique is tested with real-life data for varying liquid levels and additives. The results obtained show that the successful implementation of the proposed objective producing a root mean square of percentage error is 1.1% over the full scale is possible.
1. Introduction
The level process is one of the most commonly found processes in any process industry, like the diary, pharmacy, fabric, petroleum, and confectionary. The liquid process ideally involves control of the liquid level in a container under a dynamic or static condition with the set point level as desired by the user. The controller is implemented to obtain the desired set point by actuating the final control element. To design a controller, an instrument is needed to measure the actual liquid level. This instrument is a device used to measure physical parameters, in this case, liquid level.
Many measurement techniques are available for liquid level measurement; a detailed study of available measurement techniques is reported. Several liquid measurement techniques such as capacitance and conductive are analysed in [1]. A technique for liquid level measurement using multiple capacitive sensors to increase the sensitivity of measurement is reported in [2]. Analysis of capacitive liquid level sensor characteristics for fuel measurement in a level control process used in the upper-stage rocket system is reported in [3]. Design and development of semicylindrical capacitor for measurement of liquid level is reported in [4]. In [5], the principle of variation in conductivity of an electrode with variation in liquid level is used for measurement of liquid. Image processing technique used to compute the level of liquid from the captured image of the container is reported in [6, 7]. Measurement of liquid level in a distillation process using a digital camera is discussed in [8]. Paper [9] discusses the technique of liquid level measurement based on the reflective principle of light. Change in the total internal reflection of light passing through the optical fiber varies with a change in liquid, which is utilized in [10] for measuring the liquid level. In [11], a reflected acoustic wave is analysed to compute the level of the liquid. Paper [12] reported the analysis of radiated frequency-modulated millimeter wave through a container with liquid for measurement of liquid level measurement. Time-domain reflectometry is analysed to compute the level of liquid in [13]. In [14], refractive index analysis via coreless multimode fiber is carried on to compute the level of liquid in a container. Paper [15] reports measurement of liquid level by intercepting signal to the controller using wavelet packet transform. Design and evaluation of a capacitance water level sensor are discussed in [16]. In [17], the design and analysis of coaxial cylindrical CLS, which is used to measure the level of conductive liquid, are reported. Monitoring the wavelength shift caused by a multimode interface in a no core fiber for measurement of liquid level is discussed in [18]. Paper [19] reports the design of a Mach-Zehnder interferometer formed by sandwiching photonic crystal fiber to measure the level of the liquid. Echo from the liquid surface and wire immersed in the liquid are analysed to detect changes in propagation speed. This change is used to measure the liquid level in [20]. The acoustic response was detected to measure the penetration depth by comparing the true value and the Helmholtz resonance frequency in [21]. Paper [22] discusses the implementation of a comb-type capacitor design for improved sensitivity in liquid level measurement. Optical fiber is used to measure the dynamic level of liquid in [23]. Paper [24] discusses the design of printed resonator used to measure the level of the liquid. Optical fibre is used to measure the level of liquid in the cryogenic propellant tank [25] and paper [26] uses a charged couple to measure the radiation reflected from the surface thereby measuring the level of the liquid. Although a lot of liquid level measuring instruments have been reported in the literature, they are confined to a particular measurement and are often calibrated under defined boundary conditions.
Few papers have reported on the effect of internal parameters on the measurement such as in paper [27] that discusses the effect of humidity on the capacitance sensor output. The effect of crude palm oil composition on electrical capacitance is analysed in [28]. Water permeation in organic coatings is measured by computing change in capacitance across the parallel plate electrodes in [29]. Measurement of moisture content in a solid structure by using a capacitance-based sensor is reported in [30]. In [31], the effect of the oil-water mixture on the capacitance sensor output is analysed to characterize the two-phase flow. Double helix capacitance is used to measure the liquid holdup in oil-water two-phase flow pipers in [32]. Density profile analysis is carried on using a capacitance sensor for a vibrated granular bed in [33]. In [34], pressure sensors are used to measure liquid level by measuring the density of a liquid. In [35], the liquid level is measured indirectly by measuring pressure exerted on a tube by the change in the liquid level. This paper also discussed the effect of temperature on measurement. Similarly, the effect of temperature on fiber Bragg grating sensor used for measurement of liquid level is discussed in [36]. Effect of change in liquid temperature on level measurement by capacitance level sensor is discussed in [37]. Effect of sensor placement on measurement when an acoustic sensor is used for measurement of liquid level is reported in [38]. In [39], liquid level measurement based on reflection guidance mechanism by using a silica tube is discussed. This technique also discusses its robustness towards temperature changes. Detailed analysis from the available literature gives us the information that output of capacitance liquid level sensor is not just the function of liquid level but also gets affected by the type of liquid, temperature of liquid, composition of liquid, etc. The above reported characteristics of capacitance level sensor are put to use in this proposed work to measure liquid level along with the concentration of soluble mixed in the liquid solution.
2. Experimental Setup
The experimental setup consists of a tank in which the liquid is stored. To measure the level of liquid, a capacitive level sensor is used. The output of this sensor is connected to a signal conditioning circuit to convert the output signal into a standard voltage signal. The voltage signal is then acquired using a NI myRIO board, as shown in Figure 1.
Experimental setup.
The equation for the capacitance level sensor is derived from the basic principles of capacitance, where the capacitance between two parallel plates can be given in Equation (1) [40, 41].
(1)C=∈0∈rAd,where “A” is the cross-sectional area of the plates, “d” is the distance between two plates, “∈0” is the permittivity of air, and “∈r” is the permittivity of liquid. If there is a change in the dielectric element, the capacitance will change accordingly.
In the proposed work, the capacitance level sensor is designed considering two parallel cylindrical rods that act as electrodes instead of parallel plates. The choice of this structure is for the ease of maintenance and for improved ruggedness as shown in Figure 2.
Schematic of the capacitance level sensor.
Total capacitance C is given by [42]
(2)C=πεoH−hlnd−a/a+πεoεrhlnd−a/a,where C is the total capacitance, ε0 is the vacuum permittivity, εr is the relative permittivity of water, d is the distance between electrodes, a is the electrode radius, h is the liquid level, and H is the electrode and tank height.
In the experimental setup considered for the proposed work, the dimensions of the capacitive level sensor are the distance between the electrodes d=0.0088m, radius of electrodes a=0.0015m, and the full height of the tank H=0.66m.
To convert the CLS output to voltage, a timer circuit and frequency to voltage conversion circuit is used. Timer circuit consists of a 555 IC as shown in Figure 3, and frequency to voltage conversion achieved using LM331 IC and a conversion circuit as shown in Figure 4. The outputs obtained from the timer circuit and frequency to voltage circuit is represented using Equation (3) and Equation (4), respectively. The output voltage is then acquired on to the computer using an analogue channel of NI myRIO (National Instruments Reconfigurable Input-Output Embedded Boards). The datasheets for 555 IC and LM331 IC provide the following equations. Figure 5 shows the practical implementation of the circuit for acquiring the capacitance and converting to voltage to acquire to PC by data acquisition devices [43].
(3)fi/p=1ln2RA+2RBCHz,(4)VO/P=R7R5+R6×2.09×R4×C2×FI/PV.
Circuit diagram of the timer.
Circuit diagram of frequency to voltage converter.
Practical setup for signal conditioning and acquisition.
3. Problem Statement
The above section shows how the experimental setup is designed. The experimental setup is subjected to varying levels of liquid and the output obtained is plotted. For experimentation, we use water and the output obtained for different levels is acquired by NI myRIO and the plot is as shown in Figure 6. From the highlighted region in characteristic plot of capacitance level sensor, as shown in Figure 6, it can be noted that a part of the initial range of measurement has a higher nonlinearity. This effect in the measurement is relative to the mechanical design of the electrode as can be seen in Figure 7 of the electrodes used.
Output of capacitance level sensor for variation of liquid level.
Capacitance electrodes for liquid level measurement.
To understand the effect of solution concentration on the output of a capacitance sensor, water is replaced by the sugar solution. Test result obtained for the same is as shown in Table 1 and the complete changes in terms of capacitance, frequency, and voltages are shown in Table 2. A similar analysis is carried out for the variation in liquid concentration by the addition of 10%, 20%, and 30% of the sugar solution. Figure 8 shows the variations of CLS output with changes in concentration and liquid level. From Table 1, it is clear that the output of capacitance is a function of liquid level and the property of liquid (permittivity). This property of the capacitance level sensor is used in the proposed work to design a multisensor system which can measure the level of liquid and in addition indicate details about the concentration of liquid under consideration.
Change in permittivity with a change in sugar concentration.
Weight of sugar (gms)/ltr of water
Permittivity at 25°C
0
78.54
10
76.19
20
73.65
30
70.70
40
67.72
50
64.20
60
60.19
Output of capacitance level sensor for variation of solution concentration.
Case 1: plain solution
Change in liquid level (in m)
Sensor output (nF)
Timer output (MHz)
Frequency to voltage converter output (V)
0.10
17.05
26.3
0.1
0.20
27.29
16.2
0.156
0.30
39.99
11.0
0.204
0.40
51.64
8.5
0.264
0.50
63.2
6.8
0.314
Case 2: 10% concentrated sugar solution
Change in liquid level (in m)
Sensor output (nF)
Timer output (kHz)
Frequency to voltage converter output (V)
0.10
16.22
26.8
0.093
0.20
26.1
16.6
0.15
0.30
38.36
11.3
0.203
0.40
49.61
8.8
0.265
0.50
61.1
7.1
0.324
Case 3: 20% concentrated sugar solution
Change in liquid level (in m)
Sensor output (nF)
Timer output (kHz)
Frequency to voltage converter output (V)
0.10
16.01
27.1
0.106
0.20
25.5
17.0
0.148
0.30
37.27
11.7
0.216
0.40
48.08
9.0
0.277
0.50
58.7
7.3
0.336
Case 4: 30% concentrated sugar solution
Change in liquid level (in m)
Sensor output (F)
Timer output (kHz)
Frequency to voltage converter output (V)
0.10
14.48
30.2
0.110
0.20
23.32
18.5
0.173
0.30
34.63
12.5
0.227
0.40
44.89
9.7
0.289
0.50
55.78
7.8
0.348
Plot of variation of CLS output for variation in the concentration of sugar solution.
4. Problem Solution
To achieve the objective of measuring the liquid level and the concentration simultaneously, a multisensor system is incorporated in addition to using the available capacitance level sensor. Two additional sensors, an ultrasonic level sensor and a pressure sensor, are placed on the container in which the liquid level is being measured, as shown in Figure 9. We consider a transit-type ultrasonic level sensor, which measures the level of liquid based on the time taken for the signal to travel from the sensor and back again. This value would be a direct indicator of the liquid level and will not vary with the type of liquid. In addition, a pressure sensor is also used in the experiment, which will measure the liquid level based on the density of the liquid.
Process setup with multiple physical sensors.
The data acquired from these three sensors are combined using Pau’s framework [44]. The block diagram in Figure 10 shows the process flow for data fusion using Pau’s. The first stage in the data fusion process is data alignment. In this stage, it is seen that the data to be fused will be of the same magnitude and be dimensionless.
Pau’s framework.
4.1. Additional Sensors
Ultrasonic Level Sensor. Transit time ultrasonic level sensor (ULS) is used to measure the level of the liquid. An ultrasonic level sensor is placed on top of the container such that the wave is transmitted on the surface of the water and the reflected signal is captured back. The time taken for the signal to transmit and reflect is used to compute the level of the liquid. Timer port of the microcontroller is used to compute the travel time, and the output corresponding to the time is transmitted in the form of a 16-bit digital signal. This 16-bit data relating to the liquid level is acquired by the standalone NI myRIO
Capacitive Pressure Sensor. Capacitance pressure sensor (CPS) output varies with a change in input pressure. As the liquid height varies, the pressure created at the nozzle varies. Liquid pressure is more when the liquid level is high and the pressure reduces accordingly as the liquid level in the tank reduces. This change in pressure also varies with variation in liquid density. Table 3 shows the variations of density on variation in the concentration of sugar. The experimental setup consists of a storage tank with dimension 12cm×10cm×60cm. From Table 3, it is very evident that there is variation in liquid density for a varying concentration of sugar. The change in pressure induces the change in a physical dimension of the diaphragm used in CPS, causing a relative change in capacitance. This change in capacitance is converted to a voltage using a De Sauty bridge followed by a rectifier circuit. The voltage output from the rectifier is acquired by the analog channel of NI myRIO as shown in Figure 11. From Figure 11, it can be seen that the nonlinearity exists in the characteristics due to the accuracy of discrete components and would be compensated at the time of fusion using artificial neural networks
Change in density for variation in liquid concentration.
Plain solution in kg/m3
10% concentration in kg/m3
20% concentration in kg/m3
30% concentration in kg/m3
Density
1001
1053
1118
1156
Output of capacitance pressure sensor of signal conversion output.
4.2. Alignment Techniques
Now that data from all three sensors (CLS, ULS, and pressure sensor) is acquired on to a NI myRIO board, they need to be fused and processed. The first step towards fusion is the alignment technique/common representation format. The purpose of this stage is to make sure that all the sensor sources are equally prioritized in terms of its magnitude. This implies that all the signals are directed to dimensionless values ranging from 0 to 1 or 0 to 100%. In the proposed work, we consider it to be between 0 and 1. Since the data derived from all three sources are one-dimensional, radiometric normalization technique is implemented.
Alignment Technique for CLS Output. Capacitance level sensor with a data conversion circuit produces an output that is a change in voltage for a change in the liquid level. The voltage varies from 0.05 V to 0.35 V for a corresponding change in liquid level of 0 cm to 50 cm. A spatial transformation is used in the proposed work to convert the signal strength in the range of 0 to 1. For carrying out the spatial transformation, a signal level of 0.05 V is considered as a reference and using this point, the rest of the signal is computed
Alignment Technique for ULS Output. Timer data corresponding to the transmission time of the ultrasonic signal that represents the liquid level is converted to a range of 0 to 1. For this, we use spatial alignment technique where the time taken for the wave to transmit and reflect when the tank is full is considered as “0” and when the tank is empty it is considered as “1.” Intermediate values are extrapolated based on the time taken for a signal to transmit and reflect
Alignment Technique for Pressure Sensor Output. The output of the pressure sensor is the voltage varying from 0.1 V to 3.6 V, as seen from the input-output relation from Figure 11. To represent this data in terms of normalized value between 0 and 1 as shown in Figure 12, min–max expression as represented in Equation (5) is used.
(5)Ynorm=ymax−yymax−ymin∗100.
Output of capacitance pressure sensor CRF output.
4.3. Association Fusion
Association is a technique, where data is grouped into different clusters over the entire range of inputs to perform computation in relation to the objective. The cluster is grouped such that the contribution of that particular cluster of data towards achieving the objective function can be computed. Several functions like the nearest neighbourhood, boundary conditions, the binary tree, and kd tree are used for this purpose. In the proposed work, boundary condition algorithms are used on CLS data; kd tree algorithm is used on pressure sensor data, followed by the nearest neighbourhood algorithm for ULS data.
4.4. Analysis and Aggregation or Decision-Making Process
The decision-making step in the proposed work involves the computation of the liquid level independent of the liquid used to determine the concentration of the solution. In the proposed work, evidence matching technique is used. For carrying out evidence matching, the neural network algorithm [45] is used. For training neural network, data corresponding to varying liquid levels with a defined concentration of solvent is considered. Here, 50 grams, 100 grams, 150 grams, and 200 grams of sugar are added to every 10 litres of water.
The input data for the neural network block is from the association vector, each of which is derived from the capacitance level sensor, pressure sensor, and ultrasonic level sensor. The neural network algorithms are trained such that the information related to the liquid level is derived directly from the ultrasonic level sensor output. For the information corresponding to the addition of liquid, CLS and pressure sensor data are used. Since it is clearly demonstrated that CLS output depends on the level of liquid and type of liquid (permittivity of liquid), the pressure sensor output depends on the density of the liquid (volume and mass). Backpropagation network with artificial bee colony algorithm is used in the proposed work. Backpropagation network can be decomposed into a feed-forward computation, backpropagation to the output layer, backpropagation to the hidden layers, and weight updates. Table 4 shows the details regarding the neural network model implemented in the proposed work. Pictorial representation of neural network signal connectivity is shown in Figure 13.
Neural network parameters.
Input layer
6 neurons
Output layer
8 neurons
Hidden layers
7 neurons
6 neurons
R
0.98
MSE
0.65E−7
Transfer function
Sigmoid
Neural network connectivity and structure.
Weight of the first connection matrix is given by P1=PU+1, c. Similarly, the weight of the second connection matrix is given by P2=Pc+1, v, since there will be (u+1)∗cweights between the input side and hidden layers and, similarly, (c+1)∗v weights in between hidden layers and output side. By considering the association vector for three transducer signals as f=f1,f2⋯fu, the excitation gi for the ith hidden unit is given by
(6)gi=∑j=1u+1Pijf^j.
Considering the sigmoid “s” as the activation function, a forward vector is computed.
(7)fi=s∑j=1u+1Pijf^j.
In the backward path, from the output of the network, the computation is similarly reversed such that the error is minimized. Artificial bee colony algorithm is used to update the weights “P.” Training is carried out until the network produces target as per the objective. This is achieved by monitoring the value of regression “R” which should ideally be one and mean square error “MSE” which should ideally be zero.
4.5. Representation
At this stage, the data is converted to the form of a physical variable. Until this stage, computation was carried out with a dimensionless value in the range of 0 to 1. The result obtained from the neural network will also be in the range of 0 to 1 which can be difficult to interpret by the user. Therefore, it is imperative to represent the results in the form of liquid level in terms of “cm” and concentration of the liquid in terms of “grams per litre.”
5. Results and Discussion
Once the process of data fusion is complete, the performance of the reported technique needs to be evaluated. For testing, the liquid level is measured by varying the concentration of sugar used in water and varying the level of the liquid. The level of liquid is varied in the range of 0 to 50 cm, and subsequently, the concentration of sugar is varied from 0 gram per litre of water to 25 grams per litre of water. Table 5 shows the results obtained for the same.
Results of water level measurement with varying sugar concentrations.
Sl. no.
Actual level of liquid in cm
Actual sugar in gram per litre of water
Measured level of liquid in cm
Measured sugar in gram per litre of water
1
0
0
0.06
0.09
2
2
2.5
2.14
2.65
3
4
3.6
3.85
3.54
4
6
4.8
5.65
5.12
5
8
10.0
8.19
9.93
6
10
7.6
9.89
7.75
7
12
13.5
11.89
13.21
8
14
17.5
14.02
17.65
9
16
25.0
15.91
24.61
10
18
8.5
17.88
8.32
11
20
15.5
20.1
15.39
12
22
21.0
21.5
20.84
13
24
1.0
23.59
0.94
14
26
5.0
25.9
5.21
15
28
19.0
28.01
19.34
16
30
23.5
30.09
23.04
17
32
6.0
31.82
5.87
18
34
14.0
33.69
14.42
19
36
17.2
35.71
17.51
20
38
11.0
38.05
11.11
21
40
22.0
39.82
21.81
22
42
17.0
41.8
16.74
23
44
2.5
43.95
2.52
24
46
10.0
45.82
10.12
25
48
20.0
47.95
19.63
26
50
0
49.78
0.03
Measurement of the liquid level is carried out using the designed multisensor technique for a liquid with varying concentrations. Liquid level is measured for different liquid concentrations. In Table 5, the output measured by the instrument for the varied sugar concentration is noted. Liquid level is measured when different liquids are used with varying sugar concentration without any recalibration of the system. In any available instrument, when the process medium is changed an error would be introduced, which is not the case here. The proposed system is used to measure the varying levels of liquid starting from 0 m to 50 cm with different liquid concentrations. From Table 5, it can be seen that the proposed technique is able to measure the liquid level with a maximum deviation of 5 mm from the desired value. The proposed system is also designed to identify the change in concentration using which the additive in the water is measured. The last column of Table 5 shows the measured concentration of sugar in the solution; it is observed that the proposed technique can measure the concentration of sugar added with the maximum deviation of 400 mg from the actual value.
The characteristics in terms of percentage error for the measurement are obtained and are plotted in Figures 14 and 15 for level measurement and concentration analysis. It is seen that the maximum percentage error produced by the measurement system is around 7%.
Error characteristics for liquid level measurement of sugar syrup.
Error characteristics for concentration analysis of sugar syrup.
To evaluate the performance, measurement is carried out considering milk powder instead of sugar. The results obtained for the test conducted are shown in Table 6. For the measurement of liquid level, a range of 0 cm to 50 cm is considered and the concentration of milk powder in water is varied from 0 grams to 100 grams per litre of water. Error characteristics are plotted in Figures 16 and 17.
Results of water level measurement with varying milk powder concentrations.
Sl. no.
Actual level of liquid in cm
Actual milk powder in gram per litre of water
Measured level of liquid in cm
Measured milk powder in gram per litre of water
1
0
0
0
0.10
2
4
45
3.7
44.5
3
10
85
10.1
87.8
4
10
10
9.4
10.4
5
15
100
14.8
97.6
6
18
60
17.1
61.4
7
18
35
17.8
34.1
8
25
75
26.4
73.6
9
30
50
30.9
48.9
10
30
85
28.9
85.1
11
34
55
35.6
55.1
12
42
10
40.1
9.7
13
42
90
41.4
89.5
14
42
0
43.7
0.23
15
45
70
45.9
73.7
16
48
25
50.0
24.5
17
48
60
50.0
58.9
18
50
40
50.0
39.2
19
50
12
48.3
12.7
20
50
100
49.1
100
Error characteristics for liquid level measurement of milk.
Error characteristics for concentration analysis of milk powder.
Similar to the experiment with the sugar solution, the proposed system is subjected to testing by considering the milk solution to validate the proposed measurement technique. Similar to the previous experiment, the results show a maximum deviation of 1 cm for the liquid level measured and a maximum deviation of 3 gm/litre for the measured concentration as compared to the actual values.
From Tables 5 and 6 and Figures 14–17, it is seen that the reported multisensor technique is able to measure liquid level accurately and robustly without the influence of additives in the liquid. The concentration of the additives was also measured accurately. Further tests were conducted under different conditions (different concentrations of additives and liquid level) with approximately 260 samples in addition to the results shown in Table 5 and Table 6. Root mean square of percentage error from the reported measurement technique was found to be 1.1%.
6. Conclusion
The level process is one of the widely used industrial processes, indicating a need for accurate measurement. Accuracy in measurement can be only be achieved if the process can produce results with the highest resistance to noise. Here, the noise is the additives in liquid. To achieve this, a technique comprising of multiple sensors fused together is suggested. For this purpose, a capacitive level sensor, an ultrasonic level sensor, and a pressure sensor are used. The output from each of the sensor is converted to a standard signal with the help of the data conversion circuit. The obtained signals are processed in four stages: alignment, association, analysis, and representation. Test results produced by the reported technique clearly indicate that the measurement is accurate and robust. Root mean square percentage error value of 1.1% indicates that the measurement system can be used in industries. With the use of an additional sensor or an improved training algorithm, this value can be increased. One constraint to this measurement process is that neither the liquid nor the additives can be conductive. Additionally, additives added must be soluble in the liquid.
Data Availability
The data used to support the findings of this study are included within the article.
Conflicts of Interest
The authors declare that they have no conflicts of interest.
KulkarniA.KarekarR. N.AiyerR. C.Liquid level sensor2005761010510810511310.1063/1.20544122-s2.0-27544473869CanbolatH.A novel level measurement technique using three capacitive sensors for liquids200958103762376810.1109/TIM.2009.20197152-s2.0-70349466794BalakinS. V.Errors of level sensors of a fueling level control system of an upper-stage rocket201558997598110.1007/s11018-015-0828-62-s2.0-84956881740PalS.BarikR.Design, development and testing of a semi cylindrical capacitive sensor for liquid level measurement201011651320ZhengG.ZongH.ZhuanX.LuanJ.Fast dynamic liquid level sensor based on liquid resistanceAFRICON 20072007Windhoek, South AfricaChakravarthyS.SharmaR.KasturiR.Noncontact level sensing technique using computer vision200251235336110.1109/19.9978372-s2.0-0036543805WangT. H.LuM. C.HsuC. C.ChenC. C.TanJ. D.Liquid-level measurement using a single digital camera200942460461010.1016/j.measurement.2008.10.0062-s2.0-61549100267LorenzM. G.Mengibar-PozoL.Izquierdo-GilM. A.High resolution simultaneous dual liquid level measurement system with CMOS camera and FPGA hardware processor201320146847610.1016/j.sna.2013.08.0052-s2.0-84883495169SinghH. K.ChakrobortyS. K.TalukdarH.SinghN. M.BezboruahT.A new non-intrusive optical technique to measure transparent liquid level and volume201111239139810.1109/JSEN.2010.20685432-s2.0-78649306771LomerM.ArrueJ.JaureguiC.AiestaranP.ZubiaJ.López-HigueraJ. M.Lateral polishing of bends in plastic optical fibres applied to a multipoint liquid-level measurement sensor20071371687310.1016/j.sna.2007.02.0432-s2.0-34249330961LucklumF.JakobyB.Non-contact liquid level measurement with electromagnetic-acoustic resonator sensors2009201212400210.1088/0957-0233/20/12/1240022-s2.0-72149094076NakagawaT.HyodoA.KogoK.KurataH.OsadaK.OhoS.Contactless liquid-level measurement with frequency-modulated millimeter wave through opaque container201313392693310.1109/JSEN.2012.22203462-s2.0-84873364523di SanteR.Time domain reflectometry-based liquid level sensor200576909510709511210.1063/1.20379272-s2.0-25844521156LiuY.LiY.YanX.LiW.High refractive index liquid level measurement via coreless multimode fiber2015272021112114PaulR.SenguptaA.Design and application of discrete wavelet packet transform based multiresolution controller for liquid level system20177158559810.1016/j.isatra.2017.07.0302-s2.0-8502829757728807374LoizouK.KoutroulisE.Water level sensing: state of the art review and performance evaluation of a low-cost measurement system20168920421410.1016/j.measurement.2016.04.0192-s2.0-84964323844JinB.ZhangZ.ZhangH.Structure design and performance analysis of a coaxial cylindrical capacitive sensor for liquid-level measurement2015223849010.1016/j.sna.2014.12.0272-s2.0-84921511379RanY.XiaL.NiuD.WenY.YuC.LiuD.Design and demonstration of a liquid level fiber sensor based on self-imaging effect2016237414610.1016/j.sna.2015.11.0182-s2.0-84948441756ZhangX.PengW.LiuZ.GongZ.Fiber optic liquid level sensor based on integration of lever principle and optical interferometry2014621710.1109/JPHOT.2014.23102082-s2.0-84920739293LiuB.WangD. Y.WangA.Liquid-surface-level sensing based on transverse pulse train technique20161682317232110.1109/JSEN.2016.25216592-s2.0-84962110291NakanoA.NishizuT.Experimental study of liquid level gauge for liquid hydrogen using Helmhotz resonance technique201674148GongC. S. A.ChiuH. K.HuangL. R.LinC. H.HsuZ. D.TuP. H.Low-cost comb-electrode capacitive sensing device for liquid-level measurement20161692896289710.1109/JSEN.2016.25246962-s2.0-84963865453ZhangH.-X.HouY.-L.FengL.-S.SuS.ZhangJ.-W.LiuJ.LiuW.-Y.LiuJ.XiongJ.-J.Polymer optical fiber continuous liquid level sensor for dynamic measurement20151595238524210.1109/JSEN.2015.24381532-s2.0-84937858453KarimiM. A.ArsalanM.ShamimA.A low cost, printed microwave based level sensor with integrated oscillator readout circuitry2017 IEEE MTT-S International Microwave Symposium (IMS)2017Honololu, HI, USA1742174510.1109/MWSYM.2017.80589802-s2.0-85032465075ChiX.KeX.XuW.Optical fibre liquid sensor for cryogenic propellant mass measurement201955527828010.1049/el.2018.73412-s2.0-85062707546NieR.GuoW.LuoY.LiW.XiaM.YangK.Optical liquid-level sensor based on a designed light guide plate201929635235610.1016/j.sna.2019.07.0452-s2.0-85069651680IslamT.KhanS. A.KhanM. F. A.MukhopadhyayS. C.A relaxation oscillator-based transformer ratio arm bridge circuit for capacitive humidity sensor201564123414342210.1109/TIM.2015.24594732-s2.0-84959575144MohamadE. J.RahimR. A.RahimanM. H. F.AmeranH. L. M.WahabY. A.MarwahO. M. F.Analysis of crude palm oil composition in a chemical process conveyor using electrical capacitance tomography201650576410.1016/j.flowmeasinst.2016.06.0112-s2.0-84974594029ThomasK. A.NairS.KumarA. R.NatarajanV.JohnR.Application of fringe field capacitance sensor for the study of water permeation in organic coatings201613582983510.1007/s11998-016-9795-32-s2.0-84976312766FuchsA.ZanglH.HollerG.MukhopadhyayS. C.GuptaG. S.Capacitance-based sensing of material moisture in bulk solids: applications and restrictions2008Berlin, HeidelbergSpringer235248TanC.LiP.DaiW.DongF.Characterization of oil-water two-phase pipe flow with a combined conductivity/capacitance sensor and wavelet analysis201513415316810.1016/j.ces.2015.04.0462-s2.0-84929571862ZhaiL.JinN.GaoZ.WangZ.Liquid holdup measurement with double helix capacitance sensor in horizontal oil-water two-phase flow pipes201523126827510.1016/j.cjche.2014.10.0102-s2.0-84927602245AsencioK.Bramer-EscamillaW.GutiérrezG.SánchezI.Electrical capacitance sensor array to measure density profiles of a vibrated granular bed20152701910.1016/j.powtec.2014.10.0032-s2.0-84949140993ParkK.-W.KimH. C.High accuracy pressure type liquid level measurement system capable of measuring densityTENCON 2015 - 2015 IEEE Region 10 Conference2015Macao, China10.1109/TENCON.2015.73729252-s2.0-84962136639KimJ.-Y.LeeJ.-H.BaeS.-E.PaekS.KimS. H.KimT.-J.ParkT.-H.Automated high-temperature liquid level measurement system using a dynamic tube pressure technique201749303510.1016/j.jiec.2016.10.0412-s2.0-85011933925LiC.NingT.ZhangC.LiJ.WenX.PeiL.GaoX.LinH.Liquid level measurement based on a no-core fiber with temperature compensation using a fiber Bragg grating2016245495310.1016/j.sna.2016.04.0462-s2.0-84968542368SanthoshK. V.RoyB. K.A practically validated adaptive calibration technique using optimized artificial neural network for level measurement by capacitance level sensor201548721722410.1177/00202940155959982-s2.0-84960503570WoeckelS.ArndtH.SteinmannU.AugeJ.LucklumR.Acoustic clamp-on liquid level detection in case of transducer misalignment20151201201120410.1016/j.proeng.2015.08.7952-s2.0-84984940609LiuS.TianJ.LiuN.XiaJ.LuP.Temperature insensitive liquid level sensor based on anti-resonant reflecting guidance in silica tube201634225239524310.1109/JLT.2016.26110072-s2.0-85013489538LiptakB.20044th EditionCRC PressMurtyD. V. S.2008PHIIosselY.KochanovE.StrunskiiM.1971Ft. Belvoir: Defense Technical Information CenterFrancoS.2002New YorkMcGraw-HillMitchellH. B.2007SpringerFausettL.2004Pearson Education