# Light Path Model of Fiber Optic Liquid Level Sensor Considering Residual Liquid Film on the Wall

Authors: Zhijun Zhang; Shiwei Zhang
Journal: Journal of Sensors
 (2015)

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## Abstract

The working principle of the refractive-type fiber optic liquid level sensor is analyzed in detail based on the light refraction principle. The optic path models are developed in consideration of common simplification and the residual liquid film on the glass tube wall. The calculating formulae for the model are derived, constraint conditions are obtained, influencing factors are discussed, and the scopes and skills of application are analyzed through instance simulations. The research results are useful in directing the correct usage of the fiber optic liquid level sensor, especially in special cases, such as those involving viscous liquid in the glass tube monitoring.


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## Body

## 1. Introduction

Liquid level monitoring is necessary in the industry and in the scientific research field [1]. The designs of liquid level sensors indicate the preset height of liquid levels, including magnetic [2], vibrant, capacitive [3], microwave [4], ultrasonic [5], and photoelectric liquid level sensor [6, 7]. The traditional glass tube liquid level gauge is widely utilized in simple structures for clear indication and visual observation [8, 9]. When a glass tube liquid level gauge is combined with a fiber optic sensor, a type of fiber optic liquid level sensor is formed. It includes the optical emission fiber, optical acceptance fiber, light source, optical modulator, amplifier, and glass tube liquid level gauge [10, 11]. The advantage of this sensor is that it can achieve genuine noncontact liquid level monitoring. The additional sensor elements, such as float or fiber, are not required to to be set in the liquid [12–16]. The micro size of the optic fiber enhances the accuracy of liquid level monitoring. The transformation of old equipment, which consists only of the glass tube liquid level gauge and which works by relying on the observations of the naked eye, into automatic liquid level monitoring by adding fiber optic sensors to the outside of the glass tube is convenient. The fiber optic liquid level sensor has the characteristics of fast response, corrosion resistance, electrical insulation, and small volume as well as the ability to easily compose the remote monitoring network with the fiber optic transmission system. Coupled with the high sensitivity of the electronic amplifier, this sensor possesses outstanding advantages in terms of antielectromagnetic interference capability and high sensitivity [17, 18].As the advantage of fiber optic liquid level sensor, the study, and application are wide, a noncontact fiber optic liquid level sensor based on the phenomenon of reflective concept is presented [19]. The device consists of fiber optic transmitter, fiber optic probe, floating reflector, photodiode detector, and digital multimeter. A simple intensity-modulated fiber optic sensor is developed based on frustrated total internal reflection effect caused by refractive index change of a medium surrounding an optical fiber [20]. An optical fiber sensor liquid level based on light intensity modulation and such modulation results from alteration of total internal reflection into partial reflection at the interface are reported [21]. A liquid level sensor based on the refractive-index sensitivity of long-period fiber optic gratings is proposed and demonstrated. The form of the transmission spectrum of the long-period grating is dependent on the fraction of the length of the long-period grating that is surrounded by the liquid [7]. A fiber optic level sensor with special microoptical refractometric transducer is designed to measure the level of liquid propane-butane in a relatively short range (60 cm) in the top part of storage tanks at oil refineries [22]. A micro change in level using plastic optical fiber sensor is demonstrated [23]. This sensor operates on light intensity modulation and such modulation results due to displacement of the reflector floating on the liquid. An experimental realization of a simple all-fiber optic sensor for liquid level measurement is demonstrated. It is an intensity-modulated on-off switching sensor whose operating principle is based on the frustrated total internal reflection effect caused by the refractive-index change of the surrounding medium [24]. An intensity-based fiber optic liquid level sensor for point measurement is described. The sensing principle is based on the total internal reflection of light, which is disturbed by contact with a liquid [25]. A simple and compact reflective liquid level sensor based on modes conversion in the thin-core fiber incorporating one tilted fiber Bragg grating (TFBG) is proposed and experimentally demonstrated [26]. A new and simple fiber optic liquid level sensor based on light intensity modulation was presented when rising and falling mode of liquid level causes coupling optical path distance variation between two optical fibers [27].A fiber optic liquid level sensor that is conducted by a combination of optical interferometer and lever principle is presented [12]. Its sensing unit is a Mach-Zehnder interferometer (MZI). The measuring equipment is composed of a rotatable lever and a fixed link. A fiber optic liquid level sensor based on multimode interference (MMI) effects is proposed and demonstrated [13, 17]. The MMI and self-image effects can be effectively applied for multiplexed liquid level sensing, because the natural response as a band-pass filter for each sensor is clearly distinct from each other, in the case for several sensors working at the same time. A simple and low-cost discrete liquid level measurement system which consists of a group of plastic optical fiber segments, which are aligned coaxially and spaced equally, is present [28]. A novel optical liquid level sensor based on polarization-maintaining fiber (PMF) modal interferometer with waist enlarge splicing is proposed [29]. The design and packaging of simple, small, and low-cost sensor heads, used for continuous liquid level measurement using uniformly thinned (etched) optical fiber Bragg grating (FBG) are proposed [30]. An asymmetric Fabry-Perot fiber optic pressure sensor is capable of precisely measuring liquid levels [31]. They are directly proportional to pressures that can modulate cavity length of Fabry-Perot cavity. An efficient approach to develop large-range liquid level sensors based on an extrinsic Fabry-Perot optical fiber interferometer with an all-fused-silica structure and CO2 laser heating fusion bonding technology is also presented [32].Although the principle of the refracting-type fiber optic liquid level sensor is simple and clear, the method and rules for its application, such as the arrangement of both emission and acceptance optical fibers, are quite complex. In practice, the position and angle of the optical fibers are determined by driftless tests in most cases because of the lack of quantitative theoretical basis. However, blind search does not always work, and theoretical analysis is necessary in special cases of applications.


## 2. Problem Description

The study in present paper is from the practical problem encountered when they developed the “automatic vapor vacuum pump performance measurement system” patented in China (Chinese Patent: ZL200910012545.3) [33]. According to the performance measuring method of vapor vacuum pump which is recommended by both the international standard ISO 1607-1 (1993) and the Chinese standard GB/T 19955.1 (2005), the measurement of volume rate of flow (pumping speed) needs to monitor the liquid level in a series of glass tubes with given diameter. In the experiment, the liquid level is forced to rise and drop several times between the two preset heights which is 20 cm. The change of liquid level is because of the change of pressure on the top of liquid. The inner diameters of the glass tubes in present study are 1.5 mm, 3 mm, and 5 mm according to above standard. The liquid medium in the tube is a type of industry transformer oil with lower saturation vapor pressure limiting oil pollution for vapor vacuum pump. The oil is transparent and has higher viscosity. In order to realize the automatic test, the fiber liquid level sensors are the best method as above mentioned. The two fiber optic liquid level sensors are set and provide the responsive signals. The device photograph of fiber optic liquid level device is show in Figure 1.Figure 1
The photograph of fiber optic liquid level sensor in present study.The refracting-type fiber optic liquid level sensor was developed based on the principle of light refraction. The incidence detecting light beam (AB in Figure 2) from the optical emission fiber arrives at the outer surface of the glass tube obliquely and passes through the glass tube sinuously. The light beam (GTHT or GDHD in Figure 2) is then received by the optical acceptance fiber, which is located on the other side of the glass tube at a slanted angle. The optical path is a zigzag line across the glass tube because the light beam is refracted at each interface between two transparent media with different refractive indices. The light path through the liquid (ABCFDGDHD in Figure 2) is different from the path through the gas (ABCFTGTHT in Figure 2) because of the difference in the refractive indices of the liquid and gas inside the glass tube. Therefore, the position and angle of the emergent detecting light beam passing through the liquid are different from those of the beam passing through the gas. If the optical acceptance fiber is arranged at a position and angle corresponding to the emergent detecting light beam passing through the liquid with the possibility of receiving the light signal, the emergent detecting light beam passing through the gas will not be received and vice versa. Thus, the refracting-type fiber optic liquid level sensor works well when the liquid is good and transparent.Figure 2
Light path models of three conditions: gas in glass tube (ABCFTGTHT), liquid medium in glass tube (ABCFDGDHD), and residual liquid film on the glass wall (ABCDEFGH).However, the optical acceptance fiber cannot frequently receive the emergent light in time at expected emergent point (GTHT in Figure 2) because the light path is changed to GH as in Figure 2. The change is the residual oil film on the tube wall. It is the medium changing the light path. The thickness of oil is changed with the time due to which GH is changed. The oil film effect is not known well until now. The theory study would clarify the detail information and maybe would guide the application of sensors.In this paper, the light path model considering the residual liquid film is established. The derivation and analysis are performed to meet the requirements for theoretical research provided above. The working mechanism of the refracting-type fiber optic liquid level sensor with glass liquid level is discovered.


## 3. Review of Simplified Model of Optical Path

The simplified model of optical path calculation [33] is shown with dotted line in Figure 1. It is the cross-section of the glass tube. Glass tube center O is considered to be the coordinate origin; a rectangular coordinate system XOY is established. The darker part is the cylindrical wall of the glass tube, the outer radius of which is RB and the inner radius of which is RC. At the circle with radius RA, point A is the incident point of the light and point H is the emergent point of the light. Lastly, the original positioning parameter of the light path is set. The coordinate of incident point B is selected as the positioning point of the light path. In the rectangular coordinate system XOY, the coordinate of point B is (xB=-RB,yB=0).The parameters and symbols of the various angles in Figure1 are defined as follows.(1) Azimuth: the angle between the negativeX axis of the coordinate and the normal line at each turning point (ABCFGH) in the light path, denoted by γ with a subscript, such as γA, γB, and γC.(2) Incidence angle: the angle between the incident light and the normal line at each turning point (ABCFGH) in the light path, denoted by α with a subscript, such as αA,αB, and αC.(3) Refraction angle: the angle between the refraction light and the normal line at each turning point (ABCFGH) in the light path, denoted by β with a subscript, such as βB; the refraction angle at point C is especially distinguished when the refractive indices of the media in the tube are different, such as with βCT and βCD.(4) The total deflection angle: also called total acceptance angle, this angle is the azimuth difference between light incident pointA and emergent point HD or HT; when the optically denser medium nD is in the tube, ηD is noted as the total deflection angle; when the optically thinner medium nT is in the tube, ηT is noted as the total deflection angle; the difference is expressed as the deflection angle difference denoted by Δη.Four kinds of optical media divided by the optical refractive index are involved in the glass tube liquid level gauge. Their refractive indices are denoted bynA,nG,nD, and nT in outward to inward turns. The medium outside the tube that nA stands for is generally air; therefore, nA≈1. However, this relationship is not directly used to simplify the formulae in the following derivation and calculation. nG stands for the refraction index of the glass tube. Two kinds of media are present in the tube, and their refraction indices must be different, which is the physical basis of the method introduced in this paper. The medium with the larger refractive index is called the optically denser medium denoted by nD; the medium with the less refractive index is called the optically thinner medium denoted by nT. Both nD and nT may be less than nG. The optically denser medium is typically a liquid, whereas the optically thinner medium is typically a gas.The detecting light emitted from the emission fiber goes through this plane. Incident lightAB enters the tube at angle αB. The outer surface is normal at point B. When gas is in the tube, the light refracts at points B,C,FT, and GT on the inside and outside surfaces of the tube wall when light passes through the tube. The light is finally received by the optical acceptance fiber at point HT. By contrast, the refraction angle of the light changes at point C on the inside of the tube wall when the tested liquid in the tube reaches the height of the light and when the refractive index changes, resulting in the change in the path followed by the light. The entire light path changes to ABCFDGDHD. As point HD deflects from the original accepting position of point HT, the optical acceptance fiber at point HT can no longer receive the light signal. Thus, a great contrast with regard to the existence of light at the points HD and HT is present before and after the increase in the liquid level, thereby improving the responses sensitivity especially in transparent media.


## 4. Light Path Model Considering Residual Liquid Film on the Wall

The liquid in the tube is usually characterized by high viscosity and large surface tension. The signal response when the liquid surface rises and passes the detecting light position is unaffected. However, a residual layer of liquid film appears on the glass wall when the liquid drops and merely passes the detecting light position. Thus, the incident light must first pass the liquid film to arrive at the gas area in the tube. The emergent light must also pass through the liquid film to pass the glass wall; therefore, the detecting light must pass through the liquid film twice and refract on the interface. In this period of time, the emergent light angle deviates fromηT when only gas is present in the tube as predicted in the simplified model. Over time, the liquid on the wall falls automatically because of gravity, thereby making the liquid film thinner and the refraction of the detecting light smaller until the tube is full of gas and the angle position of the emergent light returns to ηT. The problem of residual liquid film on the wall during the falling process directly causes errors in liquid level monitoring. Therefore, special research on this phenomenon is necessary.The light path calculation model considering the residual liquid film on the wall adopts the basic assumption and parameter definition of the previous simplified model [33]. The graph of the light path model shown with solid line in Figure 1 was established based on [33]. The only change is the addition of a layer of liquid film in the glass tube, which is a circle concentric with the inner radius of RD. This addition causes the detecting light path in the glass tube to change from line CFT into three line segments CD,DE, and EF in present study in Figure 2.


### 4.1. Hypothesis

(1) The outer and inner surfaces of the glass tube are standard coaxial cylindrical surfaces. The shape error is ignored.(2) All materials involved in the light path are isotropic homogeneous transparent optical media. The detecting light in various media is linear, and the light path obeys the refraction law at the interfaces of the two kinds of media.(3) The size of the light can be ignored; that is, it can be regarded as a geometric straight line because it is very fine relative to the tube size.


### 4.2. Coordinate, Azimuth, and Incident Angle of PointA

PointA is the intersecting point of the incident light y=kB(x+RB) with the circle x2+y2=RA2 where the optical emission fiber is located. The slope of the incident light is kB=tanαB, and the coordinate of point A is(1)xA=-RB·cos⁡αB·RARB2-sin2αB1/2+sin2αB,yA=RB·sinαB·cos⁡αB-RARB2-sin2αB1/2.The azimuth of pointA can be expressed by the slope of line y=fA·x as(2)tanγA=fA=yAxA=sinαB·RA/RB2-sin2αB1/2-cos⁡αBcos⁡αB·RA/RB2-sin2αB1/2+sin2αB.At pointA, the incidence angle αA is(3)tanαA=kB-fA1+kBfA=sinαBRA/RB2-sin2αB1/2.


### 4.3. Refraction Angle of PointB

At the interface of pointB, nAsinαB=nGsinβB according to the refraction law. The refraction angle of point B can thus be obtained as follows: (4)sinβB=nAnGsinαBor(5)tanβB=nA/nG·sinαB1-nA/nG2·sin2αB1/2.


### 4.4. Coordinate, Azimuth, and Incident Angle of PointC

PointC is the intersecting point of the refracted light from point By=kC(x+RB) with the circle x2+y2=RC2 on the inner wall of the glass tube. The slope of the refracted light is kC=tanβB, and the coordinate of point C is(6)xC=-RB·cos⁡βB·RC/RB2-sin2βB1/2+sin2βB,yC=RB·sinβB·cos⁡βB-RC/RB2-sin2βB1/2.The azimuth of pointC can be expressed by the slope of line y=fCx as(7)tanγC=fC=-yCxC=sinαBnGnA2-sin2αB1/2-RCnGRBnA2-sin2αB1/2·nGnA2-sin2αB1/2-RCnGRBnA2-sin2αB1/2·nGnA2-sin2αB1/2RCnGRBnA2-sin2αB1/2+sin2αB·RCnGRBnA2-sin2αB1/2+sin2αB-1.At pointC, the incidence angle αC is(8)tanαC=kC-fC1+kCfC=sinαBRCnG/RBnA2-sin2αB1/2or(9)sinαC=RBnARCnGsinαB.


### 4.5. Refraction Angle of PointC

The two kinds of media with different refractive indices in the tube correspond to two different refraction angles at pointC; therefore, the light path after point C also has two possible paths. When the refractive index of the medium in the tube is nT,nGsinαC=nTsinβCT according to the refraction law and (8). The calculation formula of the refraction angle at point C is(10)sinβCT=RBnARCnTsinαBor(11)tanβCT=sinαBRCnT/RBnA2-sin2αB1/2.When the refractive index of the medium in the tube becomesnD, the refraction angle at point C as calculated by the refraction law and (8) is(12)sinβCD=RBnARCnDsinαBor(13)tanβCD=sinαBRCnD/RBnA2-sin2αB1/2.


### 4.6. Coordinate, Azimuth, Incident, and Refraction Angles of PointD

PointD is the intersecting point of refraction line y=kD(x-xC)+yC from point C and inner surface circle x2+y2=RD2 of the liquid film. The slope of the refraction line is kD=tan(βCD-γC), the radius of the circle is RD=RC-δ, and the thickness of the liquid film is δ.The coordinate of pointD in the XOY coordinates can be obtained by the following simplification: (14)xD=-sin⁡βCD-γC·sinβCD·RC-cos⁡⁡βCD-γC·RD2-sin2βCD·RC21/2,yD=cos⁡⁡βCD-γC·sinβCD·RC-sin⁡βCD-γC·RD2-sin2βCD·RC21/2.The same applies to the relationship as follows:(15)yD-kDxD=yC-kDxC.AzimuthγD of point D is expressed by the slope of line y=fDx as(16)tanγD=-fD=-yDxD=sinβCD-tan(βCD-γC)·(RD/RC)2-sin2βCD1/2tan(βCD-γC)·sinβCD+(RD/RC)2-sin2βCD1/2.The incidence angleαD of point D is determined by the following equation:(17)tanαD=kD-fD1+kDfD=kDxD-yDxD+kDyD.This angle can be obtained by simplification as follows:(18)sinαD=RCRDsinβCD=RBnARDnDsinαB.The refraction angleβD of point D can be obtained by the refraction law nDsinαD=nTsinβD. Consider(19)sinβD=nDnTsin⁡αD=RBnARDnTsinαBor(20)tanβD=sinαBRDnT/RBnA2-sin2αB.


### 4.7. Total Deflection Angle

As shown in Figure1, the total deflection angle from incident point A to emergent point H with the residual liquid film is (21)η=π-2βD-γD-γA.The following have already been calculated at this point:(22)βD=arctansinαBRDnT/RBnA2-sin2αB1/2,γD=arctansinβCD-tan⁡βCD-γCRDRC2-sin2βCD1/2+RDRC2-sin2βCD1/2-1·RDRC2-sin2βCD1/2·tan(βCD-γC)·sinβCDRDRC2-sin2βCD1/2+RDRC2-sin2βCD1/2-1,γA=arctansinαB·RA/RB2-sin2αB1/2-cos⁡αBcos⁡αB·RA/RB2-sin2αB1/2+sin2αB.


### 4.8. Constraints of the Model

When a residual liquid film exists on the wall, the constraints must be considered to avoid the total reflection of light as in the simplified model. In this situation, the total reflection of light is likely to occur at pointD; therefore, the condition of avoiding the total reflection is(23)sinαD<nTnDor(24)sinαB<RDnTRBnA.


## 4.1. Hypothesis

(1) The outer and inner surfaces of the glass tube are standard coaxial cylindrical surfaces. The shape error is ignored.(2) All materials involved in the light path are isotropic homogeneous transparent optical media. The detecting light in various media is linear, and the light path obeys the refraction law at the interfaces of the two kinds of media.(3) The size of the light can be ignored; that is, it can be regarded as a geometric straight line because it is very fine relative to the tube size.


## 4.2. Coordinate, Azimuth, and Incident Angle of PointA

PointA is the intersecting point of the incident light y=kB(x+RB) with the circle x2+y2=RA2 where the optical emission fiber is located. The slope of the incident light is kB=tanαB, and the coordinate of point A is(1)xA=-RB·cos⁡αB·RARB2-sin2αB1/2+sin2αB,yA=RB·sinαB·cos⁡αB-RARB2-sin2αB1/2.The azimuth of pointA can be expressed by the slope of line y=fA·x as(2)tanγA=fA=yAxA=sinαB·RA/RB2-sin2αB1/2-cos⁡αBcos⁡αB·RA/RB2-sin2αB1/2+sin2αB.At pointA, the incidence angle αA is(3)tanαA=kB-fA1+kBfA=sinαBRA/RB2-sin2αB1/2.


## 4.3. Refraction Angle of PointB

At the interface of pointB, nAsinαB=nGsinβB according to the refraction law. The refraction angle of point B can thus be obtained as follows: (4)sinβB=nAnGsinαBor(5)tanβB=nA/nG·sinαB1-nA/nG2·sin2αB1/2.


## 4.4. Coordinate, Azimuth, and Incident Angle of PointC

PointC is the intersecting point of the refracted light from point By=kC(x+RB) with the circle x2+y2=RC2 on the inner wall of the glass tube. The slope of the refracted light is kC=tanβB, and the coordinate of point C is(6)xC=-RB·cos⁡βB·RC/RB2-sin2βB1/2+sin2βB,yC=RB·sinβB·cos⁡βB-RC/RB2-sin2βB1/2.The azimuth of pointC can be expressed by the slope of line y=fCx as(7)tanγC=fC=-yCxC=sinαBnGnA2-sin2αB1/2-RCnGRBnA2-sin2αB1/2·nGnA2-sin2αB1/2-RCnGRBnA2-sin2αB1/2·nGnA2-sin2αB1/2RCnGRBnA2-sin2αB1/2+sin2αB·RCnGRBnA2-sin2αB1/2+sin2αB-1.At pointC, the incidence angle αC is(8)tanαC=kC-fC1+kCfC=sinαBRCnG/RBnA2-sin2αB1/2or(9)sinαC=RBnARCnGsinαB.


## 4.5. Refraction Angle of PointC

The two kinds of media with different refractive indices in the tube correspond to two different refraction angles at pointC; therefore, the light path after point C also has two possible paths. When the refractive index of the medium in the tube is nT,nGsinαC=nTsinβCT according to the refraction law and (8). The calculation formula of the refraction angle at point C is(10)sinβCT=RBnARCnTsinαBor(11)tanβCT=sinαBRCnT/RBnA2-sin2αB1/2.When the refractive index of the medium in the tube becomesnD, the refraction angle at point C as calculated by the refraction law and (8) is(12)sinβCD=RBnARCnDsinαBor(13)tanβCD=sinαBRCnD/RBnA2-sin2αB1/2.


## 4.6. Coordinate, Azimuth, Incident, and Refraction Angles of PointD

PointD is the intersecting point of refraction line y=kD(x-xC)+yC from point C and inner surface circle x2+y2=RD2 of the liquid film. The slope of the refraction line is kD=tan(βCD-γC), the radius of the circle is RD=RC-δ, and the thickness of the liquid film is δ.The coordinate of pointD in the XOY coordinates can be obtained by the following simplification: (14)xD=-sin⁡βCD-γC·sinβCD·RC-cos⁡⁡βCD-γC·RD2-sin2βCD·RC21/2,yD=cos⁡⁡βCD-γC·sinβCD·RC-sin⁡βCD-γC·RD2-sin2βCD·RC21/2.The same applies to the relationship as follows:(15)yD-kDxD=yC-kDxC.AzimuthγD of point D is expressed by the slope of line y=fDx as(16)tanγD=-fD=-yDxD=sinβCD-tan(βCD-γC)·(RD/RC)2-sin2βCD1/2tan(βCD-γC)·sinβCD+(RD/RC)2-sin2βCD1/2.The incidence angleαD of point D is determined by the following equation:(17)tanαD=kD-fD1+kDfD=kDxD-yDxD+kDyD.This angle can be obtained by simplification as follows:(18)sinαD=RCRDsinβCD=RBnARDnDsinαB.The refraction angleβD of point D can be obtained by the refraction law nDsinαD=nTsinβD. Consider(19)sinβD=nDnTsin⁡αD=RBnARDnTsinαBor(20)tanβD=sinαBRDnT/RBnA2-sin2αB.


## 4.7. Total Deflection Angle

As shown in Figure1, the total deflection angle from incident point A to emergent point H with the residual liquid film is (21)η=π-2βD-γD-γA.The following have already been calculated at this point:(22)βD=arctansinαBRDnT/RBnA2-sin2αB1/2,γD=arctansinβCD-tan⁡βCD-γCRDRC2-sin2βCD1/2+RDRC2-sin2βCD1/2-1·RDRC2-sin2βCD1/2·tan(βCD-γC)·sinβCDRDRC2-sin2βCD1/2+RDRC2-sin2βCD1/2-1,γA=arctansinαB·RA/RB2-sin2αB1/2-cos⁡αBcos⁡αB·RA/RB2-sin2αB1/2+sin2αB.


## 4.8. Constraints of the Model

When a residual liquid film exists on the wall, the constraints must be considered to avoid the total reflection of light as in the simplified model. In this situation, the total reflection of light is likely to occur at pointD; therefore, the condition of avoiding the total reflection is(23)sinαD<nTnDor(24)sinαB<RDnTRBnA.


## 5. Results and Discussion

Figure3 shows the calculated results of total deflection angle ηD for transformer oil, total deflection angle ηT for the vacuum without a residual oil film, and total deflection angle ηi for the vacuum with residual oil films of different thickness (η1 for δ=0.05mm, η2 for δ=0.1mm, and η3 for δ=0.15mm). The denser light medium in the tube is a type of industry transformer oil with nD=1.46, whereas the thinner light medium in the tube is a vacuum with nT=1. The other structure parameters are RA=12mm, RB=6mm, and RC=1.5mm. The difference between ηT and ηi shows the effect of the residual oil film and explains the missing emergent light at point HT.Figure 3
Variation inηD,ηT, and ηi with incident angle αB, for example.


### 5.1. Influence of Liquid Film Thickness

Total deflection angleη with the residual liquid film on the wall, which is calculated with (21), is always less than total deflection angle ηT without the residual liquid film calculated with the equation in [33]. As shown in Figure 3, the thicker the film, the greater the difference between ηT and η. Thus, deflection angle difference Δη′=ηD-η between optical thickness and the thinner media is large. When the thickness of the residual liquid film decreases, the light at emergent point H is near point HT, and η is close to ηT.


### 5.2. Influence of the Incident Angle

As shown in Figure3, the larger initial detecting light incident angle αB of detecting light is, the greater the difference between H and HT is under the condition of similar liquid film thickness; this phenomenon is accompanied by the increase in gas-liquid media deflection angle difference Δη′=ηD-η. A critical incidence angle αBK=arcsin((RDnT)/(RBnA)) is determined with (24) for each specified film thickness. The determined critical incidence angle is always smaller than critical incidence angle αBTmax⁡=arcsin((RCnT)/(RBnA)) which does not consider the residual liquid film. When actual incidence angle αB<αBK, actual total deflection angle η can be calculated with (21). When αBK<αB<αBTmax⁡, the total detecting light reflection occurs on the liquid film interface, and the emergent light is not emitted at gas emergent point HT until the liquid film disappears.


### 5.3. Critical Incidence Angle at PointB

The analysis above provides a very important conclusion: in the presence of residual liquid film on the tube wall, the receipt of the emergent light at emergent pointHT is unreliable as mentioned in the simplified model. The best substitution method in this situation is to select HD as the light emergent point, which corresponds to the liquid in the glass tube. Total deflection angle η can be calculated with (21). Thus, the effect of the residual liquid film on emergent points H and HT need not be considered even with regard to the possibility of the occurrence of total reflection when gas is in the tube. The only requirement is to ensure that the liquid in tube is transparent and that total reflection does not occur when the detecting light passes through the liquid. Therefore, the maximum allowable incident angle (critical incidence angle) at point B is(25)αBDmax⁡=arcsinnDRCnARB.


## 5.1. Influence of Liquid Film Thickness

Total deflection angleη with the residual liquid film on the wall, which is calculated with (21), is always less than total deflection angle ηT without the residual liquid film calculated with the equation in [33]. As shown in Figure 3, the thicker the film, the greater the difference between ηT and η. Thus, deflection angle difference Δη′=ηD-η between optical thickness and the thinner media is large. When the thickness of the residual liquid film decreases, the light at emergent point H is near point HT, and η is close to ηT.


## 5.2. Influence of the Incident Angle

As shown in Figure3, the larger initial detecting light incident angle αB of detecting light is, the greater the difference between H and HT is under the condition of similar liquid film thickness; this phenomenon is accompanied by the increase in gas-liquid media deflection angle difference Δη′=ηD-η. A critical incidence angle αBK=arcsin((RDnT)/(RBnA)) is determined with (24) for each specified film thickness. The determined critical incidence angle is always smaller than critical incidence angle αBTmax⁡=arcsin((RCnT)/(RBnA)) which does not consider the residual liquid film. When actual incidence angle αB<αBK, actual total deflection angle η can be calculated with (21). When αBK<αB<αBTmax⁡, the total detecting light reflection occurs on the liquid film interface, and the emergent light is not emitted at gas emergent point HT until the liquid film disappears.


## 5.3. Critical Incidence Angle at PointB

The analysis above provides a very important conclusion: in the presence of residual liquid film on the tube wall, the receipt of the emergent light at emergent pointHT is unreliable as mentioned in the simplified model. The best substitution method in this situation is to select HD as the light emergent point, which corresponds to the liquid in the glass tube. Total deflection angle η can be calculated with (21). Thus, the effect of the residual liquid film on emergent points H and HT need not be considered even with regard to the possibility of the occurrence of total reflection when gas is in the tube. The only requirement is to ensure that the liquid in tube is transparent and that total reflection does not occur when the detecting light passes through the liquid. Therefore, the maximum allowable incident angle (critical incidence angle) at point B is(25)αBDmax⁡=arcsinnDRCnARB.


## 6. Conclusions

The optical fiber liquid level sensor composed of a glass tube level gauge and a fiber optic sensor can monitor transparent liquid level in a thin glass tube through the method based on the light refraction principle. The acceptance fiber should be set at the emergent point of the optically denser medium in the tube when the influence of the residual liquid film on the tube wall cannot be ignored to receive the emergent light signal. The total reflection of the detecting light in the optically thinner medium can generally be adopted by increasing the incident angle to within the constraint condition of the optically denser medium.



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*Source: 729507-2015-03-08.xml*