# Static Characteristics of a Linear Bipotentiometer Sensor

Authors: Chang-Zhong Chen; Yong Cai; Tao Fan; Ping He
Journal: Security and Communication Networks
 (2021)

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## Abstract

In this paper, the structure and the working principle of an existing linear potentiometer sensor are introduced; furthermore, the structure and circuit connection method of a new linear bipotentiometer sensor is proposed. The sensitivity, step error, and load characteristics of the existing potentiometer sensor and the linear bipotentiometer sensor are both studied and compared. The simulation results of their static characteristics show that the sensitivity of the linear bipotentiometer sensor is increased, the relative load error is greatly reduced, and the linearity is improved. Meanwhile, the measurement accuracy of the linear bipotentiometer sensor is effectively improved.


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## Body

## 1. Introduction

A sensor is a device that can sense the needed signal and convert it into an available output signal according to certain rules [1–3]. The sensor is the key part of the measurement in control systems [4, 5]. If the sensor accuracy is not high and the dynamic performance is poor, the whole system will be difficult to operate normally. Therefore, the working reliability, static precision, and dynamic performance of the sensor are the most basic indexes [6].A linear potentiometer sensor is a kind of resistance sensor, which can be used to measure pressure, displacement, acceleration, and other parameters [7, 8]. An existing linear potentiometer sensor is composed of a linear potentiometer, which has the advantages of simple structure and large output signal, but its load error is relatively large and linearity is relatively poor, especially when the detection input is in the half range, its load error is the largest, and it is difficult to achieve high precision measurement [9, 10]. In order to improve this shortcoming, the load characteristic of the potentiometric displacement sensor is automatically compensated by a general-purpose integrated operational amplifier and an integrated voltage regulator in the paper [11]. In [12], the nonlinear errors are lowered by a magnetic levitation control system and an aerostatic bearing device in the vertical and horizontal directions.In order to improve the application performance of the existing linear potentiometer sensor, many methods are proposed [13–15], and some of them are effective. In this paper, based on an existing linear potentiometer sensor, a new scheme of a linear bipotentiometer sensor is proposed, the sensitive part of which is composed of two identical linear potentiometers. Under the same measuring conditions, some static characteristics of both the existing linear potentiometer sensor and the linear bipotentiometer sensor are studied, simulated, analyzed, and compared, and the conclusion of the linear bipotentiometer sensor is drawn. The static characteristics of the linear bipotentiometer sensor are improved, the relative load error is reduced, and the measurement accuracy is improved.The main contributions of this paper focus on the following three aspects:(i)
A new linear bipotentiometer sensor is designed relative to the existing linear potentiometer sensor.(ii)
Some static characteristics of the linear bipotentiometer sensor are studied relative to the existing linear potentiometer sensor.(iii)
The static characteristics of the two kinds of sensors are simulated, and the conclusion is drawn.The linear bipotentiometer sensor is a kind of sensor with improved structure, which is based on the existing linear potentiometer sensor. From the layout point of view, in this paper, firstly, the principle of the linear potentiometer is introduced, so is the circuit connection of the existing linear potentiometer sensor, which leads to the structure and circuit connection of the linear bipotentiometer sensor. Then, some static characteristics of the linear bipotentiometer sensor are analyzed and compared with the existing linear potentiometer sensor. Finally, numerical simulation of their static characteristics is carried out, and a conclusion is drawn.The rest of the paper is organized as follows. Section2 gives structures of a linear bipotentiometer sensor and an existing linear potentiometer sensor. On the basis of the sensor structure described above, the sensitivity, step error, and load characteristics of the existing linear potentiometer sensor and the linear bipotentiometer sensor are studied in Section 3. For verifying the theoretical results, numerical simulations are given in Section 4. At last, conclusions are presented in Section 5.


## 2. Structure of a Linear Bipotentiometer Sensor

A linear potentiometer sensor is a kind of resistance sensor that converts the change of measured physical quantity into the change of resistance value, which is to transform the mechanical linear displacement or angular displacement into a corresponding resistance output.


### 2.1. Linear Potentiometer

The linear potentiometer is the sensitive component of the linear potentiometer sensor. The schematic diagram of the linear potentiometer is shown in Figure1.Figure 1
Schematic diagram of linear potentiometer sensor. (1) Resistance wire. (2) Insulated framework. (3) Sliding arm.The linear potentiometer is made of resistance wire regularly and neatly wound on an insulated framework, and the resistance wire is very thin, and its resistance coefficient is very high. The resistance wire is alloy resistant with surface insulation. The insulating layer on the surface of the resistance wire is removed and polished to form a contact point, where the brush can slide on it smoothly. A sliding arm and an electric brush on it are moved along the potentiometer. The cross section of the framework is equal everywhere, and the distance between the resistance coils is equal. The structure diagram of the linear potentiometer is shown in Figure2; then, it can be concluded that(1)Rx=xLRmax,Rmax=2b+hnpA,n=Lt,where Rmax is the total resistance of the potentiometer, the distribution of which along the length is uniform, and the total length of which is L.x0<x<L, which is the length of brush movement, Rx is the resistance value corresponding to the brush movement x, b and h are the width and height of the framework, respectively, A is the cross-sectional area of the wire, the resistivity of which is ρ, the total number of winding turns of the potentiometer is n, and t is the distance between the resistance coils.Figure 2
Structure diagram of the linear potentiometer.


### 2.2. Principle of an Existing Linear Potentiometer Sensor

An existing linear potentiometer sensor is composed of a linear potentiometer, and its circuit connection is shown in Figure3.Figure 3
Circuit connection diagram of an existing linear potentiometer sensor.In Figure3, RL is the load resistance value, which may be the internal resistance of the display instrument, the input resistance of the amplifier circuit, or other loads. Ui is the input voltage of the sensor. Uo1 is the output voltage of the existing linear potentiometer sensor.


### 2.3. Structure and Principle of a Linear Bipotentiometer Sensor

The sensing element of a linear bipotentiometer sensor is composed of two identical linear potentiometers. These two potentiometers share one sliding arm, and there is an electric brush at each end of the sliding arm. The two brushes move on the two potentiometers with equal displacement at the same time; the resistance changes uniformly with the brush displacement; and the structure diagram of the linear bipotentiometer sensor is shown in Figure4. The two sides of the brush are not conductive, and the two ends of the output voltage are led out from both sides of the brush; its specific circuit connection is shown in Figure 5, where Uo2 is the output voltage of the linear bipotentiometer sensor, which is the output voltage from the two brush ends after the brush is shifted.Figure 4
Structure diagram of a linear bipotentiometer sensor.Figure 5
Circuit connection diagram of a linear bipotentiometer sensor.In the process of brush sliding, it can be concluded that(2)R1=R4=xLRmax,R2=R3=1−xLRmax,R1+R2=Rmax,R3+R4=Rmax.


## 2.1. Linear Potentiometer

The linear potentiometer is the sensitive component of the linear potentiometer sensor. The schematic diagram of the linear potentiometer is shown in Figure1.Figure 1
Schematic diagram of linear potentiometer sensor. (1) Resistance wire. (2) Insulated framework. (3) Sliding arm.The linear potentiometer is made of resistance wire regularly and neatly wound on an insulated framework, and the resistance wire is very thin, and its resistance coefficient is very high. The resistance wire is alloy resistant with surface insulation. The insulating layer on the surface of the resistance wire is removed and polished to form a contact point, where the brush can slide on it smoothly. A sliding arm and an electric brush on it are moved along the potentiometer. The cross section of the framework is equal everywhere, and the distance between the resistance coils is equal. The structure diagram of the linear potentiometer is shown in Figure2; then, it can be concluded that(1)Rx=xLRmax,Rmax=2b+hnpA,n=Lt,where Rmax is the total resistance of the potentiometer, the distribution of which along the length is uniform, and the total length of which is L.x0<x<L, which is the length of brush movement, Rx is the resistance value corresponding to the brush movement x, b and h are the width and height of the framework, respectively, A is the cross-sectional area of the wire, the resistivity of which is ρ, the total number of winding turns of the potentiometer is n, and t is the distance between the resistance coils.Figure 2
Structure diagram of the linear potentiometer.


## 2.2. Principle of an Existing Linear Potentiometer Sensor

An existing linear potentiometer sensor is composed of a linear potentiometer, and its circuit connection is shown in Figure3.Figure 3
Circuit connection diagram of an existing linear potentiometer sensor.In Figure3, RL is the load resistance value, which may be the internal resistance of the display instrument, the input resistance of the amplifier circuit, or other loads. Ui is the input voltage of the sensor. Uo1 is the output voltage of the existing linear potentiometer sensor.


## 2.3. Structure and Principle of a Linear Bipotentiometer Sensor

The sensing element of a linear bipotentiometer sensor is composed of two identical linear potentiometers. These two potentiometers share one sliding arm, and there is an electric brush at each end of the sliding arm. The two brushes move on the two potentiometers with equal displacement at the same time; the resistance changes uniformly with the brush displacement; and the structure diagram of the linear bipotentiometer sensor is shown in Figure4. The two sides of the brush are not conductive, and the two ends of the output voltage are led out from both sides of the brush; its specific circuit connection is shown in Figure 5, where Uo2 is the output voltage of the linear bipotentiometer sensor, which is the output voltage from the two brush ends after the brush is shifted.Figure 4
Structure diagram of a linear bipotentiometer sensor.Figure 5
Circuit connection diagram of a linear bipotentiometer sensor.In the process of brush sliding, it can be concluded that(2)R1=R4=xLRmax,R2=R3=1−xLRmax,R1+R2=Rmax,R3+R4=Rmax.


## 3. Static Characteristic Analysis of the Linear Potentiometer and Bipotentiometer Sensors

The research content of a kind of sensor includes many aspects, mainly including the basic characteristics, working principle, calibration, and interference factors of the sensor. The basic characteristics of the sensor include static and dynamic characteristics and also many specific characteristic indexes. The partial relationship is shown in Figure6. In this paper, the linear bipotentiometer sensor is a new structure potentiometer sensor compared with the existing linear potentiometer sensor; therefore, only the static characteristics different from the existing linear potentiometer sensor are studied, that is, the contents in the red box in Figure 6.Figure 6
Relationship diagram of partial research content of sensor.


### 3.1. No-Load Characteristic

As shown in Figure3, when the load resistance RL⟶∞, i.e., no load, the output voltage uo1 of the brush sliding from the initial position to x is as follows:(3)Uo1=UiRxRmax=xLUi.Whenx changes from 0 to L, the range of the output voltage Uo1 is 0,Ui.In Figure5, when the load resistance RL⟶∞, i.e., no load, the output voltage uo2 of the brush sliding from the initial position to x is as follows:(4)Uo2=x/LRmax−1−x/LRmaxRmaxUi=UiR1Rmax−R3Rmax=2xL−1Ui.Whenx changes from 0 to L, the range of the output voltage Uo2 is −Ui,Ui.According to the above analysis, the no-load output voltage range of the linear bipotentiometer sensor is twice that of the existing linear potentiometer sensor.


### 3.2. Sensitivity

The static sensitivity is defined as the ratio of the change of the output of the sensor to the change of the input that causes the change of the output [3]. For the existing linear potentiometer sensor, in the whole path of brush movement, the output voltage variation range ΔU1 is as follows:(5)ΔU1=LLUi−0LUi=Ui.Its voltage sensitivitySv1 is as follows:(6)sv1=ΔU1Δxmax=UiL.For the linear bipotentiometer sensor, in the whole path of brush movement, the output voltage variation rangeΔU2 is as follows:(7)ΔU2=2LL−1Ui−0L−1Ui=2Ui.Its voltage sensitivitySv2 is as follows:(8)Sv2=ΔU2Δxmax=2UiL.The above analysis shows that the voltage sensitivity of a linear bipotentiometer sensor is twice that of the existing linear potentiometer sensor. That is,(9)Sv2=2Sv1.


### 3.3. Step Characteristic, Voltage Resolution, and Step Error

According to the structure of the potentiometer sensor, the output voltage will jump one step when the brush moves one turn of the coil; the relationship between the output voltage curve of the sensor and the movement of the brush is shown in Figure7.Figure 7
Actual step characteristic curve of linear potentiometer sensor.(1) The brush being in contact with a wire. (2) The brush being in contact with two wires. (3) Potentiometer wire. (4) Actual step characteristic curve. (5) Ideal characteristic curve.When the brush moves one turn of the coil, the change of resistance isΔR, that is,(10)ΔR=Rmaxn,and the output voltage variation caused by it is called apparent resolution pulse ΔUn, that is,(11)ΔUn=UiRmax×ΔR=1nUi.When the brush moves between the two adjacent turns (thej and j+1 turns), the two adjacent turns will be short-circuited, which makes the total turns of linear potentiometer sensor become n−1 turns. At this time, the output voltage will have a small jump ΔUb, that is,(12)ΔUb=ui1n−1−1n.Therefore, the apparent resolution pulse is composed of two steps of different sizes. The large step is regarded as the main resolution pulseΔUa, and the small step is regarded as the secondary resolution pulse ΔUb. It can be concluded that(13)ΔUn=ΔUa+ΔUb.For the existing linear potentiometer sensor, its apparent resolution pulseΔUn1 is as follows:(14)ΔUn1=ΔUa1+ΔUb1=Uin.In Figure7, the actual step characteristic is shown with real broken line; however, the ideal sensor output is shown by the red dotted line. The step characteristic curve fluctuates up and down around the ideal characteristic line, which results in a certain deviation and is called step error [8]. The step error of the linear potentiometer sensor is usually expressed as the percentage of the ratio between the maximum deviation of the actual step characteristic curve to the ideal characteristic line and the output voltage variation range. That is,(15)γn1=±1/2ΔUn1ΔU1×100%=±1/2UiΔUi×100%=±12n×100%.Voltage resolution is defined as the percentage of the ratio between the maximum value voltage step of the potentiometer and the maximum output voltage range within the whole path of the brush movement. For the existing linear potentiometer sensor, the voltage resolution is as follows:(16)en1=ΔUn1ΔU1×100%=Ui/nUi×100=1n×100%.For the linear bipotentiometer sensor, its step characteristic curve is similar to the existing linear potentiometer sensor, and its apparent resolution pulse, step error, and voltage resolution are as follows:(17)ΔUn2=R1+ΔRRmax−R3−ΔRRmaxUi−R1Rmax−R3RmaxUi=2nUi,γn2=±1/2ΔUn2ΔU2×100%=±1/22Ui/n2Ui×100%=12n×100%,en2=Un2ΔU2×100%=2Ui/n2Ui×100=1n×100%.The above analysis shows that the apparent resolution pulse of the linear bipotentiometer sensor is twice that of the existing linear potentiometer sensor, and the step error and voltage resolution of the linear bipotentiometer sensor are equal to that of the existing linear potentiometer sensor. That is,(18)ΔUn2=2ΔUn1,γn2=γn1,en2=en1.In practical application, the ratio of brush diameter to wire diameter is 10, so the influence of step error can be ignored.


### 3.4. Load Characteristic and Load Error

If the output of potentiometer sensor is connected with load resistance, its output characteristic is called load characteristic.For the existing linear potentiometer sensor, the circuit connected with load resistanceRL is shown in Figure 3: its load output voltage UL1 is as follows:(19)UL1=RxRLRLRmax+RxRmax−Rx2Ui.The input voltage and measurement range of many sensors from different manufacturers or models are different. For analysis and comparison, they are processed by removing dimensions.Supposed relative variation of resistance isr, that is,(20)r=RxRmax,where r is defined as the relative change factor of displacement.Let(21)m=RmaxRL,where m is defined as the load factor.Taking equations (1), (20), and (21) into equation (22), the load characteristic Y1 of the existing linear potentiometer sensor is obtained, that is,(22)Y1=UL1Ui=r1+rm−mr2.It can be seen from equation (22) that when the potentiometer is connected with a load resistor, the load characteristic of the existing linear potentiometer sensor is nonlinear, and the larger the load coefficient m is, the more serious it is.The deviation between load characteristic and no-load characteristic is called load error. The load error of the existing linear potentiometer sensor is assumed to beδL1. Then,(23)δL1=Uo1−UL1.The load error can show how close the actual output of the sensor is to the ideal output, but it cannot show the measurement accuracy of different values, so the relative error is often used to show the accuracy of the measured value. Because the output voltage of the linear bipotentiometer sensor has positive, negative, and zero values, the relative load error is defined as the percentage of the ratio of the absolute load error to the output range of the sensor. For the existing linear potentiometer sensor, its relative load errorσL1 is as follows:(24)σL1=Uo1−UL1ΔU1×100%.For the linear bipotentiometer sensor, the circuit connected with load resistanceRL is shown in Figure 5; its load output voltage is as follows:(25)UL2=R1R4−R2R3RL∗Ui,where ∗=R1+R2R3+R4RL+R1R2R3+R4+R3R4R1+R2.The load characteristic expressionY2 of the linear bipotentiometer sensor can be obtained by taking equations (2), (20), and (21) into equation (24), i.e., (26)Y2=UL2Ui=2r−11+2r1−rm.According to the definition of load error, the load errorδL2 of the linear bipotentiometer sensor is as follows:(27)δl2=Uo2−UL2.According to the definition of the relative load error, the relative load errorσL2 of the linear bipotentiometer sensor is as follows:(28)σL2=Uo2−UL2ΔU2×100%.Based on the previous analysis of static characteristics, the four static characteristics are summarized as shown in Table1.Table 1
Some static characteristics of the two kinds of sensors.
SensitivityStep characteristicNo-load characteristicLoad characteristicThe existing linear potentiometer sensorsv1=Ui/Lγi1=±1/2n×100%Uo1=x/LUiY1=r/1+rm−mr2The linear bipotentiometer sensorsv2=2Ui/Lγi2=±1/2n×100%Uo2=2x/L−1UiY2=2r−1/1+2r1−rmRelationshipsv2=2sv1γi2=γi1


## 3.1. No-Load Characteristic

As shown in Figure3, when the load resistance RL⟶∞, i.e., no load, the output voltage uo1 of the brush sliding from the initial position to x is as follows:(3)Uo1=UiRxRmax=xLUi.Whenx changes from 0 to L, the range of the output voltage Uo1 is 0,Ui.In Figure5, when the load resistance RL⟶∞, i.e., no load, the output voltage uo2 of the brush sliding from the initial position to x is as follows:(4)Uo2=x/LRmax−1−x/LRmaxRmaxUi=UiR1Rmax−R3Rmax=2xL−1Ui.Whenx changes from 0 to L, the range of the output voltage Uo2 is −Ui,Ui.According to the above analysis, the no-load output voltage range of the linear bipotentiometer sensor is twice that of the existing linear potentiometer sensor.


## 3.2. Sensitivity

The static sensitivity is defined as the ratio of the change of the output of the sensor to the change of the input that causes the change of the output [3]. For the existing linear potentiometer sensor, in the whole path of brush movement, the output voltage variation range ΔU1 is as follows:(5)ΔU1=LLUi−0LUi=Ui.Its voltage sensitivitySv1 is as follows:(6)sv1=ΔU1Δxmax=UiL.For the linear bipotentiometer sensor, in the whole path of brush movement, the output voltage variation rangeΔU2 is as follows:(7)ΔU2=2LL−1Ui−0L−1Ui=2Ui.Its voltage sensitivitySv2 is as follows:(8)Sv2=ΔU2Δxmax=2UiL.The above analysis shows that the voltage sensitivity of a linear bipotentiometer sensor is twice that of the existing linear potentiometer sensor. That is,(9)Sv2=2Sv1.


## 3.3. Step Characteristic, Voltage Resolution, and Step Error

According to the structure of the potentiometer sensor, the output voltage will jump one step when the brush moves one turn of the coil; the relationship between the output voltage curve of the sensor and the movement of the brush is shown in Figure7.Figure 7
Actual step characteristic curve of linear potentiometer sensor.(1) The brush being in contact with a wire. (2) The brush being in contact with two wires. (3) Potentiometer wire. (4) Actual step characteristic curve. (5) Ideal characteristic curve.When the brush moves one turn of the coil, the change of resistance isΔR, that is,(10)ΔR=Rmaxn,and the output voltage variation caused by it is called apparent resolution pulse ΔUn, that is,(11)ΔUn=UiRmax×ΔR=1nUi.When the brush moves between the two adjacent turns (thej and j+1 turns), the two adjacent turns will be short-circuited, which makes the total turns of linear potentiometer sensor become n−1 turns. At this time, the output voltage will have a small jump ΔUb, that is,(12)ΔUb=ui1n−1−1n.Therefore, the apparent resolution pulse is composed of two steps of different sizes. The large step is regarded as the main resolution pulseΔUa, and the small step is regarded as the secondary resolution pulse ΔUb. It can be concluded that(13)ΔUn=ΔUa+ΔUb.For the existing linear potentiometer sensor, its apparent resolution pulseΔUn1 is as follows:(14)ΔUn1=ΔUa1+ΔUb1=Uin.In Figure7, the actual step characteristic is shown with real broken line; however, the ideal sensor output is shown by the red dotted line. The step characteristic curve fluctuates up and down around the ideal characteristic line, which results in a certain deviation and is called step error [8]. The step error of the linear potentiometer sensor is usually expressed as the percentage of the ratio between the maximum deviation of the actual step characteristic curve to the ideal characteristic line and the output voltage variation range. That is,(15)γn1=±1/2ΔUn1ΔU1×100%=±1/2UiΔUi×100%=±12n×100%.Voltage resolution is defined as the percentage of the ratio between the maximum value voltage step of the potentiometer and the maximum output voltage range within the whole path of the brush movement. For the existing linear potentiometer sensor, the voltage resolution is as follows:(16)en1=ΔUn1ΔU1×100%=Ui/nUi×100=1n×100%.For the linear bipotentiometer sensor, its step characteristic curve is similar to the existing linear potentiometer sensor, and its apparent resolution pulse, step error, and voltage resolution are as follows:(17)ΔUn2=R1+ΔRRmax−R3−ΔRRmaxUi−R1Rmax−R3RmaxUi=2nUi,γn2=±1/2ΔUn2ΔU2×100%=±1/22Ui/n2Ui×100%=12n×100%,en2=Un2ΔU2×100%=2Ui/n2Ui×100=1n×100%.The above analysis shows that the apparent resolution pulse of the linear bipotentiometer sensor is twice that of the existing linear potentiometer sensor, and the step error and voltage resolution of the linear bipotentiometer sensor are equal to that of the existing linear potentiometer sensor. That is,(18)ΔUn2=2ΔUn1,γn2=γn1,en2=en1.In practical application, the ratio of brush diameter to wire diameter is 10, so the influence of step error can be ignored.


## 3.4. Load Characteristic and Load Error

If the output of potentiometer sensor is connected with load resistance, its output characteristic is called load characteristic.For the existing linear potentiometer sensor, the circuit connected with load resistanceRL is shown in Figure 3: its load output voltage UL1 is as follows:(19)UL1=RxRLRLRmax+RxRmax−Rx2Ui.The input voltage and measurement range of many sensors from different manufacturers or models are different. For analysis and comparison, they are processed by removing dimensions.Supposed relative variation of resistance isr, that is,(20)r=RxRmax,where r is defined as the relative change factor of displacement.Let(21)m=RmaxRL,where m is defined as the load factor.Taking equations (1), (20), and (21) into equation (22), the load characteristic Y1 of the existing linear potentiometer sensor is obtained, that is,(22)Y1=UL1Ui=r1+rm−mr2.It can be seen from equation (22) that when the potentiometer is connected with a load resistor, the load characteristic of the existing linear potentiometer sensor is nonlinear, and the larger the load coefficient m is, the more serious it is.The deviation between load characteristic and no-load characteristic is called load error. The load error of the existing linear potentiometer sensor is assumed to beδL1. Then,(23)δL1=Uo1−UL1.The load error can show how close the actual output of the sensor is to the ideal output, but it cannot show the measurement accuracy of different values, so the relative error is often used to show the accuracy of the measured value. Because the output voltage of the linear bipotentiometer sensor has positive, negative, and zero values, the relative load error is defined as the percentage of the ratio of the absolute load error to the output range of the sensor. For the existing linear potentiometer sensor, its relative load errorσL1 is as follows:(24)σL1=Uo1−UL1ΔU1×100%.For the linear bipotentiometer sensor, the circuit connected with load resistanceRL is shown in Figure 5; its load output voltage is as follows:(25)UL2=R1R4−R2R3RL∗Ui,where ∗=R1+R2R3+R4RL+R1R2R3+R4+R3R4R1+R2.The load characteristic expressionY2 of the linear bipotentiometer sensor can be obtained by taking equations (2), (20), and (21) into equation (24), i.e., (26)Y2=UL2Ui=2r−11+2r1−rm.According to the definition of load error, the load errorδL2 of the linear bipotentiometer sensor is as follows:(27)δl2=Uo2−UL2.According to the definition of the relative load error, the relative load errorσL2 of the linear bipotentiometer sensor is as follows:(28)σL2=Uo2−UL2ΔU2×100%.Based on the previous analysis of static characteristics, the four static characteristics are summarized as shown in Table1.Table 1
Some static characteristics of the two kinds of sensors.
SensitivityStep characteristicNo-load characteristicLoad characteristicThe existing linear potentiometer sensorsv1=Ui/Lγi1=±1/2n×100%Uo1=x/LUiY1=r/1+rm−mr2The linear bipotentiometer sensorsv2=2Ui/Lγi2=±1/2n×100%Uo2=2x/L−1UiY2=2r−1/1+2r1−rmRelationshipsv2=2sv1γi2=γi1


## 4. Numerical Simulation

In this section, MATLAB software is used to simulate the curves of two kinds of sensors of linear potentiometer under no-load and load conditions. Suppose the total length of the potentiometerL=15cm, input voltage Ui=5V, coil turn n=750, pitch t=0.2mm, and Uo is the output voltage when the brush moves to x0<x<15cm.The no-load output voltage is simulated according to equations (3) and (4), and the simulation curve is shown in Figure 8. It can be seen from Figure 8 that the relationship between input and output of the two linear potentiometer sensors is linear and is without nonlinear error. Therefore, the no-load voltage output curve is the ideal output curve of the sensor. The output range of the linear bipotentiometer sensor is twice that of the existing linear potentiometer sensor. Therefore, the linear bipotentiometer sensor increases the signal output of measured parameters, which is the result of increased sensitivity with identical measurement range.Figure 8
No-load output voltage curve of the two kinds of linear potentiometer sensors.Whenm=0, 0.5, 2, and 5, the load output voltage curve of the existing linear potentiometer sensor is simulated according to equation (19); the simulation curve family is shown in Figure 9. It can be seen from Figure 9 that the load output voltage curve of the existing linear potentiometer sensor is a droop curve, which indicates that the load output voltage is lower than the no-load output voltage, and the less the m value is, the closer the load output voltage curve is to the no-load curve m=0.Figure 9
Load output voltage curve of the existing linear potentiometer sensor.Whenm=0, 0.5, 2, and 5, the load output voltage curve of the linear bipotentiometer sensor is simulated according to equation (25), and the simulation curve is shown in Figure 10. It can be seen from Figure 10 that the load output voltage curve of the linear bipotentiometer sensor has no load error when the brush is in the middle position of the potentiometer. When the brush is located on both sides of the midpoint of the potentiometer, the load output voltage curve is distributed on both sides of the no-load output voltage curve.Figure 10
Load output voltage curve of the linear bipotentiometer sensor.Whenm=0, 0.5, 2, and 5, the load characteristic curve of the existing linear potentiometer sensor is simulated according to equation (22), and the simulation curve family is shown in Figure 11. It can be seen from Figure 11 that the load characteristic curve of the existing linear potentiometer sensor is a droop curve, which indicates that the load output voltage is lower than the no-load output voltage, and the less the m value is, the closer the load characteristic curve is to the no-load curve m=0.Figure 11
Load characteristic curve of the existing linear potentiometer sensor.Whenm=0, 0.5, 2, and 5, the load characteristic curve of the linear bipotentiometer sensor is simulated according to equation (26), and the simulation curve is shown in Figure 12. It can be seen from Figure 12 that the load characteristic curve of the linear bipotentiometer sensor has no load error when the brush is in the middle position of the potentiometer. The load characteristic curve is distributed on both sides of the no-load characteristic curve when the brush is at both ends of the potentiometer.Figure 12
Load characteristic curve of the linear bipotentiometer sensor.Whenm=0, 0.5, 2, and 5, the load error curve of the existing linear potentiometer sensor is simulated according to equation (23), and the simulation curve family is shown in Figure 13. It can be seen from Figure 13 that the load error curve of the existing linear potentiometer sensor gets the largest valve when the brush is in the middle position.Figure 13
Load error curve of the existing linear potentiometer sensor.Whenm=0, 0.5, 2, and 5, the load characteristic curve of the linear bipotentiometer sensor is simulated according to equation (27), and the simulation curve is shown in Figure 14. It can be seen from Figure 14 that the load error curve of the linear bipotentiometer sensor is smaller or even zero when the brush is in the middle section of the potentiometer.Figure 14
Load error curve of the linear bipotentiometer sensor.Whenm=0, 0.5, 2, and 5, the relative load error curve of the existing linear potentiometer sensor is simulated according to equation (24), and the simulation curve family is shown in Figure 15. It can be seen from Figure 15 that the relative load error curve of the existing linear potentiometer sensor gets the largest valve when the brush is about two-thirds of the way position. When the larger the m value is, the larger the relative error of the brush in the same position is.Figure 15
Relative load error curve of the existing linear potentiometer sensor.Finally, whenm=0, 0.5, 2, and 5, the relative load error curve of the linear bipotentiometer sensor is simulated according to equation (28), and the simulation curve is shown in Figure 16. It can be seen from Figure 16 that the relative load error curve of the linear bipotentiometer sensor has positive and negative, and the relative load error is equal to zero when the brush is in the middle position, which is convenient to linearize the output signal of the sensor.Figure 16
Relative load error curve of the linear bipotentiometer sensor.The no-load output voltage, load output voltage, load characteristic, and relative load error curve of two kinds of sensors are simulated and analyzed. Compared with the two types of sensors, under the same conditions (the same asm and r), the linearity of the linear bipotentiometer sensor is much better than that of the existing linear potentiometer sensor, and the relative load error curve of the linear bipotentiometer sensor is only half that of the existing linear potentiometer sensor. From the different values of m, the sensor is working in the case of less m value, that is, the load resistance of the sensor is much larger than that of the sensitive element. Compared with the existing linear potentiometer sensor, the measurement value of the middle part of the linear bipotentiometer sensor is more accurate. Hence, a theoretical basis is provided for the use of the linear bipotentiometer sensor.


## 5. Conclusions

In this paper, the linear bipotentiometer sensor is proposed by changing the structure of the existing linear potentiometer sensor; at the same time, its working principle and some static characteristics are studied in detail. Compared with the existing linear potentiometer sensor, the sensitivity of the linear bipotentiometer sensor is doubled, the no-load output voltage range is doubled, the relative load error is half, the step error is unchanged, and its linearity is improved, which has a certain application value.



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*Source: 9958652-2021-06-09.xml*