# Design of a Compact and High Sensitivity Temperature Sensor Using Metamaterial

Authors: Sabah Zemouli; Abdelhafid Chaabi; Houcine Sofiane Talbi
Journal: International Journal of Antennas and Propagation
 (2015)

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## Abstract

The present paper aims at sensing the temperature. A sensor metamaterial consisting of two concentric metallic rings and a thin metallic wire deposited on the surface of BaTiO3 substrate is reported. The use of BaTiO3 makes the resonant frequency of the structure shift as the temperature varies and makes the sensor applicable in many fields of applications. Numerical simulations and theoretical results are presented and compared to each other; there was a good agreement between them. This sensor is smaller, easier to fabricate, and very sensitive to the changes in temperatures.


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## Body

## 1. Introduction

In this decade, metamaterials (MTM) or left handed materials (LHM) have attracted much attention among researchers in the microwave communities because of their unusual properties, such as negative permittivity [1], negative permeability [2], and negative refractive index [3, 4]. These periodic materials are very useful for many fields of applications [5–7]. Recently, a great interest has been devoted to the application of metamaterials in sensing; hereafter, we have provided some researches in this concern. Ishimaru and his colleagues have studied a metamaterial based on surface plasmon resonance (SPR) sensors in GHz regime while the traditional SPR is usually operated in optical domain only [8]. Kabashin et al. in [9] have enhanced the SPR sensor’s performances by using metamaterial. In [10], the authors have proposed a method of dielectric sensing using ε near zero narrow waveguide channels. In [11], Ekmekci and his colleague have studied a double sided square SRR (split ring resonator) topology for multipurpose sensor operating in X band; this sensor exhibits a negative value of permeability for frequencies close to the magnetic resonance frequency of the SRR structure, whereas our suggested structure exhibits negative permittivity and negative permeability close to the magnetic resonance frequency of the structure; in addition and according to [12] circular SRR can present a higher quality factor compared to square SRR. References [13, 14] have studied the application of a Terahertz metamaterial for chemical sensing and [15] have explained how metamaterials can offer solutions to overcome technical limitations of wireless sensors.Metamaterials are better in sensing than the conventional resonators (e.g., spiral coils), because they are easy and rapid in detection [16–18] and they can exhibit a strong localization and enhancement of fields; that is, they can improve the sensor’s selectivity and sensibility [19] due to the application of an axial time varying magnetic field parallel to the particle plane in the orthogonal direction to the splits which creates a huge electric field density localized between them and presents higher signal and higher dips in their transmission spectrum, which results in a high quality factor Q compared to the conventional RF (radio frequency) resonators. This enables us to make telemetric measurements and to observe the operating frequency relatively easier [20]. Another advantage of the gaps existence in the MTM structure is the production of an additional capacitive effect which exhibits a lower resonance frequency (hence avoid the background absorption of the structure) and results in higher shift of the operating frequency with the same applied load, leading to higher sensitivity. The use of Barium titanate dielectric that is very sensitive to the changes of temperature makes our sensor more sensitive.The aim of this paper is to design a high sensitive and smaller electrical sensor of temperature based on metamaterial operating in GHz regime. The proposed structure consists of a combination of two concentric circular metallic rings opened in the opposite sides commonly called SRR and a thin metallic wire placed on a dielectric substrate. Because the resonant frequency of the MTM structure is very sensitive to the changes of the capacitive effects (since its fundamental resonance behavior can be modeled by anLC circuit [21]) which are basically dependent on the resonator’s topology and the substrate’s parameters (i.e., substrate’s thickness and relative permittivity), we have proposed a structure with a varying dielectric characteristics substrate. When the temperature changes, the dielectric properties of the substrate of the MTM will change and this will affect the capacitance of the SRR and then a shift in the resonant frequency will appear; this will indicate the measured temperature.In this work, we have designed the equivalent circuit model of the proposed structure and we have derived the relations of its coefficients of reflexion and transmission using the ABCD Matrix approach; then we have compared them to those resulting from the simulation. The results were very close. In this study the metamaterial sensor is smaller, is easier to fabricate, possesses higher sensitivity, and is useful in a wide range of applications. The mechanism behind this is the use of a varying dielectric characteristics substrate.


## 2. Design OF LHM

The MTM structure is composed of a combination of PEC (perfect electric conductor) circular SRR and thin wire placed on a dielectric substrate of 0.1 mm of thickness(td); the length and width of this substrate are 2 mm and 2.5 mm, respectively. The external radius of the SRR is r0=0.75 mm, the width of the two rings is d=0.18 mm, the spacing between them is 0.24 mm, the split of the outer ring is 0.4 mm, the split of the inner ring is equal to 0.2 mm, and the thickness of the rings is tm=0.035 mm; the wire has a 0.2 mm of width and 1.8 mm of length. The substrate of this model is the Barium titanate dielectric BaTiO3 [22, 23] which is one of the best known and commonly used materials for electric ceramics due to its excellent dielectric, ferroelectric, and piezoelectric properties at and above room temperature. We have specially chosen this material because its relative permittivity has a big dependence with the temperature (see Figure 1) which can be tailored in a wide range of applications. Furthermore, this material is sintered at high temperatures. This allows an operation at very elevated temperatures. Figure 2 shows the proposed structure.Figure 1
Variation of the dielectric constant of BaTiO3 versus the temperature [22].Figure 2
SRRr0=0.75 mm, width d=0.18 mm, spacing between the two rings c=0.24 mm, thickness of the SRR tm=0.035 mm, and the split of the outer ring sout=0.4 mm and of the inner ring sin=0.2 mm; the wire has 0.2 mm of width and 1.8 mm of length.
(a)
(b)


## 3. Simulation and Equivalent Circuit Model

The simulation of the MTM structure has been executed using the High Frequency Structure Simulator (HFSS) software. A perfect magnetic conductor (PMC) boundary condition was set alongz-axis while the perfect electric conductor (PEC) boundary condition was set along y-axis. On the last two faces, we have set two ports rectangular waveguide for sensor measurements. The LHM structure was placed at the center of the waveguide.In Figure3, we have studied the variation of the coefficient of the transmission S21 versus the variation of the frequency using the commercial simulator HFSS to study the shift in the resonant frequency according to the variation of the temperature of the sensor.Figure 3
Variation of the coefficient of transmission S21 versus frequency at 40°C.The effective permittivity of the LHM structure is different from the relative permittivity of the BaTiO3 substrate(εBaTiO3≠εMTMstructure). We have calculated the effective permittivity εeff and the effective permeability μeff of the MTM structure using the Nicolson-Ross-Weir method [24]; the results are shown in Figure 4.Figure 4
The variation of the real (red) and imaginary part (blue) of the permittivity (ε) and the variation of the real (red) and imaginary part (blue) of the permeability (μ) according to the frequency.
(a)
(b)We notice that the resonant frequency of the simulated structure is 2.3 GHz with return loss of −20 dB. The relative permittivity at this frequency is −12.19, whereas the relative permeability is −12.65.


### 3.1. Study of the Effects of the Dielectric Substrate on the MTM Structure

The resonant frequency of the MTM structure is inversely related to the total capacitanceCT of the sensor f=1/2πLTCT [21]; it is known that the capacitance is proportional to the dielectric constant C=ε(l/S), where S is area of a dielectric material, l is the thickness of a dielectric material, and ε is dielectric material’s permittivity.Whenε increases, the capacitance of the sensor CT increases which will decrease the resonant frequency. The shift in the resonant frequency resulting from the variation of the permittivity will indicate the variation in the temperature since the dielectric characteristics of the BaTiO3 substrate are related to the temperature (see Figure 1).When a time harmonic external magnetic field is applied alongz axis of this structure, an electromotive force will create an induced current in the structure that will explain the inductive part of our system.Because the LHM structure has a size much smaller than the operating wavelength, we can describe its electromagnetic characteristics by lumped circuit components capacitors and inductors. The overall structure can be represented by anLC circuit and the equivalent circuit model proposed for our LHM structure is shown in Figure 6, where L models the total inductance of the two rings of the SRR, C is the capacitance of the split in the inner and outer ring and the capacitance of the gap between them, Cs models the coupling between the SRR and the line, and Ls models the inductance of the wire. After calculation, we noticed L⋙M, so the mutual inductance can be neglected and the inductive currents will be neglected.Figure5 shows the distribution of the current around the wire and the SRR and demonstrates the previous conclusion.Figure 5
The distribution of the current around the wire and the SRR.Figure 6
Equivalent circuit model for the LHM structure.In Figure7, we have plotted the calculated S21 parameter versus the frequency using ABCD Matrix approach, which is based on the following equations:(1)A=V1V2I2=0,B=V1I2V2=0,C=I1V2I2=0,D=I1I2V2=0,Z11=AC,Z12=AD-BCC,Z21=1C,Z22=DC,S11=Z11-Z0Z22+Z0-Z12Z21ΔZ,S21=Z11+Z0Z22-Z0-Z12Z21ΔZ,ΔZ=Z11+Z0Z22+Z0-Z12Z21.The ABCD Matrix for this kind of a cascade connection of two port networks is 1ZT01 with ZT=jωLs+1/jωCs+(1-LCω2)/jCω; the parameters L, C, Ls, and Cs can be approximated by the following relationships [25, 26]:(2)L=8μDln⁡Dd+0.9+0.2ω2D2+0.5c2ρD2ln⁡Dd+0.9+0.2ω2D2+0.5c2ρD2+0.4sc+dD2-0.5ln⁡d+tmd+2μDln⁡1ρ-0.6+0.7ρ2+0.2+112ρ2d2D2,C=0.06+3.5×10-5×rout+rin+εε0dtms,Ls=μlπ2ln⁡⁡2.067lω+0.36ωl+0.25ω2l2,Cs=εε0dtmc,ρ=d+cD,D=0.5D1+D2.Figure 7
The variation of S21 versus frequency calculated using the ABCD Matrix approach from the equivalent circuit model.The resonant frequency calculated is 2.4 GHz with return loss of −52 dB. We note that the calculated and the simulated results are very close.Each time the temperature varies, it leads to a variation in the dielectric characteristics of the substrate BaTiO3 of the LHM structure which affects its capacitance which depends inversely on the frequency of resonance of the structure.To obtain the effects of the temperature on theS parameters and hence on the resonant frequency of the MTM structure, we have studied the variation of the dielectric characteristics of the BaTiO3 that are corresponding to well-known temperatures according to the variation of the resonant frequency of the MTM structure. In the interval of temperature from 20° to 150°, we have plotted the variation of the resonance frequency in function of temperature (see Figure 8).Figure 8
Variation of frequency versus the temperature.The minimum and maximum temperatures that can be detected by this sensor depend on the minimum and maximum temperatures that can be supported by the BaTiO3 substrate.The BaTiO3 material is sintered at high temperatures, which allows an operation at wide range temperatures [27]. So, TMax has a high value and because this material has no linear variation of the temperature in function of ε, the variation of the resonance frequency will not have a linear variation in function of the temperature (when ε increases the resonant frequency of the MTM structure decreases; this is because the frequency is inversely proportional to the capacitive effect which is proportional to epsilon), but we can note that the curve is linear just in the intervals [20–40], [40–60], [60–120], and [120–140].We have done this study in GHz regime, but the variations of the frequency are in the order of MHz; that is why in Table1 we have presented the sensibility of this sensor in MHz.Table 1
The interval of temperature
Δ
f [MHz]
The sensibility [MHZ]
[20°–40°]
80
4
[40°–60°]
30
1.5
[60°–80°]
90
4.5
[80°–100°]
100
5
[100°–120°]
140
7
[120°–140°]
70
3.5


## 3.1. Study of the Effects of the Dielectric Substrate on the MTM Structure

The resonant frequency of the MTM structure is inversely related to the total capacitanceCT of the sensor f=1/2πLTCT [21]; it is known that the capacitance is proportional to the dielectric constant C=ε(l/S), where S is area of a dielectric material, l is the thickness of a dielectric material, and ε is dielectric material’s permittivity.Whenε increases, the capacitance of the sensor CT increases which will decrease the resonant frequency. The shift in the resonant frequency resulting from the variation of the permittivity will indicate the variation in the temperature since the dielectric characteristics of the BaTiO3 substrate are related to the temperature (see Figure 1).When a time harmonic external magnetic field is applied alongz axis of this structure, an electromotive force will create an induced current in the structure that will explain the inductive part of our system.Because the LHM structure has a size much smaller than the operating wavelength, we can describe its electromagnetic characteristics by lumped circuit components capacitors and inductors. The overall structure can be represented by anLC circuit and the equivalent circuit model proposed for our LHM structure is shown in Figure 6, where L models the total inductance of the two rings of the SRR, C is the capacitance of the split in the inner and outer ring and the capacitance of the gap between them, Cs models the coupling between the SRR and the line, and Ls models the inductance of the wire. After calculation, we noticed L⋙M, so the mutual inductance can be neglected and the inductive currents will be neglected.Figure5 shows the distribution of the current around the wire and the SRR and demonstrates the previous conclusion.Figure 5
The distribution of the current around the wire and the SRR.Figure 6
Equivalent circuit model for the LHM structure.In Figure7, we have plotted the calculated S21 parameter versus the frequency using ABCD Matrix approach, which is based on the following equations:(1)A=V1V2I2=0,B=V1I2V2=0,C=I1V2I2=0,D=I1I2V2=0,Z11=AC,Z12=AD-BCC,Z21=1C,Z22=DC,S11=Z11-Z0Z22+Z0-Z12Z21ΔZ,S21=Z11+Z0Z22-Z0-Z12Z21ΔZ,ΔZ=Z11+Z0Z22+Z0-Z12Z21.The ABCD Matrix for this kind of a cascade connection of two port networks is 1ZT01 with ZT=jωLs+1/jωCs+(1-LCω2)/jCω; the parameters L, C, Ls, and Cs can be approximated by the following relationships [25, 26]:(2)L=8μDln⁡Dd+0.9+0.2ω2D2+0.5c2ρD2ln⁡Dd+0.9+0.2ω2D2+0.5c2ρD2+0.4sc+dD2-0.5ln⁡d+tmd+2μDln⁡1ρ-0.6+0.7ρ2+0.2+112ρ2d2D2,C=0.06+3.5×10-5×rout+rin+εε0dtms,Ls=μlπ2ln⁡⁡2.067lω+0.36ωl+0.25ω2l2,Cs=εε0dtmc,ρ=d+cD,D=0.5D1+D2.Figure 7
The variation of S21 versus frequency calculated using the ABCD Matrix approach from the equivalent circuit model.The resonant frequency calculated is 2.4 GHz with return loss of −52 dB. We note that the calculated and the simulated results are very close.Each time the temperature varies, it leads to a variation in the dielectric characteristics of the substrate BaTiO3 of the LHM structure which affects its capacitance which depends inversely on the frequency of resonance of the structure.To obtain the effects of the temperature on theS parameters and hence on the resonant frequency of the MTM structure, we have studied the variation of the dielectric characteristics of the BaTiO3 that are corresponding to well-known temperatures according to the variation of the resonant frequency of the MTM structure. In the interval of temperature from 20° to 150°, we have plotted the variation of the resonance frequency in function of temperature (see Figure 8).Figure 8
Variation of frequency versus the temperature.The minimum and maximum temperatures that can be detected by this sensor depend on the minimum and maximum temperatures that can be supported by the BaTiO3 substrate.The BaTiO3 material is sintered at high temperatures, which allows an operation at wide range temperatures [27]. So, TMax has a high value and because this material has no linear variation of the temperature in function of ε, the variation of the resonance frequency will not have a linear variation in function of the temperature (when ε increases the resonant frequency of the MTM structure decreases; this is because the frequency is inversely proportional to the capacitive effect which is proportional to epsilon), but we can note that the curve is linear just in the intervals [20–40], [40–60], [60–120], and [120–140].We have done this study in GHz regime, but the variations of the frequency are in the order of MHz; that is why in Table1 we have presented the sensibility of this sensor in MHz.Table 1
The interval of temperature
Δ
f [MHz]
The sensibility [MHZ]
[20°–40°]
80
4
[40°–60°]
30
1.5
[60°–80°]
90
4.5
[80°–100°]
100
5
[100°–120°]
140
7
[120°–140°]
70
3.5


## 4. Conclusion

This paper presents a sensor of temperature using the metamaterial. We have studied the variations of the resonant frequency according to the permittivity of structure which depend on the temperature.We have proposed an equivalent circuit model of our LHM structure and using the software MATLAB we have calculated the coefficients of reflection and transmission; the obtained curves are in accordance with those obtained by the HFSS.Using the two methods HFSS and Matrix ABCD, we can notice that the variation in the temperature involves a variation of the frequency of resonance and it is illustrated in a curve.Because the BaTiO3 has big dependence of the relative permittivity with the temperature, this sensor can be tailored in a wide range of applications.Based on the promising results of this sensor, we believe that the use of the proposed sensor’s topology will efficiently be used in various sensing applications including pressure and humidity and also in biological and chemical sensing for any region of wavelengths.



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*Source: 301358-2015-05-18.xml*