# An Effective Method for Electromagnetic Parameter Measurement of Flexible Materials Based on Air Coaxial Line

Authors: Jinjing Ren; Mingjie Sheng; Zhongyuan Zhou
Journal: International Journal of Antennas and Propagation
 (2022)

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## Abstract

When measuring the electromagnetic parameters of flexible material with an air coaxial line, the specimen is prone to bend and deform in the fixture, which results in erroneous results. In order to solve this problem, this paper proposes a new measurement method. Firstly, a rigid material is selected and loaded into the air coaxial line for two-portS parameters measurement. Then, the flexible material is attached to one end of the rigid material and loaded into the air coaxial line together for repeated two-port S parameter measurement. According to the S parameters measured and the two-port network cascading theory, the S parameters of the flexible material separately loaded in the fixture can be deduced. Finally, the electromagnetic parameters of the flexible material can be calculated by the Nicolson−Ross−Weir (NRW) method. Experimental results show that the method proposed is effective and reliable.


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## Body

## 1. Introduction

The electromagnetic parameters of materials mainly include complex permittivity and complex permeability [1, 2]. The commonly used measurement methods include lumped parameter, network parameter, and resonant cavity method [3–5]. The network parameter method based on air coaxial line is widely used because of its wide band and simple operation [6]. The measurement setup with an air coaxial line is shown in Figure 1. The specimen must be made into a concentric circle with the same section size as the device (specimen 1 in Figure 1) and loaded into the air coaxial line for two-port S parameters measurement. Conversion methods can obtain the electromagnetic parameters of the material according to the S parameters measured. There are many kinds of conversion methods based on the air coaxial line. The standard ASTM D7449 [7] summarizes and compares their characteristics. The NRW method only needs the reflection and transmission coefficients and can calculate both the complex permittivity and complex permeability, which the standard recommends [7–9]. The measurement process is easy to implement for materials with good rigidity [10]. However, for thin flexible materials, bending and deformations are prone to occur during clamping, as specimens 2 and 3 in Figure 1, which will result in inaccurate measurement results.Figure 1
Setup for electromagnetic parameter measurement with an air coaxial line.To avoid this problem, a waveguide can be adopted as the measurement device, but the working frequency of it is narrow [11–13]. Another approach is sticking multiple pieces of specimens together to increase the material’s rigidity by increasing the thickness. However, many adhesives will be introduced, which will lead to a deviation between the test results and the real electromagnetic parameters of the material. Reference [14] proposes a method to determine the dielectric model parameters of thin-film material with an air coaxial line. The method is based on input impedance measurement and calculates the electromagnetic parameters in the low frequency band. For higher frequencies, the method does not work because of the resonance.This paper proposes a measurement method for attaching flexible material to rigid material. Firstly, we select a rigid material with a smooth end face as the substrate and load it into the air coaxial line to measure the two-portS parameters. Then, we attach the flexible material to one end of the substrate and load these two materials into the air coaxial line together to measure the two-port S parameters again. The results can be regarded as a cascade of two two-port networks. According to the S parameters measured above and the transition matrix of cascaded networks, the S parameters of the flexible material separately and flatly loaded in the air coaxial line can be calculated. Finally, the complex permittivity and permeability can be obtained with the NRW method. In the process mentioned above, the substrate material should be put at the same position in the air coaxial line, which is very important.


## 2. Methods and Principle

### 2.1. Measurement Method and Procedure

The cross section of the air coaxial line with a rigid material specimen is shown in Figure2. The standard [7] gives the calculation equations of complex permittivity and complex permeability based on the NRW method as follows:(1)μr=2πΛγ02−γc21+Γ1−Γ,(2)εr=2πμrγ024π2Λ2=γc2,where Γ=X±X2−1, X=S112−S212+1/2S11, T=S11+S21−Γ/1−S11+S21Γ, 1/Λ2=−1/2πL∊T2, γ0=j2πfε0μ0 is the propagation constant of the air section, and γc=γ0εrμr is the propagation constant of the specimen section. The references of S11 and S21 are planes 2 and 3, respectively. It can be seen from equations (1) and (2) that in order to calculate the complex permittivity and complex permeability, getting values of the reflection coefficient and transmission coefficient at both ends of the specimen is the prerequisite.Figure 2
The cross section of the air coaxial line containing a specimen.In the NRW method, it is necessary to know the position of the specimen in the air coaxial line accurately when measuring the electromagnetic parameters of materials [9]. For the convenience of measurement, the end face of the specimen is generally flush with one port of the fixture, i.e., l1 or l2 is equal to 0 in Figure 2. It is difficult to ensure that the substrate is always at the same position in the air coaxial line during multiple measurements. In order to make the measurement more operable, the measurement process proposed in this paper is shown in Figure 3, where Z0, Z1, Z2, and Z3 are the characteristic impedances of the air, specimen 1, specimen 2, and specimen 3 sections in the air coaxial line, respectively, and the specimens 1 and 2 are the same material in this paper, i.e., Z1 = Z2. The measurement process is as follows: first, we load the rigid material specimens 1 and 2 into the air coaxial line from port 1 in sequence as shown in Figure 3(a) and measure the S parameters between planes 1 and 4 with the vector network analyzer (VNA). Because the specimen and the inner conductor of the air coaxial line are tightly matched and the end faces of specimens 1 and 2 are smooth, it can be considered that there is no air gap between specimens. In this case, the S parameters measured can be regarded as the results of the two-port network cascade of specimens 1 and 2. Then, we put specimen 2 into the air coaxial line separately as shown in Figure 3(b) and measure the S parameters. Finally, we load specimen 1 and the material to be tested (specimen 3) into the air coaxial line in sequence and measure the S parameters between planes 1 and 4 again. The results can be regarded as the two-port network cascading of specimens 1 and 3. According to the process mentioned above, S parameters of specimen 3 separately loaded into the air coaxial line (as shown in Figure 3(d)) can be deduced. It is noted that the thickness of specimens 2 and 3 should be the same.Figure 3
Measurement process of electromagnetic parameters of flexible materials. (a) Step 1: measurement and equivalent network of specimens 1 and 2. (b) Step 2: measurement and equivalent network of specimen 2. (c) Step 3: measurement and equivalent network of specimens 1 and 3. (d) Equivalent measurement of specimens 3 derived from step 1, step 2, and step 3.
(a)(b)(c)(d)


### 2.2. Calculation and Principle

To express clearly,Tn,ki,j and Sxyi,j are used to represent the transmission matrix and the S parameters in calculations, respectively, and Sxym is used to represent the S parameters obtained from VNA, where n and k represent the measurement specimen, respectively, and i and j represent the reference plane. The scattering matrix of the equivalent two-port network can be obtained from measurements in Figures 3(a)–3(c) directly. For the cascaded two-port network, the transfer matrix is adopted for analysis [15].We suppose that the transfer matrix is expressed as equation (3) when the characteristic impedance on both sides of the specimen I is Z0.(3)Ti=aiZ0bi1Z0cidi.The corresponding normalized transfer matrix is expressed as [15](4)T˜i=aibicidi,where i = 1, 2, or 3 and a, b, c, and d are the four elements of the normalized transition matrix T˜ [16].


#### 2.2.1. For Measurement in Figure3(a)

The transfer matrices of specimens 1 and 2 are expressed as equations (5) and (6), respectively.(5)T12,3=Z2Z0a1Z0Z2b11Z0Z2c1Z0Z2d1,(6)T21,2=Z0Z1a2Z0Z1b21Z0Z1c2Z1Z0d2.According to the two-port network cascade theory, the transition matrix of the cascaded networks is equal to the product of single network transition matrix. So, for the measurements in Figure3(a), we can get(7)T2,11,3=T21,2T12,3=a1a2+b2c1Z0b1a2+b2d11Z0a1c2+c1d2b1c2+d1d2,where T2,11,3 can be deduced from the S parameters measured as [15](8)T2,11,3=12S211,3A1B1C1D1,where(9)A1=1+S1111−S223+S121,3S211,3,B1=Z01+S1111+S223−S121,3S211,3,C1=1Z01−S1111−S222−S121,3S211,3,D1=1−S1111+S223+S121,3S211,3.The reference planes ofS parameters directly measured by VNA are planes 1 and 4, so it is necessary to convert the reference planes as (10)S111=S11m,S112=S11me2γ0d2,S211,3=S21meγ0l1,S211,2=S21meγ0l1+d1,S211,3=S12meγ0l1,S121,2=S12meγ0l1+d1,S222=S22me2γ0l1+d1,S223=S22me2γ0l1.Based on equations (7) to (10), the product of T˜2 and T˜1 can be calculated.


#### 2.2.2. For Measurement in Figure3(b)

(11)T21,2=a2Z0b2Z0c2d2=12S211,2A2B2C2D2,where(12)A2=1+S1111−S222+S121,2S211,2,B2=Z01+S1111+S222−S121,2S211,2,C2=1Z01−S1111−S222−S121,2S211,2,D2=1−S1111+S222+S121,2S211,2.T˜2 can be solved from equations (11) and (12) Combined with the results obtained from measurement in Figure 3(a), T˜1 can be calculated.


#### 2.2.3. For Measurement in Figure3(c)

(13)T3,11,3=T31,2T12,3=Za1a3+1Zb3c1Z0Za3b1+1Zb3d11Z0Za1c3+1Zc1d3Zb1c3+1Zd1d3=12S211,3A3B3C3D3,where(14)A3=1+S1111−S223+S121,3S211,3,B3=Z01+S1111+S223−S121,3S211,3,C3=1Z01−S1111−S223−S121,3S211,3,D3=1−S1111+S223+S121,3S211,3,Z=Z3Z1.For the convenience of calculation, we decompose equations (13) as(15)T3,11,3=Za3Z01Zb3ZZ0c31Zd3a1Z0b11Z0c1d1=Za3Z01Zb3ZZ0c31Zd3T1.In (15), T3,11,3 and T1 are already calculated, so we can get the following:(16)Za3Z0Zb31ZZ0c31Zd3=T3,11,3T1−1.The two-port network corresponding toT3 is symmetric, and equation (17) can be obtained according to its properties [16].(17)a3=d3.Now, there are four unknownsa3d3,b3,c3,andZ and four equations in equation (16), so T3 and T˜3 can be solved easily. According to the transformation relationship between the scattering parameters and the transfer matrix [16], S parameters of the two-port network in Figure 3(d) can be obtained. Finally, the electromagnetic parameters of specimen 3 can be calculated by the NRW method (Equations (1) and (2)).


### 2.3. Experiment and Analysis

In this part, flexible material is measured. A piece of polytetrafluoroethylene (PTFE) with the thickness of 0.5 mm shown in Figure4 is adopted as specimen 3 to carry out the verification experiment. The electromagnetic parameters are obtained with the method proposed in this paper, which are compared with the reference values. The reference values are obtained from the measurement with the air coaxial line according to the standard [7], where a 2 mm PTFE specimen is adopted. For specimens 1 and 2, rigid materials code K04 with the thickness of 2 mm and 0.5 mm are selected, respectively. The inner and outer diameters of specimens all meet the test requirements of the air coaxial line, which are shown in Figure 4.Figure 4
Photo of specimens.The measurement setup is shown in Figure5, where the VNA is R&S ZNB20 and is calibrated by the calibration kit R&S ZVZ270 (type N, 50 Ω). The settings are as follows: frequency 0.1 GHz to 18 GHz, output power −10 dBm, IF bandwidth 700 Hz, 1601 sampling points, and no averaging applied to data. The outer diameter of the air coaxial line is 7.0 mm, the diameter of the inner conductor is 3.04 mm, and the length is 80 mm.Figure 5
Measurement setup.The results are shown in Figure6. The measurement results in blue are based on the proposed method in this paper and the reference values in red are based on the method in standard ASTM D7449. It can be seen that the results of the method proposed in this paper consist well with the reference value from 1 GHz to 18 GHz. It proves the effectiveness of the method proposed. At low frequencies (0.1 GHz ∼ 1 GHz), the curves of the method proposed show larger fluctuations. This is because the measurement with VNA shows greater uncertainty when the thickness of the specimen is only 0.5 mm [17]. It should be noted that the thickness of the substrate (specimen 1) in this paper should be chosen carefully to avoid resonance [18].Figure 6
Comparison between measurement results and reference values (the measurement results in blue are based on the proposed method in this paper and the reference values in red are based on the method in standard ASTM D7449): (a) real part of relative permittivity, (b) imaginary part of relative permittivity, (c) real part of relative permeability, and (d) imaginary part of permeability.
(a)(b)(c)(d)


## 2.1. Measurement Method and Procedure

The cross section of the air coaxial line with a rigid material specimen is shown in Figure2. The standard [7] gives the calculation equations of complex permittivity and complex permeability based on the NRW method as follows:(1)μr=2πΛγ02−γc21+Γ1−Γ,(2)εr=2πμrγ024π2Λ2=γc2,where Γ=X±X2−1, X=S112−S212+1/2S11, T=S11+S21−Γ/1−S11+S21Γ, 1/Λ2=−1/2πL∊T2, γ0=j2πfε0μ0 is the propagation constant of the air section, and γc=γ0εrμr is the propagation constant of the specimen section. The references of S11 and S21 are planes 2 and 3, respectively. It can be seen from equations (1) and (2) that in order to calculate the complex permittivity and complex permeability, getting values of the reflection coefficient and transmission coefficient at both ends of the specimen is the prerequisite.Figure 2
The cross section of the air coaxial line containing a specimen.In the NRW method, it is necessary to know the position of the specimen in the air coaxial line accurately when measuring the electromagnetic parameters of materials [9]. For the convenience of measurement, the end face of the specimen is generally flush with one port of the fixture, i.e., l1 or l2 is equal to 0 in Figure 2. It is difficult to ensure that the substrate is always at the same position in the air coaxial line during multiple measurements. In order to make the measurement more operable, the measurement process proposed in this paper is shown in Figure 3, where Z0, Z1, Z2, and Z3 are the characteristic impedances of the air, specimen 1, specimen 2, and specimen 3 sections in the air coaxial line, respectively, and the specimens 1 and 2 are the same material in this paper, i.e., Z1 = Z2. The measurement process is as follows: first, we load the rigid material specimens 1 and 2 into the air coaxial line from port 1 in sequence as shown in Figure 3(a) and measure the S parameters between planes 1 and 4 with the vector network analyzer (VNA). Because the specimen and the inner conductor of the air coaxial line are tightly matched and the end faces of specimens 1 and 2 are smooth, it can be considered that there is no air gap between specimens. In this case, the S parameters measured can be regarded as the results of the two-port network cascade of specimens 1 and 2. Then, we put specimen 2 into the air coaxial line separately as shown in Figure 3(b) and measure the S parameters. Finally, we load specimen 1 and the material to be tested (specimen 3) into the air coaxial line in sequence and measure the S parameters between planes 1 and 4 again. The results can be regarded as the two-port network cascading of specimens 1 and 3. According to the process mentioned above, S parameters of specimen 3 separately loaded into the air coaxial line (as shown in Figure 3(d)) can be deduced. It is noted that the thickness of specimens 2 and 3 should be the same.Figure 3
Measurement process of electromagnetic parameters of flexible materials. (a) Step 1: measurement and equivalent network of specimens 1 and 2. (b) Step 2: measurement and equivalent network of specimen 2. (c) Step 3: measurement and equivalent network of specimens 1 and 3. (d) Equivalent measurement of specimens 3 derived from step 1, step 2, and step 3.
(a)(b)(c)(d)


## 2.2. Calculation and Principle

To express clearly,Tn,ki,j and Sxyi,j are used to represent the transmission matrix and the S parameters in calculations, respectively, and Sxym is used to represent the S parameters obtained from VNA, where n and k represent the measurement specimen, respectively, and i and j represent the reference plane. The scattering matrix of the equivalent two-port network can be obtained from measurements in Figures 3(a)–3(c) directly. For the cascaded two-port network, the transfer matrix is adopted for analysis [15].We suppose that the transfer matrix is expressed as equation (3) when the characteristic impedance on both sides of the specimen I is Z0.(3)Ti=aiZ0bi1Z0cidi.The corresponding normalized transfer matrix is expressed as [15](4)T˜i=aibicidi,where i = 1, 2, or 3 and a, b, c, and d are the four elements of the normalized transition matrix T˜ [16].


### 2.2.1. For Measurement in Figure3(a)

The transfer matrices of specimens 1 and 2 are expressed as equations (5) and (6), respectively.(5)T12,3=Z2Z0a1Z0Z2b11Z0Z2c1Z0Z2d1,(6)T21,2=Z0Z1a2Z0Z1b21Z0Z1c2Z1Z0d2.According to the two-port network cascade theory, the transition matrix of the cascaded networks is equal to the product of single network transition matrix. So, for the measurements in Figure3(a), we can get(7)T2,11,3=T21,2T12,3=a1a2+b2c1Z0b1a2+b2d11Z0a1c2+c1d2b1c2+d1d2,where T2,11,3 can be deduced from the S parameters measured as [15](8)T2,11,3=12S211,3A1B1C1D1,where(9)A1=1+S1111−S223+S121,3S211,3,B1=Z01+S1111+S223−S121,3S211,3,C1=1Z01−S1111−S222−S121,3S211,3,D1=1−S1111+S223+S121,3S211,3.The reference planes ofS parameters directly measured by VNA are planes 1 and 4, so it is necessary to convert the reference planes as (10)S111=S11m,S112=S11me2γ0d2,S211,3=S21meγ0l1,S211,2=S21meγ0l1+d1,S211,3=S12meγ0l1,S121,2=S12meγ0l1+d1,S222=S22me2γ0l1+d1,S223=S22me2γ0l1.Based on equations (7) to (10), the product of T˜2 and T˜1 can be calculated.


### 2.2.2. For Measurement in Figure3(b)

(11)T21,2=a2Z0b2Z0c2d2=12S211,2A2B2C2D2,where(12)A2=1+S1111−S222+S121,2S211,2,B2=Z01+S1111+S222−S121,2S211,2,C2=1Z01−S1111−S222−S121,2S211,2,D2=1−S1111+S222+S121,2S211,2.T˜2 can be solved from equations (11) and (12) Combined with the results obtained from measurement in Figure 3(a), T˜1 can be calculated.


### 2.2.3. For Measurement in Figure3(c)

(13)T3,11,3=T31,2T12,3=Za1a3+1Zb3c1Z0Za3b1+1Zb3d11Z0Za1c3+1Zc1d3Zb1c3+1Zd1d3=12S211,3A3B3C3D3,where(14)A3=1+S1111−S223+S121,3S211,3,B3=Z01+S1111+S223−S121,3S211,3,C3=1Z01−S1111−S223−S121,3S211,3,D3=1−S1111+S223+S121,3S211,3,Z=Z3Z1.For the convenience of calculation, we decompose equations (13) as(15)T3,11,3=Za3Z01Zb3ZZ0c31Zd3a1Z0b11Z0c1d1=Za3Z01Zb3ZZ0c31Zd3T1.In (15), T3,11,3 and T1 are already calculated, so we can get the following:(16)Za3Z0Zb31ZZ0c31Zd3=T3,11,3T1−1.The two-port network corresponding toT3 is symmetric, and equation (17) can be obtained according to its properties [16].(17)a3=d3.Now, there are four unknownsa3d3,b3,c3,andZ and four equations in equation (16), so T3 and T˜3 can be solved easily. According to the transformation relationship between the scattering parameters and the transfer matrix [16], S parameters of the two-port network in Figure 3(d) can be obtained. Finally, the electromagnetic parameters of specimen 3 can be calculated by the NRW method (Equations (1) and (2)).


## 2.2.1. For Measurement in Figure3(a)

The transfer matrices of specimens 1 and 2 are expressed as equations (5) and (6), respectively.(5)T12,3=Z2Z0a1Z0Z2b11Z0Z2c1Z0Z2d1,(6)T21,2=Z0Z1a2Z0Z1b21Z0Z1c2Z1Z0d2.According to the two-port network cascade theory, the transition matrix of the cascaded networks is equal to the product of single network transition matrix. So, for the measurements in Figure3(a), we can get(7)T2,11,3=T21,2T12,3=a1a2+b2c1Z0b1a2+b2d11Z0a1c2+c1d2b1c2+d1d2,where T2,11,3 can be deduced from the S parameters measured as [15](8)T2,11,3=12S211,3A1B1C1D1,where(9)A1=1+S1111−S223+S121,3S211,3,B1=Z01+S1111+S223−S121,3S211,3,C1=1Z01−S1111−S222−S121,3S211,3,D1=1−S1111+S223+S121,3S211,3.The reference planes ofS parameters directly measured by VNA are planes 1 and 4, so it is necessary to convert the reference planes as (10)S111=S11m,S112=S11me2γ0d2,S211,3=S21meγ0l1,S211,2=S21meγ0l1+d1,S211,3=S12meγ0l1,S121,2=S12meγ0l1+d1,S222=S22me2γ0l1+d1,S223=S22me2γ0l1.Based on equations (7) to (10), the product of T˜2 and T˜1 can be calculated.


## 2.2.2. For Measurement in Figure3(b)

(11)T21,2=a2Z0b2Z0c2d2=12S211,2A2B2C2D2,where(12)A2=1+S1111−S222+S121,2S211,2,B2=Z01+S1111+S222−S121,2S211,2,C2=1Z01−S1111−S222−S121,2S211,2,D2=1−S1111+S222+S121,2S211,2.T˜2 can be solved from equations (11) and (12) Combined with the results obtained from measurement in Figure 3(a), T˜1 can be calculated.


## 2.2.3. For Measurement in Figure3(c)

(13)T3,11,3=T31,2T12,3=Za1a3+1Zb3c1Z0Za3b1+1Zb3d11Z0Za1c3+1Zc1d3Zb1c3+1Zd1d3=12S211,3A3B3C3D3,where(14)A3=1+S1111−S223+S121,3S211,3,B3=Z01+S1111+S223−S121,3S211,3,C3=1Z01−S1111−S223−S121,3S211,3,D3=1−S1111+S223+S121,3S211,3,Z=Z3Z1.For the convenience of calculation, we decompose equations (13) as(15)T3,11,3=Za3Z01Zb3ZZ0c31Zd3a1Z0b11Z0c1d1=Za3Z01Zb3ZZ0c31Zd3T1.In (15), T3,11,3 and T1 are already calculated, so we can get the following:(16)Za3Z0Zb31ZZ0c31Zd3=T3,11,3T1−1.The two-port network corresponding toT3 is symmetric, and equation (17) can be obtained according to its properties [16].(17)a3=d3.Now, there are four unknownsa3d3,b3,c3,andZ and four equations in equation (16), so T3 and T˜3 can be solved easily. According to the transformation relationship between the scattering parameters and the transfer matrix [16], S parameters of the two-port network in Figure 3(d) can be obtained. Finally, the electromagnetic parameters of specimen 3 can be calculated by the NRW method (Equations (1) and (2)).


## 2.3. Experiment and Analysis

In this part, flexible material is measured. A piece of polytetrafluoroethylene (PTFE) with the thickness of 0.5 mm shown in Figure4 is adopted as specimen 3 to carry out the verification experiment. The electromagnetic parameters are obtained with the method proposed in this paper, which are compared with the reference values. The reference values are obtained from the measurement with the air coaxial line according to the standard [7], where a 2 mm PTFE specimen is adopted. For specimens 1 and 2, rigid materials code K04 with the thickness of 2 mm and 0.5 mm are selected, respectively. The inner and outer diameters of specimens all meet the test requirements of the air coaxial line, which are shown in Figure 4.Figure 4
Photo of specimens.The measurement setup is shown in Figure5, where the VNA is R&S ZNB20 and is calibrated by the calibration kit R&S ZVZ270 (type N, 50 Ω). The settings are as follows: frequency 0.1 GHz to 18 GHz, output power −10 dBm, IF bandwidth 700 Hz, 1601 sampling points, and no averaging applied to data. The outer diameter of the air coaxial line is 7.0 mm, the diameter of the inner conductor is 3.04 mm, and the length is 80 mm.Figure 5
Measurement setup.The results are shown in Figure6. The measurement results in blue are based on the proposed method in this paper and the reference values in red are based on the method in standard ASTM D7449. It can be seen that the results of the method proposed in this paper consist well with the reference value from 1 GHz to 18 GHz. It proves the effectiveness of the method proposed. At low frequencies (0.1 GHz ∼ 1 GHz), the curves of the method proposed show larger fluctuations. This is because the measurement with VNA shows greater uncertainty when the thickness of the specimen is only 0.5 mm [17]. It should be noted that the thickness of the substrate (specimen 1) in this paper should be chosen carefully to avoid resonance [18].Figure 6
Comparison between measurement results and reference values (the measurement results in blue are based on the proposed method in this paper and the reference values in red are based on the method in standard ASTM D7449): (a) real part of relative permittivity, (b) imaginary part of relative permittivity, (c) real part of relative permeability, and (d) imaginary part of permeability.
(a)(b)(c)(d)


## 3. Conclusions

A method for the electromagnetic parameters measurement of flexible materials based on air coaxial line is proposed in this paper. The method solves the problem that the specimen is easy to deform in the process of installation when measuring the electromagnetic parameters of flexible materials with the air coaxial line. The experimental results show that the proposed method is effective and feasible.In order to obtain the transfer matrix of specimen 1 in step 3, measurement procedure steps 1 and 2 are introduced. Actually, there are also some other solutions. For example, specimen 1 can be loaded at one certain position of the air coaxial line forS parameters measurement, and the transfer matrix can be calculated by phase extension then. However, the procedure in this paper is more maneuverable in engineering. It is also possible to fix the flexible specimen further by using two rigid specimens based on the method in this paper.



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