1. Introduction
Due to the advantages of lower computational requirements and readily available hardware, wireless local area networking (WLAN) has been widely used in military surveillance, industrial process control and environmental monitoring [1-3]. Recently, indoor localization based on WLAN has attracted significant research attention and growing interest [4]. The indoor localization algorithms can be divided into two categories: range-based and range-free. Typical range-based localization algorithms include time of arrival (TOA), time difference of arrival (TDOA), angle of arrival (AOA) and received signal strength indicator (RSSI), which have higher accuracy than that of range-free [3]. RSSI is widely used in indoor localization because its low power consumption and no additional hardware required. However, there are various obstacles in the actual indoor environment, such as wall, door and furniture, which will cause the NLoS interference in the wireless signals propagation path [5]. Wireless signals through the obstacle environment are affected by diffraction, reflection and scattering, which will cause RSSI attenuation and fluctuation [6-7]. Among the observation errors of RSSI, the NLoS caused by signals reflection and transmission path loss when wireless signals through the wall, is the main factor affecting the indoor localization accuracy. The ranging error caused by NLoS can reach 20%-50% of the communication radius [8]. Therefore, the key to wireless indoor localization using RSSI is to analyze the path loss of signals through the wall and establish the mathematical models.
At present, the research on the path loss of wireless signals through the medium focuses on the theoretical method and the empirical method. The theoretical method usually adopts deterministic or semi-deterministic methods to study the signal attenuation characteristics based on the propagation theory and physical laws of electromagnetic wave and numerical simulation. The finite element method (FEM), the plane wave expansion (PWE) method and the finite difference time domain (FDTD) method are used to simulate and analyze the propagation characteristics of electromagnetic wave through the medium [9-14]. According to the in-fluence of the permittivity, conductivity, permeability, incident frequency and incident angle on reflection coefficient and transmission coefficient, the attenuation characteristics of wireless signals through the medium are obtained. However, each of these methods has its drawbacks, such as high complexity, large amount of calculation [9]. In addition, it’s difficult to accurately obtain the actual permittivity, conductivity and permeability of medium.
The empirical method composes of deterministic method and statistical method. Statistical method is based on the empirical path loss models of wireless signals propagation and RSSI observations. The popular empirical path loss models, such as Okumura-Hata, COST 231, Keenan-Motley model and log-distance path loss model are the most widely used for path loss predictions [15-16]. The advantages of empirical path loss models are easier to implement than theoretical path loss models [6]. Moreover, stepwise regression, genetic algorithm, particle swarm optimization and machine learning are used to establish the empirical path loss model [6,17-18]. However, due to the observations error of RSSI, the calculated path loss has the irregular fluctuations and discontinuity of adjacent areas.
In order to obtain the actual regional path loss of wireless signals through wall, we propose a hybrid path loss model by combining theoretical and empirical models. The propagation process of wireless signals through the wall is divided into three sections, and the power loss relation between each key point is deduced based on incident angle, thickness and electromagnetic characteristic parameters of the wall. According to the power loss and RSSI definition, the path loss of signals through the wall is deduced, and the theoretical model of signals through the wall is established. Combined with the theoretical and empirical models of path loss, the electromagnetic characteristic parameters in the hybrid model are solved. The hybrid model of path loss can improve the path loss accuracy and maintain the spatial continuity of regional path loss.
The rest of this paper is organized as follows. In Section 2, we analyze the path loss process of wireless signals propagation through the wall, describe the establishment of theoretical model and empirical model of path loss, and present the hybrid model of path loss. In section 3 we describe our experiments and analyze the effect of each electromagnetic characteristic parameters on path loss, and the validity of the hybrid model for regional path loss is discussed. Finally, some conclusions from this study are given in section 4.
2. Modeling of path loss of wireless signals through the wall
2.1 The path loss process of wireless signals propagation through the wall
The propagation process of wireless signalsthrough the wall can be divided into three sections: before the incidence of the wall, through the wall and after output of the wall. During the propagation of signals through the wall, reflection and transmission of signals occur. From the transmitting node Tn to the receiving node Rn , the propagation paths are TnA , A' B' and BRn , respectively. The directions of reflection and transmission of signals incident-point A are AA'' and AA' , respectively. The directions of reflection and transmission of signal outputpoint B' are B' B'' and B' B , respectively. The propagation process of wireless signals through the wall is shown in Fig. 1.
Fig. 1. The propagation process of wireless signals through the wall
PTn is set as the power of transmitting node Tn , PRn is the power of receiving node Rn . PA , PA' , PB' and PB are the power of incident-point A , point A' , point B' and output-point B , respectively. The power unit is mw , and the power relationship at A , point A' , point B' and output-point B is [19] :
\(\begin{aligned}\left\{\begin{array}{c}P_{A^{\prime}}=\left(1-R_{A}\right) P_{A} \\ P_{B^{\prime}}=P_{A} e^{-2 \alpha l} \\ P_{B}=\left(1-R_{B}\right) P_{B^{\prime}}\end{array}\right.\end{aligned}\). (1)
where RA and RB are the power reflection coefficient of point A and point B , respectively. α is the attenuation constant of signals through the wall, and l is the propagation distance of signals in the wall.
The power reflection coefficients RA and RB are functions of signal reflection coefficient τA and τB , respectively. RA and RB are calculated in the same way. Take RA as an example, and can be expressed as [20-21]:
\(\begin{aligned}R_{A}=\left|\tau_{A}\right|^{2}=\left|\frac{\cos \theta_{1}-\sqrt{\frac{\varepsilon_{2}}{\varepsilon_{1}}-\sin ^{2} \theta_{1}}}{\cos \theta_{1}+\sqrt{\frac{\varepsilon_{2}}{\varepsilon_{1}}-\sin ^{2} \theta_{1}}}\right|^{2}\end{aligned}\), (2)
where ε1 and ε2 are the permittivity of air and wall, respectively. θ1 is the incident angle, θ2 is the transmission angle in the wall. Based on Snell's law of refraction, the incident angle and transmission angle have the following relation [22]:
\(\begin{aligned}\frac{\sin \theta_{2}}{\sin \theta_{1}}=\sqrt{\frac{\varepsilon_{1}}{\varepsilon_{2}}}=\sqrt{\varepsilon_{r}}\end{aligned}\), (3)
where the ratio of ε1 to ε2 is defined as the relative permittivity εr .
Since air and wall are weak loss media, the attenuation constant of signal through the wall can be approximately expressed as [19]:
\(\begin{aligned}\alpha=\omega \sqrt{\varepsilon_{2} \mu_{2}} \sqrt{\frac{1}{2}\left[\sqrt{1+\frac{\sigma_{2}^{2}}{\omega^{2} \varepsilon_{2}^{2}}}\right]} \approx \frac{1}{2} \sigma_{2} \sqrt{\frac{\mu_{2}}{\varepsilon_{2}}}\end{aligned}\), (4)
where ω is angular frequency, σ2 , μ2 are the conductivity and permeability of the wall, respectively.
Combined with equation (3), the propagation distance l of signals in the wall can be expressed as:
\(\begin{aligned}l=d_{\text {wall }} / \cos \theta_{2}=d_{\text {wall }} / \sqrt{1-\frac{\varepsilon_{1}}{\varepsilon_{2}} \sin ^{2} \theta_{1}}\end{aligned}\), (5)
where dwall is the thickness of wall.
2.2 Theoretical model of path loss of signals through the wall
The path loss of wireless signals caused by the wall, including reflection and transmission loss, can be calculated by the total loss of the transmitting node to the receiving node minus the path loss of TnA and BRn . According to the definition of path loss, the total loss from transmitting node Tn to receiving node Rn is [23-24]:
PLtotal[dB] = PTn[dBm] − RSSIRn[dBm] (6)
Similarly, the path loss from transmitting node Tn to point A is:
PLTnA[dB] = PTn[dBm] − RSSIA[dBm] (7)
Combined with equation (1), the path loss from point B to receiving node r is:
\(\begin{aligned}P L_{B R n}=\frac{P_{B[m w]}}{P_{R n[m w]}}=\frac{\left(1-R_{B}\right)\left(1-R_{A}\right) e^{-2 \alpha l} P_{A[m w]}}{P_{R n[m w]}}\end{aligned}\) (8)
The unit of path loss converted into dBm can be expressed:
PLBRn[dB] = 10 lg(1-RB)(1-RA)e-2αl + RSSIA[dBM] − RSSIRn[dBm] (9)
Therefore, the loss caused by wall reflection and transmission is:
PLwall[dB] = PLtotal[dB] - PLTnA[dB] - PLBRn[dB] = 10lg(1-RB) (1-RA)e-2αl (10)
If the incident angle, permittivity, conductivity and permeability of the wall can be accurately obtained, the theoretical model of path loss of signals through the wall can be established. The advantage of the theoretical model of path loss of wireless signals through the wall is that it can reflect the law of signals attenuation by wall and maintain the regional continuity of path loss. However, the permittivity, conductivity and permeability of wall usually cannot be accurately obtained, which limits the practical application of the theoretical model.
2.3 Statistical model of path loss of signals through the wall
Statistical model can be established by the empirical path loss models of wireless signals propagation and RSSI observations. The most commonly used empirical model is log-distance path loss model because of its accuracy and convenience [25]. The statistical model of the path loss of signals through wall is based on the total loss from the transmitting node to the receiving node, minus the path loss of the same distance of line of sight (LoS), which is calculated by statistical method. When there is no wall barrier between the transmitting node and the receiving node, the LoS path loss can be expressed as [5, 25]:
\(\begin{aligned}P L_{L o S[d B]}=P_{T n[d B m]}-R S S I_{d_{0}[d B m]}+10 \eta \lg \left(\frac{d_{T n R n}}{d_{0}}\right)\end{aligned}\) (11)
where, d0 is the reference distance, RSSId0 is the signal strength with distance of d0 from transmitting node, dTnRn is the distance between transmitting node and receiving node. η is the regional path loss index, which can be calculated by statistics of the transmitting node and multiple receiving nodes before the incidence of the wall.
Combined with equation (6), the NLoS error caused by wall is:
\(\begin{aligned}P L_{N L o S[d B]}=P L_{\text {total[dB] }}-P L_{L O S[d B]}=R S S I_{d_{0}[d B m]}-R S S I_{R n[d B m]}-10 \eta \lg \left(\frac{d_{T n R n}}{d_{0}}\right)\end{aligned}\) (12)
The statistical model of path loss caused by wall can be established by RSSI at d0 from the transmitting node, RSSI at the receiving node, and regional path loss index. The statistical model of signals path loss through the wall is based on the RSSI observations, which can better reflect the actual environment of signals attenuation. However, since η solved by the least square method reflects the path loss index of the region, and RSSI has observation error, the established path loss statistical model has large error at some observation points. The calculated path loss by the statistical model has the irregular fluctuations and discontinuity of adjacent areas.
2.4 Hybrid model of path loss of signals through the wall
In practice, the path loss of the theoretical model PLwall and the path loss of the statistical model PLNLoS should be approximately equal. Therefore, combining the theoretical model established by equation (10) and the statistical model established by equation (12), a hybrid model can be established as:
\(\begin{aligned}R S S I_{d_{0}[d B m]}-R S S I_{R n[d B m]}-10 \eta \lg \left(\frac{d_{T n R n}}{d_{0}}\right)=-10 \lg \left(1-R_{B}\right)\left(1-R_{A}\right) e^{-2 \alpha l}\end{aligned}\) (13)
Based on RSSI observations and calculated regional path loss index η , the least square method is used to solve the relative permittivity εr and the attenuation constant α of the wall. The solved εr and α can be substituted into equation (10) to solve the path loss of wireless signals through the wall. Then, the regional path loss of wireless signals through wall can be solved.
The Hybrid model is based on theoretical model and statistical model, and its modeling process includes both models, with the main steps of this modeling process described in Algorithm 1.
Algorithm 1 The Hybrid modeling process
Input: Transmitting power PTn , distance between Tn1 and Tn2, RSSId0 of reference distance d0
, incident angle θ1 , RSSI observations
Step 1: Calculate the regional path loss index η under line-of-sight condition, using RSSI observations of each receiving node in front of the wall and logarithmic distance path loss model;
Step 2: Calculate the NLoS error PLNLoS under non-line of sight condition based on RSSI observations of each receiving node behind the wall, the regional path loss index η and logarithmic distance path loss model;
Step 3: Combine the theoretical model and the statistical model, calculate the relative permittivity εr and the attenuation constant α , using RSSI observations of each receiving node behind the wall and the least square method;
Step 4: Substitute the relative permittivity εr and the attenuation constant α into the theoretical model;
Output: The regional path loss of signals through the wall
3. Experimental Results and Analysis
This section consists of four main parts: the RSSI observation experiment of wireless signals through the wall, the theoretical model established by the empirical values of electromagnetic characteristic parameters of the concrete wall, the hybrid model of path loss through wall established based on RSSI observations, and the validity of the hybrid model for regional path loss.
3.1 The RSSI observation experiment of wireless signals through the wall
In order to analyze the path loss of signals through the wall, the RSSI observation experiment is designed. The experiment is carried out on the second floor of the gymnasium. The internal dimensions of the lounge are 8m long and 4.8m wide, and the outside of the lounge is a capped terrace. The thickness of the concrete wall is 0.24m, and the wall material is unknown. The transmitting node is placed in the lounge, and located at Tn1 (-1, 0) and Tn2 (-2, 0) in turn. The receiving node is deployed on each grid point of the lounge and terrace, and the grid spacing is 0.5 m. The definition of the coordinate system, nodes distribution and region division of the RSSI observation experiment are shown in Fig. 2. The transmitting node and receiving node are ZigBee module (2.4G), and fixed on the tripod with height of 1.5m. The transmitting node is powered by USB mobile power supply. The laptop is connected to the receiving node, supplies power to the receiving node and stores data. The transmitting power is 4.5dBm, the sampling interval is 0.1s, and the sampling time of each grid point is 10min. The scene and measurement of the RSSI observation experiment of signals through the wall are shown in Fig. 3.
Fig. 2. The definition of the coordinate system, nodes distribution and region division of the RSSI observation experiment
Fig. 3. The scene and measurement of the RSSI observation experiment
The receiving nodes are distributed in three zones. The RSSI observations of each receiving node in zone I are used to calculate the path loss index of the region. The RSSI observations of each receiving node in zone II are used to establish the statistical model and the hybrid model of path loss of signals through the wall. The RSSI observations of each receiving node in zone III are used to verify the effect of the established model.
3.2 The theoretical model established by the empirical values of electromagnetic characteristic parameters of the concrete wall
3.2.1 The effect of electromagnetic characteristic parameters on path loss
Given the relative permittivity, attenuation constant and wall thickness, the theoretical model of path loss of signals through the wall can be established based on the equation (10). Therefore, empirical values for these parameters can be used if the wall material is known. Researchers have studied the electromagnetic properties of concrete walls [26-28]. In the literature [26], Kaplanvural et al tested the relative permittivity according to the water content of concrete, and the value range of relative permittivity was 0.1764 to 0.4202, with an average value of 0.247. In the literature [27], Ramaniraka et al showed that the absorption attenuation constants of concrete are 7 and 9 Np/m, with an average value of 8. In the literature [28], Stone carried out the experiments of electromagnetic signal attenuation in concrete walls with thickness of 0.102m, 0.203m and 0.305m, respectively. Since the wall thickness measured in the experiment is 0.24m, the effect of 0.24m wall thickness on path loss is simulated simultaneously. According to the parameters of concrete wall mentioned above, the path loss of theoretical model of signals through the wall can be simulated, and the relationship between path loss and relative permittivity, attenuation constant and wall thickness can be analyzed. The values of relative permittivity, attenuation constant, wall thickness and incident angle are shown in Table 1.
Table 1. The values of relative permittivity, attenuation constant, wall thickness and incident angle.
In order to analyze the effect of each parameter on the path loss at different incident angles, one parameter is varied while the other parameters take intermediate values. When dwall =0.24 and α =8, the path loss at different relative permittivity varies with incident angle as shown in Fig. 4. When dwall =0.24 and εr =0.247, the path loss at different attenuation constant varies with incident angle as shown in Fig. 5. When α =8 and εr =0.247, the path loss at different wall thickness varies with incident angle as shown in Fig. 6.
Fig. 4. The path loss at different relative permittivity varies with incident angle
Fig. 5. The path loss at different attenuation constant varies with incident angle
Fig. 6. The path loss at different wall thickness varies with incident angle
It can be seen from Fig. 4, Fig. 5 and Fig. 6 that the path loss increases with the increase of incident angle. The path loss increases slowly with the incident angle form 0° to 70°, and the path loss increases sharply with the incident angle from 70° to 89°. The wall thickness has a great influence on the path loss, followed by the attenuation constant, and the relative permittivity has a small influence on the path loss.
3.2.2 Regional path loss based on theoretical model and empirical values of electromagnetic characteristic parameters
Based on the empirical values of electromagnetic characteristic parameters of concrete wall and equation (10), the theoretical model of signal path loss through the wall can be established. Since the coordinates of each grid points are known, the angle between the line of transmitting node and receiving node and the wall can be solved. The range of angle between the line of Tn1(-1,0) and receiving nodes is 0° to 67.7064°, and the range of angle between the line of Tn1(-2,0) and receiving nodes is 0° to 53.3753°. The maximum value of the above two angle ranges is less than 70°. The angle between the line of transmitting node and receiving node and the wall has little effect on the path loss, and the angle can be approximated as the incident angle. The path loss of zone II corresponding to Tn1(-1,0) and Tn2(-2,0) are shown in Fig. 7 and Fig. 8, respectively.
Fig. 7. The path loss of zone II corresponding to Tn1(-1,0) based on theoretical model of electromagnetic characteristic parameters empirical value (εr =0.247 , α = 8 , dwall =0.24 )
Fig. 8. The path loss of zone II corresponding to Tn2(-2,0) based on theoretical model of electromagnetic characteristic parameters empirical value (εr =0.247 , α = 8 , dwall =0.24 )
It can be seen from Fig. 7 and Fig. 8 that the path loss solved by the theoretical model changes with the position relationship between different transmitting node and receiving node. The path loss increases with the increase of incident angle, and maintains the continuity in adjacent areas. With the increase of incident angle, the signals reflection increases and the transmission decreases, which leads to the increase of the path loss with the increase of the incident angle. However, due to the empirical value of the electromagnetic characteristic parameters of the concrete wall are used, the calculated path loss of the wall is usually inconsistent with actual path loss. Furthermore, if the wall material is unknown, the electromagnetic characteristics of the wall cannot be obtained, and the theoretical model of the path loss of the wireless signals through the wall cannot be established.
3.3 The hybrid model of path loss of signals through the wall established based on RSSI observations
Based on the power of transmitting nodes Tn1(-1,0), Tn2(-2,0) and the RSSI observations of each receiving node, the RSSI observations are denoised by Kalman filter. The fluctuation range of RSSI is 2-5dbm, and the mean value is taken to participate in modeling. Using the RSSI of each receiving node in zone I and formula (11), the calculated regional path loss index of LoS is η=1.7787 . Using the denoising RSSI of each receiving node in zone II , the statistical model and the hybrid model of the path loss through the wall can be established by equation (12) and equation (13), respectively. The relative permittivity εr and the attenuation constant α of the wall are solved. Introduce the solved εr and α into formula (10), then the path loss through the wall is obtained. The model parameters are shown in Table 2, and the RMSE is the root mean square error of the hybrid model. The path loss of zone II based on the statistical model and RSSI observations is shown in Fig. 9 and Fig. 10. The path loss of zone II based on the hybrid model and RSSI observations is shown in Fig. 11 and Fig. 12.
Table 2. Parameters of the hybrid model of path loss through wall based on RSSI observations.
Fig. 9. The path loss of zone II corresponding to Tn1(-1,0) based on the statistical model and RSSI observations
Fig. 10. The path loss of zone II corresponding to Tn2(-2,0) based on the statistical model and RSSI observations
Fig. 11. The path loss of zone II corresponding to Tn1(-1,0) based on the hybrid model and RSSI observations
Fig. 12. The path loss of zone II corresponding to Tn2(-2,0) based on the hybrid model and RSSI observations
As can be seen from Fig. 9 and Fig. 10, the established statistical model of path loss through wall shows great fluctuation of path loss corresponding to each grid point due to RSSI observations error, failing to express the actual trend of regional path loss. For the hybrid model of path loss through wall, the denoising RSSI observations and least square method are used to solve the attenuation constant and relative permittivity, and the observation RSSI error of partial receiving nodes can be reduced. As can be seen from Fig. 11 and Fig. 12, the hybrid model can well express the trend and regional continuity of path loss through wall.
For the hybrid model of path loss corresponding to the transmitting node at different positions, the path loss trend is basically the same, and the solved relative permittivity and the attenuation constant have small differences. The path loss difference of the transmitting node Tn1 at position (-1,0) is 2-4dB compared with that of the transmitting node Tn2 at position (- 2,0), and the RMSE of the corresponding hybrid model is slightly smaller. The result indicates that the hybrid model is also affected by RSSI observations error, and the regional path loss is independent of the position of the transmitting node.
3.4 The verification of the hybrid model validity
The validity of the hybrid model is analyzed from three aspects: unknown material wall, model accuracy and prediction ability. In the RSSI observation experiment, the wall material is unknown. The path loss is calculated by the theoretical model based on the empirical values of electromagnetic characteristic parameters and the hybrid model based on measured RSSI, respectively. By comparing the relative permittivity and attenuation constants in Table 1 and Table 2, the empirical value of the concrete wall is close to the calculated value of the unknown material wall. Accordingly, from Fig. 7, Fig. 8, Fig. 11 and Fig. 12, the trend of path loss calculated by the theoretical model and the hybrid model is basically the same, and the path loss at the corresponding position has a difference of 3-5dB. The RMSE calculated in the modeling process of hybrid model represents the internal accuracy of the model. Form Table 2, the RMSE of the hybrid model established corresponding to Tn1(-1,0) and Tn2(-2,0) is 6.0803 and 6.1968, respectively. The RMSE of the hybrid model is basically consistent with the fluctuation range of the RSSI observations. Therefore, the hybrid model can be used to calculate the path loss of the signals through the wall.
In order to verify the prediction ability, the hybrid model are used to inversely calculate the RSSI of each grid points in zone III , which is an extended region. The RSSI observations of receiving nodes in zone III are not participate in the establishment of the hybrid model, and are only used for comparison with inversely calculated RSSI. The measured RSSI and inversely calculated RSSI corresponding to Tn1 and Tn2 are shown in Fig. 13 and Fig. 14, respectively.
Fig. 13. The measured RSSI of zone III and inversely calculated RSSI corresponding to Tn1(-1,0)
Fig. 14. The measured RSSI of zone III and inversely calculated RSSI corresponding to Tn2(-2,0)
As can be seen from Fig. 13 and Fig. 14, the inversely calculated RSSI by the hybrid model is basically consistent with the measured RSSI. The RMSE of measured RSSI and inversely calculated RSSI corresponding to Tn1 is 4.9520, and the RMSE of measured RSSI and inversely calculated RSSI corresponding to Tn2 is 4.204. The RMSE of measured RSSI and inversely calculated RSSI is the external accuracy of the hybrid model, represents the prediction ability of the model. The results show that the hybrid model can be used to predict the regional path loss. However, the accuracy of hybrid model and the effect of model prediction are affected by RSSI observation errors. In addition, the heterogeneity of wall materials also affects the accuracy of modeling and model prediction.
4. Conclusion
The localization validity of RSSI can be improved by modeling and correcting the path loss of wireless signalsthrough the wall. The theoretical model of path loss of wireless signals through the wall is difficult to obtain the accurate electromagnetic characteristic parameters in practical scenarios, and the path loss solved by the statistical model of wireless signals through wall has irregular fluctuation and discontinuity of adjacent areas. The hybrid model of path loss of signals through the wall is proposed by combining the theoretical model and statistical model. The theoretical model can be established by the empirical values of electromagnetic characteristic parameters of the concrete wall. The path loss increases with the increase of incident angle, and increases sharply with the incident angle from 70°to 89°. The wall thickness has a great influence on the path loss, followed by the attenuation constant, and the relative permittivity has a small influence on the path loss. However, if the wall material is unknown, the electromagnetic characteristics of the wall cannot be obtained, and the theoretical model of the path loss of the wireless signals through the wall cannot be established. Based on the RSSI observation experiment, the statistical model and the hybrid model of path loss of signals through wall are established, respectively. The results show that the hybrid model not only solves the inaccurate empirical values of electromagnetic propagation parameters in the theoretical model, but also weakens the influence of RSSI observation errors in the statistical model. The hybrid model can well express the actual trend of regional path loss and maintain the pass loss continuity of adjacent areas, and can be used to predict the regional path loss.
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