Analysis of a Low-Earth Orbit Satellite Downlink Considering Antenna Radiation Patterns and Space Environment in Interference Situations

Abstract

This paper investigates a low-Earth orbit (LEO) satellite downlink for high-speed data communication in interference situations. A choke ring horn type antenna is used as the data transmitting antenna with an isoflux pattern in the LEO satellite, which has a beam coverage of ±51.6° and a bore-sight gain of 4.4 dBi at 8 GHz. The receiving antenna on the ground station is a parabolic type antenna with a diameter of 11.3 m, and it has a half-power beam width (HPBW) of 0.2° with a maximum gain of 59 dBi at 8 GHz. The jamming-to-signal ratio (J/S) is calculated assuming that the LEO satellite transmits signals to the ground station, and an elevation angle of the interference source varies from 0° to 90° at an altitude of 10 km. Applying antenna characteristics, such as HPBWs and side lobes, to the calculated space wave path loss makes it possible to predict the J/S results according to the location of the interference source and the satellite. The results show that it is necessary to consider the space environment to accurately analyze the LEO satellite downlink, especially at the low elevation angle of the satellite.

1. Introduction

Low-Earth orbit (LEO) satellites have often been used to acquire image data for Earth observations, such as natural disasters and terrain changes, using synthetic aperture radars (SARs) [1,2]. These LEO satellites have a rapid velocity of around 7.6 km/s at an altitude of 550 km to a fixed point on a ground station and transmit the image data through a downlink which is the X-band (8025 MHz~8400 MHz) for the high-rate data. In order to predict the data transmission situation from LEO satellites in rapidly changing interference situations, many studies have been conducted on the link budget analysis in terms of path loss [3], the elevation angle of the satellite [4], and non-line-of-sight situations [5,6,7]. However, link budget analysis studies on misaligned off-axis and interference situations considering antenna radiation patterns and space environment have not yet been sufficiently performed. In particular, there are no in-depth studies of scenarios where power controllable interference sources are exposed to the side lobe of the receiving antenna. In addition, most previous studies have been conducted considering losses in the near-ground atmosphere [8,9,10], without accounting for the entire space environment.

In this paper, we investigate an analysis of a LEO satellite downlink, considering antenna patterns and the space environment in interference situations where the side lobe of a ground station antenna is exposed to a strong interference signal source. To calculate the link budget, considering the bore-sight error loss between the ground station and the satellite when the LEO satellite moves rapidly over the Earth, antenna patterns of the ground station and the LEO satellite are employed. The ground station antenna is assumed to be a parabolic type, and its radiation pattern is calculated by using methods of geometrical optics (GO) and physical optics (PO) [11]. The radiation pattern of a choke ring antenna, which it is assumed is that used in the LEO satellite, is obtained through a full electric magnetic (EM) simulation. The actual radiation patterns of the receiving and transmitting antennas are obtained and applied to the study, in order to more accurately estimate the data link budget when interference is strong in the side lobe of the receiving antenna. Finally, an analysis of the interference situation based on the space environment is calculated when the interference source moves over the ground station in various interference situations. We employ ray tracing techniques and geometrical optics to analyze the interference situation when the LEO satellite is located at a specific low elevation angle. Jamming-to-signal (J/S) ratio results according to the space environments are examined and they differ by about 3 dB at low elevation angles according to the space environments.

2. Antenna Simulation for LEO Downlink Analysis

Figure 1 shows the conceptual figure of the downlink scenario when the LEO satellite transmits high-rate data in interference situations, where the side lobe of the ground station antenna is exposed to a strong interference signal source. The elevation angle of the satellite is θ_gs, and the elevation angle of the interference source is θ_j. When the LEO satellite transmits data through the downlink to the ground station, the free-space loss L_f can be obtained by Formula (1)

$$L_f(\mathrm{dB})=20{\log }_{10}(d)+20{\log }_{10}(f)+20{\log }_{10}(\frac{4\pi }{c_0})$$

(1)

where d is the distance between the LEO satellite and the ground station and f is the carrier frequency. The LEO satellite and the ground station antenna can be slightly misaligned with off-axis situations in the space environment, and a bore-sight error loss L_b can be calculated using Equation (2)

$$L_b(\mathrm{dB})=12{\left(\frac{{\theta }_b}{{\theta }_h}\right)}^2$$

(2)

where θ_h is the half-power beam width (HPBW) of the ground station antenna, and θ_b is the bore-sight error angle. It is assumed that there is no manufacturing error of the receiving antenna, and the antenna is ideally well matched to the RF system. It is also assumed that the performance of the receiver system does not change even when the side lobe of the receiving antenna is exposed to strong interference [12]. To calculate the link budget between the LEO satellite and the ground station, the received power P_r can be expressed as (3)

$$P_r(\mathrm{dBm})=P_t+G_t+G_r-L_f-L_b-L_{at}$$

(3)

where P_t is the transmitting power, G_t is the gain of the transmitting antenna in the LEO satellite, and G_r is the receiving antenna gain of the ground station. We also consider the atmospheric loss L_at due to significant refraction and attenuation in the atmosphere. This loss is significantly observed, especially when the LEO satellite is at the low elevation angle. The atmospheric loss in the space environment will be discussed in more detail in the next section.

Figure 2a,b show the transmitting antenna of the satellite and the far-zone radiation pattern. Patch arrays [13,14,15], helical wires [16,17], and corrugated or choke ring horns [18,19,20,21,22,23] are often used as data transmission antennas for LEO satellites. Among them, the choke ring horn antenna is used as the transmitting antenna in this study, because it has a relatively simple shape and can easily have the required radiation pattern with wide beam coverage. In particular, an isoflux pattern is required to maintain uniform received power at the Earth’s surface during downlink data transmission through the X-band. To obtain the isoflux pattern, the antenna is designed based on a requirement mask for the radiation pattern, which is announced in the CNES [24,25,26]. The designed antenna has a diameter d_t of 77.4 mm, and its characteristics are obtained using the CST studio suite full EM simulation tool. It has a beam coverage of ±51.6° with a bore-sight gain of 4.4 dBi at 8 GHz.

Figure 3a,b show the receiving antenna of the ground station and the far-zone radiation pattern. In general, the ground station antenna is designed considering the regulation of ITU-R S.508-6 for efficient communication by minimizing interference [27]. The receiving antenna is a parabolic type with a diameter d_r of 11.3 m, of which the radiation pattern is obtained using the GO and PO methods. This antenna is fed by a rectangular horn antenna, and has an HPBW of 0.2° with a maximum gain of 59 dBi at 8 GHz. The receiving antenna is designed following ITU-R S.508-6 regulations to have side lobe levels (SLLs) of less than the required mask. The actual radiation patterns of the receiving and transmitting antennas are used, in order to more accurately estimate the data link budget when interference is strong in the side lobe of the receiving antenna.

3. Space Wave Propagation for LEO Downlink Analysis

In the LEO satellite data transmitting scenario, EM waves propagate through the troposphere, stratosphere, and ionosphere to reach ground stations. Thus, losses are affected and increased by the phenomena of refraction, attenuation, and reflection between each layer. To predict EM wave propagation in space environments, it is necessary to calculate the refractive indices of the troposphere and the stratosphere. The reflection and transmission of EM waves are then obtained at the interfaces of multi-layered spheres. The ray tracing technique and geometrical optics are employed to calculate EM wave propagation at interfaces among the troposphere, stratosphere, and ionosphere in a space environment.

Figure 4 shows the GO model when a ray passes through multi-layered atmospheric spheres [28]. The wave propagation characteristics can be determined by calculating the transmission and reflection at each interface of the multi-layered spheres. The polarization of the incident wave is also considered when calculating the reflection and transmission coefficients at each layer [29]. n₀, n₁, …, n_I are the effective refractive index in the divided layers of ionosphere, and n_I+1, …, n_T are the effective refractive index in the divided layers of troposphere. θ_oi, θ_Ii, and θ_Ti are incident angles on each layer of ionosphere and troposphere. E_i0 is the electric field incident on the multi-layered ionosphere, E_t0 is the electric field transmitted through each interface of the multi-layered ionosphere, and E_i1 is the electric field incident on the multi-layered troposphere. E_t1 is the electric field transmitted through the multi-layered troposphere, and E_T is the electric field reaching the observation point which is presented the blue circle marker.

The effective refractive index according to the altitude in the troposphere and the stratosphere can be approximated by the equations in [30,31]. The refractive index can be determined by temperature, pressure, and water vapor pressure obtained using daily updated weather data from the University of Wyoming [32]. Since the ionosphere has a plasma ion layer caused by solar radiation, it affects the refraction, attenuation, and reflection of EM waves [33]. The characteristics of the ionosphere and prediction methods are employed in [34] to investigate wave propagation in the ionosphere. The relative permeability of the atmosphere is assumed to be 1, and the anisotropy of the electrical conductivity is not considered.

Figure 5a,b show the bore-sight error and atmospheric attenuation that occur when transmitting signals from the LEO satellite to the ground station on Earth. The bore-sight error increases as the satellite elevation angle θ_gs decreases, as shown in Figure 5a. In particular, the bore-sight error significantly increases when considering the space environments, as shown in the blue line. At a low elevation angle (θ_gs = 10°), the difference in bore-sight error is 0.04° and at a high elevation angle (θ_gs = 90°), the difference is 0°. The reason for the large difference, especially at the low elevation angle, is the increased ray refraction. Figure 5b shows the atmospheric attenuation, and again, how the attenuation considerably increases as the satellite elevation angle θ_gs decreases. This result shows that at the low elevation angle, the total path is increased by the refraction, resulting in greater attenuation.

Figure 6 shows the normalized received power at the Earth’s surface according to latitude and longitude when transmitting signals from the LEO satellite. We assume that the elevation angle of the LEO satellite is θ_gs = 10°, and the main lobe is steered at an observation point of 78.23° latitude and 15.408° longitude. Figure 6a shows the normalized received power in free space, whereas Figure 6b shows the result in the space environment. This clearly demonstrates that there is a difference between the observation point and the location of the maximum received power due to the bore-sight error in the space wave propagation.

4. Analysis of LEO Satellite Downlink

To analyze the LEO downlink in interference situations, we set the scenario considering antenna patterns, the path loss in the space environment, and the interference source. The radiation patterns were obtained from the data transmitting antenna of the LEO satellite and the receiving ground station antenna in Section 2. We considered the bore-sight error loss by assuming that the transmitting and receiving antennas are slightly misaligned in the off-axis situation. The path loss calculated in Section 3 was then applied in the downlink analysis. In the given scenario, the LEO satellite transmits the data to the ground station, and the ground station antenna tracks the LEO satellite. The LEO satellite is located at the elevation angle of θ_gs. At the same time, it is assumed that the elevation angle θ_j of the interference source moves from 0° to 90° at an altitude of 10 km. The input power of the interference source can be adaptively controlled from 100 dBm to 150 dBm and is connected to a 10 dBi gain antenna. The interference power range was derived to maintain the target J/S such as 0 dB, 5 dB, 10 dB, and 15 dB when the interference source is located at various elevation angles. The detailed link budget parameters are listed in

Table 1. Downlink parameters for the link budget in the scenario.

Downlink Parameters	Values
Receiving antenna gain	59 dBi
Satellite altitude	550~2200 km
Frequency range	8025~8400 MHz
Transmitting power	30 dBm
Transmitting antenna bore-sight gain (dBi)	4.4 dBi
Effective isotopic radiation power (EIRP), Gt + Pt	34.4 dBm
Free-space path loss	Lf dB
Bore-sight error loss	Lb dB
Atmospheric attenuation	Lat dB
Interference source power	100~150 dBm
Interference source antenna gain	10 dBi
Interference source altitude	10 km

.

Figure 7 shows the J/S result according to the elevation angle θ_j and the interference power. “○” markers indicate the points at which the J/S is 0 dB. As can be seen, the result exhibits a large variance due to fluctuation in the antenna radiation pattern, which makes it difficult to observe the J/S tendency. To overcome this issue, we applied the regression model to “○” makers in our J/S result. This regression model (f₁) is based on a quadratic function often used to fit raw data to a curved distribution [35,36]. The quadratic regression model can be expressed as (4)

$$f_1({\theta }_j)=a_1{\theta }_j^2+a_2{\theta }_j+a_3$$

(4)

where a₁, a_2, and a₃ are coefficients that best fit the points (“○” makers) with J/S = 0 dB, which is illustrated as the solid line. We then easily examined the tendency of the results by observing the single curved line.

Figure 8 illustrates J/S according to the elevation angle θ_j and the interference power at θ_gs = 10°. To obtain the J/S in the space environment, we applied the bore-sight error loss and atmospheric attenuation in Section 3 to the link budget calculation. In Figure 8a, the solid line indicates the regression model for the points with J/S = 0 dB in the space environment. To observe the effect of the space environment, we also examined the regression model (dashed line) without the space environment. To quantify the difference between the two cases, we defined β, which is the average difference between the two models expressed as (5):

$$\beta =\frac{1}{N}{\displaystyle \sum _{k=1}^N\left|P_s(k)-P_f(k)\right|}$$

(5)

where N is the number of elevation angle points, P_s is interference power of each elevation angle with the space environment, and P_f is interference power without the space environment. When the J/S = 0 dB, β is 3.53, which is due to the high atmospheric loss and bore-sight error at the low elevation angle of θ_gs = 10°. Figure 8b presents the regression model when J/S is changed to 5 dB, and it was observed that β is 2.56 dB in this case. Figure 8c,d illustrate the regression models with J/S = 10 dB and J/S = 15 dB, where β are 2.16 dB and 1.63 dB, respectively.

Figure 9 illustrates J/S with θ_gs = 60°, which is the result of seeing the effect of the space environment when the elevation angle θ_gs is increased. In Figure 9a, the solid and dashed lines indicate the regression models with and without the space environment when J/S is 0 dB. A reduced β of 0.02 was observed in this case because the atmospheric loss and bore-sight error decrease as the elevation angle θ_gs approaches 90°. Figure 9b, Figure 9c and Figure 9d present the regression models when J/S is changed to 5 dB, 10 dB, and 15 dB, respectively. For each case, β were 0.37 dB, 0.62 dB, and 0.14 dB, respectively. The detailed values of J/S results are listed in

Table 2. J/S results depending on the J/S and θ_gs.

θgs	10				60
J/S (dB)	0	5	10	15	0	5	10	15
β (dB)	3.53	2.56	2.16	1.63	0.02	0.37	0.62	0.14

. As can be seen from the table, the smaller the elevation angle, the larger the overall β. The results demonstrate that it is necessary to consider the space environment to accurately analyze the LEO satellite downlink, especially at the low elevation angle of the satellite.

5. Conclusions

We analyzed the LEO satellite downlink, considering antenna patterns and the space environment in interference situations. The actual radiation patterns of the receiving and transmitting antennas were applied to more accurately estimate the data link budget when interference was strong in the side lobe of the receiving antenna. The choke ring horn type antenna with a diameter of 77.4 mm was used as the transmitting antenna in the LEO satellite, which had an HPBW of 103.2° and a maximum gain of 6.6 dBi at 8 GHz. The receiving antenna in the ground station was the parabolic type of antenna with a diameter of 11.3 m and an HPBW of 0.2°, with a maximum gain of 59 dBi at 8 GHz. We applied the space environment by employing the ray tracing technique and geometrical optics to calculate EM wave propagation. To observe the effects of the space environment, we examined the regression model with and without the space environment. To quantify the difference between the two cases, we defined β, which was the average difference between the two models. At θ_gs = 10°, β was from 1 dB to 4 dB, whereas β was from 0 dB to 1 dB at θ_gs = 60°. These results demonstrated that the bore-sight error and atmospheric attenuation increase due to the increased ray refraction, especially at low elevation angles, and thus it was important to consider the space environment for LEO satellite downlink analysis in interference situations.