4. Analysis of Experimental Results
Reflecting practical scenarios, the channel simulation parameters were configured in
Table 1.
Figure 3 depicts the variations in power consumption at node R, system delay, and system energy efficiency under different wake-up ratios (N1/N2). Where, N1 represents the number of consecutive cycles node R executes the DRX process after being woken up by a WUS, while N2 denotes the number of consecutive cycles node R remains in idle mode without WUS activation. To prevent the tag from being perpetually active and enhance its energy-saving performance, the constraint N2 was imposed. For each fixed N1 value, three progressively increasing N2 values were selected, forming three distinct ratio groups. The baseline scenario (N1=N2=1) represents the conventional wake-up mechanism where a WUS is transmitted whenever the source has data for node R.
From the power consumption curves, it is observed that without ratio-based optimization of the WUS transmission scheme, node R exhibits the highest power consumption and energy efficiency, coupled with the lowest delay. Within each experimental group defined by a fixed N1 value, the condition N1/N2=1 consistently corresponds to the highest power consumption, highest energy efficiency, and lowest delay for that group. Furthermore, fluctuations in power consumption, delay, and energy efficiency under this specific ratio (N1/N2=1) are minimal. This stability is attributable to the synchronous and equal-magnitude changes in N1 and N2, , which exert little net effect on the total number of wake-up cycles. When the value of N1 is held constant and N2 is increased, the power consumption at node R and the overall system energy efficiency decrease, while the system delay increases. This trend stems from the extended duration node R spends in the RRC_IDLE state resulting from a larger N2. This reduced state activity lowers the frequency of data processing, thereby decreasing power consumption. However, the consequent reduction in throughput also diminishes system energy efficiency and increases latency. Additionally, analysis reveals that as the value of N1 increases across the experimental groups, the fluctuations in power consumption and energy efficiency within the corresponding group decrease, whereas fluctuations in delay increase. This behavior results from the narrowing gap between N1 and N2 (i.e., the ratio N1/N2 progressively approaches 1) for higher N1 values. Consequently, for power-sensitive devices, employing a larger N2/N1 ratio is recommended to minimize energy consumption. Conversely, for latency-sensitive devices, ratios where N2 and N1 are closer in value are more suitable to prioritize lower delay.
Figure 4 illustrates the variation of energy efficiency with respect to the power splitting ratio ρ under distinct base station transmit power levels, denoted by markers of varying colors and shapes. Collectively, the three energy efficiency curves exhibit a monotonic decreasing trend as ρ increases progressively from 0.1 to 0.9. This behavior arises because, while a higher ρ enhances the energy harvested at R, consequently increasing the transmit power from R to C, it simultaneously reduces the throughput of information received at R. Critically, the higher path loss experienced at C relative to R means the resulting increase in throughput at C fails to compensate for the reduction incurred at R. Consequently, the numerator of the energy efficiency expression diminishes. Examining the vertical axis reveals that higher transmit power Pb corresponds to lower energy efficiency. This inverse relationship stems from the fact that an increase in
Pb elevates the total system power consumption at a rate exceeding the accompanying growth in throughput.
Figure 5 depicts the corresponding variations in overall system throughput and its constituent components as the position of relay node R is dynamically altered. Within the defined scenario, the S and C nodes are fixed at coordinates (-10, 0) and (10, 0), respectively. The relay node R traverses a horizontal line segment from (-20, 5) to (20, 5), with the abscissa representing R's x-coordinate during this movement.
Examination of the figure data reveals that in the inactive state (R not awakened), the R-C link experiences a communication outage. Consequently, the signal received at node C originates exclusively from the transmit power of node S. Given the fixed positions of S and C, the S-C throughput remains constant irrespective of variations in R's position. Conversely, in the active state (R awakened), the throughput at node C comprises contributions from both the direct S-C link transmission and the data relayed via the reflected S-R-C link. However, the signal traversing the S-R-C path undergoes multiplicative path attenuation (experienced sequentially over the S-R and R-C hops), resulting in a negligible contribution to the overall throughput at C. Therefore, even in the active state, the improvement in throughput at C compared to the inactive state is marginal.
As relay node R progressively approaches source node S, corresponding to a reduction in the S-R line-of-sight distance, the throughput of the awakened system, the total system, and awakened node R itself all exhibit a significant upward trajectory. This trend culminates when R reaches the position (-10, 5), where the S-R distance is minimized. At this location, the throughput of each aforementioned component achieves its corresponding peak. This phenomenon is attributed to the shorter transmission distance, which mitigates signal attenuation and path loss during propagation, thereby enhancing data transmission rates and throughput. Furthermore, the substantially lower throughput contribution observed at destination C compared to relay R during the active state results in the throughput curve of the awakened system exhibiting approximate symmetry with respect to x = -10. Concurrently, the throughput curve for awakened node R displays perfect symmetry about x = -10. Conversely, as the S-R distance increases, signal attenuation intensifies. This leads to a progressive diminishment in the throughput contributed by node R, consequently causing the throughput of the awakened system to decline correspondingly.
Figure 6 depicts the relationship between system outage probability and S-R distance across varying wake-up ratios. For any fixed wake-up ratio, the outage probability exhibits a persistent upward trend as the S-R distance increases. When the distance is below 20 meters, the outage probability grows rapidly. Subsequently, the rate of increase gradually attenuates, stabilizing near 0.72 when the distance reaches 25 meters and beyond. This behavior is explained by the robustness of communication links at shorter distances, resulting in lower outage probability. As distance increases, signal transmission becomes more susceptible to impairments such as fading and interference, degrading communication quality and significantly elevating outage probability. Beyond a critical distance, the outage probability asymptotically approaches stability. Examining vertically (across ratios at fixed distances), at
= 1, the outage probabilities for the specific ratios (
and
) are virtually identical. As the value of
decreases, the outage probability increases correspondingly. These results demonstrate that both the S-R distance and the tag's wake-up ratio exert significant influences on the system outage probability within this communication scenario.
To investigate the convergence characteristics of the proposed scheme,
Figure 7 presents the energy efficiency variation with alternating optimization iterations after 1000 Monte Carlo experiments. The initial energy efficiency at the first iteration is approximately 17.945. A significant improvement to 17.975 is observed between the first and second iterations. Subsequently, the energy efficiency stabilizes with negligible fluctuations, as evidenced by the near-horizontal trend line beyond the second iteration. This demonstrates the algorithm's rapid convergence and stability, ensuring reliable system operation without excessive iterative oscillations. The optimal energy efficiency is determined to be 17.975, achieved at a corresponding base station transmit power of 52.73 mW.
In the WUS transmission optimization scheme, the DRX mechanism's cycle length influences both WUS transmission frequency and the number of node R wake-up cycles. To examine DRX cycle's impact on energy efficiency optimization,
Figure 8 illustrates energy efficiency variations with respect to base station transmit power and power splitting ratio under different DRX cycles (32 ms, 64 ms, and 96 ms).
Figure 8(a) reveals that as the base station transmit power increases, the energy efficiency curves corresponding to the three DRX cycles all exhibit an initial rise followed by a subsequent decline. Each curve reaches its peak energy efficiency at approximately 50 mW transmit power, which aligns with prior optimization results. Comparative analysis of
curves further demonstrates that for any given transmit power level, longer DRX cycles yield relatively higher energy efficiency. This suggests that in the studied scenario, appropriately extending the DRX cycle can enhance system energy efficiency, while the extent of efficiency degradation with increasing transmit power varies across different DRX cycle lengths.
Figure 8(b) presents the variation in energy efficiency with respect to the power splitting ratio under different DRX cycles. Overall, as the power splitting ratio
increases from 0.2 to 0.9, all three energy efficiency curves display a monotonically decreasing trend, consistent with the theoretical derivation in
Section 3.3. Comparing the curves, it is evident that for any fixed value of the power splitting ratio, longer DRX cycles correspond to higher energy efficiency. Therefore, for services with less stringent real-time data transmission requirements, extending the DRX cycle length can effectively maintain link energy efficiency.