Abstract
Rapid technological advances in the domain of Wireless Power Transfer (WPT) pave the way for novel methods for power management in systems of wireless devices and recent research works have already started considering algorithmic solutions for tackling emerging problems. However, those works are limited by the system modeling, and more specifically the one-dimensional abstraction suggested by Friis formula for the power received by one antenna under idealized conditions given another antenna some distance away.
Different to those works, we use a model which arises naturally from fundamental properties of the superposition of energy fields. This model has been shown to be more realistic than other one-dimensional models that have been used in the past and can capture superadditive and cancellation effects. Under this model, we define two new interesting problems for configuring the wireless power transmitters so as to maximize the total power in the system and we prove that the first problem can be solved in polynomial time. We present a distributed solution that runs in pseudopolynomial time and uses various knowledge levels and we provide theoretical performance guarantees. Finally, we design three heuristics for the second problem and evaluate them experimentally.
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Notes
- 1.
The cumulative power for a set of nodes is the aggregate received power by the nodes of a set from all the operational chargers.
- 2.
Given two antennas, the ratio of power available at the input of the receiving antenna, P r , to output power to the transmitting antenna, P t , is given by \(\frac{P_{r}} {P_{t}} = G_{t}G_{r}( \frac{\lambda }{4\pi R})^{2}\) where G t and G r are the antenna gains (with respect to an isotropic radiator) of the transmitting and receiving antennas, respectively, λ is the wavelength, and R is the distance between the antennas.
- 3.
In fact, the exact formula used in [17] for the electric field is \(\mathbf{E}(C,R)\stackrel{\mathrm{def}}{=}\sqrt{\frac{Z_{0 } G_{C } P_{C } } {4\pi d^{2}}} \cdot e^{-j \frac{2\pi } {\lambda } d}\), where Z 0 is a physical constant indicating the wave-impedance of a plane wave in free space, G C is the gain, and P C is the output power of the transmitter. In this chapter, without loss of generality of our algorithmic solutions, we assume that all wireless transmitters and receivers are identical, thus the aforementioned parameters are the same for each charger.
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Katsidimas, I., Nikoletseas, S., Raptis, T.P., Raptopoulos, C. (2018). Efficient Wireless Power Transfer Maximization Algorithms in the Vector Model. In: Jayakody, D., Thompson, J., Chatzinotas, S., Durrani, S. (eds) Wireless Information and Power Transfer: A New Paradigm for Green Communications. Springer, Cham. https://doi.org/10.1007/978-3-319-56669-6_10
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