Efficient Multi-Hop Wireless Power Transfer for the Indoor Environment
Janis Eidaks1, Romans Kusnins1, Ruslans Babajans1
1Institute of Microwave Engineering and Electronics, Riga Technical University, Azenes St. 12, LV-1048 Riga, Latvia.
Sensors (Basel, Switzerland)
|September 9, 2023
Summary
This study enhances wireless power transfer (WPT) efficiency for the Internet of Things (IoT) using a multi-hop approach. This method boosts received power at end sensor nodes, improving autonomous device operation.
Area of Science:
- Electrical Engineering
- Wireless Communication Systems
- Sensor Networks
Background:
- The proliferation of Internet of Things (IoT) and wireless sensor networks (WSN) necessitates efficient wireless powering solutions for autonomous devices.
- Existing wireless power transfer (WPT) methods face efficiency challenges, particularly for low-power autonomous systems.
- Advancements in wireless communication technologies offer potential solutions for improving WPT.
Purpose of the Study:
- To investigate the efficacy of a multi-hop (MH) concept for enhancing wireless power transfer (WPT) efficiency.
- To increase the received power at the end sensor node (ESN) in wireless sensor networks (WSN).
- To explore the application of signal amplification techniques within a multi-hop WPT framework.
Main Methods:
- Developed and fabricated a multi-hop node (MHN) prototype for WPT.
- Conducted experimental measurements and power transfer modeling in the sub-GHz frequency range.
- Evaluated WPT performance in both line-of-sight (LoS) and non-line-of-sight (NLoS) scenarios, including a 90-degree turn-on angle for NLoS.
- Proposed an efficient simulation approach for analyzing MH WPT technology and sensor node distribution.
Main Results:
- Demonstrated a functional multi-hop node (MHN) prototype through laboratory experiments.
- Measured received power and RF-DC converted voltage at the end sensor node (ESN) under various conditions.
- Validated the potential of the multi-hop WPT concept to improve power delivery efficiency.
- Showcased the utility of the simulation approach for optimizing wireless sensor node placement.
Conclusions:
- The multi-hop (MH) WPT strategy, leveraging signal amplification, effectively enhances power delivery to end sensor nodes (ESN).
- Experimental validation confirms the feasibility and benefits of MH WPT in both LoS and NLoS environments.
- The proposed simulation method provides a valuable tool for optimizing spatial distribution of wireless sensor nodes for improved WPT efficiency.
Related Concept Videos
Maximum Power Transfer
285
Numerous practical applications within engineering disciplines, such as telecommunications, necessitate optimizing power delivery to a connected load. This pursuit, however, entails inherent internal losses, which can either equal or exceed the power supplied to the load. The Thevenin equivalent circuit is helpful in finding the maximum power a linear circuit can deliver to a load. It is assumed in this context that the load resistance can be adjusted.
By substituting the entire circuit with...
By substituting the entire circuit with...
285
The Maximum Power Transfer Theorem
653
Consider a linear AC Thevenin equivalent circuit connected to a load impedance.
The load connected draws the current, and the circuit delivers the power to the load. The alternating current flowing through the load is determined using the rectangular form of voltages, currents, network impedance, and load impedance. The average power delivered to the load is obtained from the product of the square of current and load resistance.
The load connected draws the current, and the circuit delivers the power to the load. The alternating current flowing through the load is determined using the rectangular form of voltages, currents, network impedance, and load impedance. The average power delivered to the load is obtained from the product of the square of current and load resistance.
653
Energy Stored In A Coaxial Cable
1.5K
A coaxial cable consists of a central copper conductor used for transmitting signals, followed by an insulator shield, a metallic braided mesh that prevents signal interference, and a plastic layer that encases the entire assembly.
In the simplest form, a coaxial cable can be represented by two long hollow concentric cylinders in which the current flows in opposite directions. The magnetic field inside and outside the coaxial cable is determined by using Ampère's law. The magnetic...
In the simplest form, a coaxial cable can be represented by two long hollow concentric cylinders in which the current flows in opposite directions. The magnetic field inside and outside the coaxial cable is determined by using Ampère's law. The magnetic...
1.5K
Induced Electric Fields: Applications
1.7K
An important distinction exists between the electric field induced by a changing magnetic field and the electrostatic field produced by a fixed charge distribution. Specifically, the induced electric field is nonconservative because it does not work in moving a charge over a closed path. In contrast, the electrostatic field is conservative and does no net work over a closed path. Hence, electric potential can be associated with the electrostatic field but not the induced field. The following...
1.7K
Conduction, Convection and Radiation: Problem Solving
1.3K
There are three methods by which heat transfer can take place: conduction, convection, and radiation. Each method has unique and interesting characteristics, but all three have two things in common: they transfer heat solely because of a temperature difference; and the greater the temperature difference, the faster the heat transfer.
In order to solve a problem related to heat transfer, first of all, the situation needs to be examined to determine the type of heat transfer involved. This could...
In order to solve a problem related to heat transfer, first of all, the situation needs to be examined to determine the type of heat transfer involved. This could...
1.3K
Propagation Speed of Electromagnetic Waves
3.4K
Electromagnetic waves are consistent with Ampere's law. Assuming there is no conduction current Ampere's law is given as:
3.4K


