Abstract

Large magnetic field volumes associated with core-less high-frequency inductive power transfer (HF-IPT) systems allow multiple receivers to be powered from one transmitter, but also provide greater probability for foreign objects to couple to the system. Knowledge of the types of objects (legitimate receivers or otherwise) that are coupled to the transmitter is critical. Such knowledge on the transmit side would allow the system to be deactivated in the presence of foreign objects, and to determine the exact state of tuning of the receivers so that it may adjust itself accordingly to optimize system performance. This article introduces a technique to calculate the induced voltage generated by coupled receivers and foreign objects on the transmit coil in real time. Changes in the position or electrical quantities of the receivers, and foreign objects, alter the induced voltage on the transmit coil, and with it the trajectory of the switching waveforms of the inverter driving the transmit coil. From the shape of these waveforms, information on the phase and amplitude of the induced voltage can be extracted, thus enabling the induced voltage on the primary to be estimated with a single, easy to access, voltage measurement, which is easier than estimating the induced voltage from measurements of coil current and total coil voltage. We used a support-vector-machine (SVM) to perform regression analysis on the drain voltage data. The experimental setup uses a 100 W, 13.56 MHz Class EF inverter, and the model was generated from a large number of samples of the drain voltage waveforms operating at different known loads. These were generated from our in-house HF-IPT test load, which uses a Class EF synchronous rectifier. The results allow the induced voltage on the transmit coil to be estimated in real time from the drain voltage waveform alone, with a normalized root mean square error of 1.1% for the real part (reflected resistance) and 1.2% for the imaginary part (reflected reactance). This article is accompanied by a video file demonstrating the experiments.

Highlights

  • D RIVING inductive power transfer (IPT) systems in the megahertz range, and in the first three ISM bands (6.78, 13.56, and 27.12 MHz) exploits the possibility of high Q factors (>500), and high efficiencies to be achieved at low coupling with compact and lightweight air-core coils

  • High-frequency inductive power transfer (HF-IPT) systems tend to be designed with a wireless link comprised of air-core coils, since, as the frequency is increased, lower inductance coils can achieve the designed coil reactance

  • The most recent improvements to the technology are showcased by HF-IPT systems, which achieve over 80% efficiencies [4]–[8] and are retrofitted for applications [9]–[13]

Read more

Summary

INTRODUCTION

D RIVING inductive power transfer (IPT) systems in the megahertz range, and in the first three ISM bands (6.78, 13.56, and 27.12 MHz) exploits the possibility of high Q factors (>500), and high efficiencies to be achieved at low coupling with compact and lightweight air-core coils. Air-core coil systems tend to have an uncontained magnetic flux shaped solely by the geometry of the electric conductor This uncontained magnetic flux feature of HF-IPT systems with air-core coils is attractive for applications in which multiple receivers with different power requirements can be concurrently coupled to a transmitter. This does create a challenge for system operation as the receivers might be tuned slightly differently or, be embedded in equipment which has metallic frames or shields, which changes the link electromagnetic characteristics. This article expands on our previous works [28]–[30] published as IEEE Conference Proceedings

MEASURING THE INDUCED VOLTAGE OF A HF-IPT COIL UNDER TEST
Considerations of Mismatch in Frequency and Harmonic Distortion
Multiple Receivers and Coupled Objects
INVERTER AND THE LOAD RANGE
Challenges of Measuring the Induced Voltage in HF-IPT Coils
Class EF Inverter
Load-Independent Class EF Inverter
Load Range of the Inverter
OBTAINING THE INDUCED VOLTAGE FROM THE DRAIN VOLTAGE WAVEFORMS
Design Methodology
Load Boundaries and the Operating Range for the Experiments
End-to-End Efficiency
Characterization of a Passive Load and a Metallic Object
Findings
CONCLUSION
Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call