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Wireless Power Transfer (WPT) technology has moved rapidly from laboratory concepts to mainstream commercial deployment, powering everything from smartphones and wearable devices to electric vehicles and industrial equipment. As WPT systems proliferate, concerns about human exposure to electromagnetic fields (EMF) have intensified. IEC PAS 63151 addresses this critical need by establishing a standardized measurement methodology for determining the electromagnetic field strength produced by WPT systems. This Publicly Available Specification (PAS) provides the technical community with a consensus approach to EMF characterization before the development of a full international standard.
The fundamental challenge in measuring WPT EMF is the combination of near-field effects, high power densities, and the presence of both magnetic (H-field) and electric (E-field) components. Unlike far-field RF measurements, where plane-wave assumptions simplify calculations, WPT systems operate in the reactive near-field region where the field distribution is highly non-uniform and strongly dependent on coil geometry, alignment, and load conditions. The PAS specifies measurement probes, positioning systems, and data processing methods specifically designed to handle these near-field conditions.
| Parameter | Specification | Notes |
|---|---|---|
| Frequency range | 1 kHz – 10 MHz | Covers inductive (10–150 kHz) and resonant (100 kHz–MHz) WPT |
| Field types measured | H-field (A/m) and E-field (V/m) | Both components required for compliance assessment |
| Measurement distance | 0 cm (contact) to 50 cm from device surface | Multiple distances to characterize decay characteristics |
| Probe type | Isotropic E/H field probes | Tri-axial design for orientation-independent measurement |
| Maximum uncertainty | ± 3 dB (k=2) | 95% confidence level for compliance decisions |
The PAS defines a rigorous measurement setup that minimizes environmental interference while ensuring reproducibility. The WPT device under test (DUT) is placed on a non-conductive, low-permittivity support structure (typically Rohacell or dry wood) at least 1 meter from any large metallic objects. The measurement probe is mounted on a computer-controlled positioning system capable of 3-axis movement with 1 mm positional accuracy. A key innovation in the standard is the virtual grid scanning method: the probe traverses a predefined 3D grid around the DUT, recording field strength at each point, and the data is interpolated to generate a complete field distribution map.
The positioning protocol defines a reference coordinate system centered on the geometric center of the WPT charging surface. Measurements are taken along three orthogonal axes (X, Y, Z) at intervals of 5 mm or less in regions where the field gradient is steep (within 5 cm of the surface), expanding to 10 mm intervals at greater distances. For each measurement point, both the RMS field strength and the peak field strength are recorded, with a minimum averaging time of 6 seconds to capture any modulation effects from the power control loop.
| Region | Distance from Surface | Grid Spacing | Measurement Points | Purpose |
|---|---|---|---|---|
| Near-field (high gradient) | 0 – 5 cm | 5 mm | ~3000 | Capture peak field regions |
| Transition region | 5 – 20 cm | 10 mm | ~1500 | Characterize field decay |
| Far-field (low gradient) | 20 – 50 cm | 20 mm | ~500 | Verify compliance boundaries |
Once the raw field measurements are collected, IEC PAS 63151 specifies a data processing pipeline that includes background field subtraction, probe factor application, spatial averaging over the human body cross-section (for comparison with ICNIRP exposure limits), and uncertainty analysis. The spatial averaging algorithm is particularly important because exposure limits (such as ICNIRP 2020 and IEEE C95.1) specify averaging over a 200 cm² surface area representing the human torso or head. The PAS provides a reference implementation of the averaging algorithm using a sliding 200 cm² window applied to the interpolated field grid.
From an engineering design perspective, the PAS offers valuable insights for WPT system developers. The measurement data can be used to validate electromagnetic simulation models, optimize coil shielding designs, and determine the minimum safe separation distance between the WPT charger and human body. The standard specifically notes that ferrite shielding on the back side of WPT coils can reduce stray magnetic fields by 15–25 dB, but the effectiveness is highly dependent on ferrite material composition (Mn-Zn ferrites with permeability >2000 at operating frequency are recommended).