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ASTM D5568-22 establishes a comprehensive, non-resonant waveguide method for measuring the relative complex permittivity and relative magnetic permeability of solid materials at microwave frequencies. It is specifically designed for isotropic, reciprocal materials and leverages rectangular waveguide transmission lines as precise sample holders.
This test method is valid for determining both relative complex permittivity (dielectric constant and loss) and relative magnetic permeability. For non-magnetic materials, the procedure can be utilized for permittivity measurements exclusively. The frequency range of this method spans approximately 100 MHz to over 40 GHz, although the exact limits are governed by the specimen dimensions, rectangular waveguide size, and the operating range of the network analyzer. Being a non-resonant technique, it supports the selection of any number of discrete measurement frequencies. The rectangular waveguide fixture is preferred over coaxial fixtures for samples that have in-plane anisotropy or are challenging to fabricate precisely.
| 🟦 Parameter | 📏 Specification |
|---|---|
| 🎯 Measured Properties | Relative Complex Permittivity (εr) and Relative Magnetic Permeability (μr) |
| ⚡ Frequency Range | ~100 MHz to >40 GHz |
| 📐 Material Type | Isotropic, Reciprocal (Non-gyromagnetic) Solid Materials |
| 🟦 Fixture Type | Rectangular Waveguide (Circular waveguide is also generally applicable) |
A successful measurement under D5568 relies heavily on a precise calibration of the network analyzer. The calibration procedure involves connecting characterized standard devices to the test ports to characterize the measurement system’s systematic errors. These effects are then mathematically removed from the measurements. The calibration also establishes the mathematical reference plane for the measurement test ports. Modern network analyzers have this capability built in, and standard calibration kits can be used to load the required definitions.
| 🟦 Element | 📏 Details from Standard |
|---|---|
| 🎯 Methodology | Non-resonant, transmission line technique using waveguide fixtures |
| ⚡ Critical Setup | Full calibration of network analyzer to remove systematic errors and define measurement reference planes |
| 📌 Specimen Criteria | Size limited by test frequency, intrinsic electromagnetic properties, and core algorithm requirements |
The primary outputs of D5568 are the relative complex permittivity and relative magnetic permeability values. The standard specifically notes that the equations provided assume an e+jωt harmonic time convention. Users must be careful to apply this convention consistently, as it affects the sign of the imaginary components representing material losses. All values are reported in SI units, with inch-pound units provided in parentheses for reference in the standard.
The standard is applicable over a frequency range of approximately 100 MHz to over 40 GHz. The precise limits depend on the waveguide size, specimen dimensions, and the network analyzer’s operational capabilities.
A rectangular waveguide fixture is preferred over a coaxial fixture when the test samples exhibit in-plane anisotropy or are difficult to manufacture with the precise tolerances required for coaxial holders.
D5568 explicitly assumes an e+jωt harmonic time convention for its equations. This is critical for determining the sign of the imaginary part of the permittivity and permeability (the loss terms).
Calibration characterizes the systematic errors of the network analyzer test setup. By connecting known standard devices, these errors are mathematically removed, and a precise reference plane for the waveguide test ports is established, ensuring accurate measurements.