Patent classifications
G01R27/04
Systems for Passive Microwave Remote Sensing and Their Calibration Methods
A system for passive microwave remote sensing using at least one microwave radiometer includes a fixed body portion and a mobile body portion. The mobile body portion is configured for rotatably coupling with the fixed body portion for rotation about a rotation axis. The mobile body portion is configured for supporting the microwave radiometer therein such that the microwave radiometer rotates about the rotation axis when the mobile body portion is rotated about the rotation axis such that a polarization axis of the radiometer is aligned with an earth axis. The fixed body portion includes a motor mechanism for effecting rotation of the mobile body portion. In an embodiment, the mobile body portion includes a plurality of body section, each body section being configured for supporting a microwave radiometer therein. In another embodiment, each one of the plurality of body sections is configured to be interchangeably coupled with each other.
Measurement system and method for matching and/or transmission measurements
A measurement system for matching and/or transmission measurements with respect to a device under test comprising an interface is provided. Said measurement system comprises at least one signal generator comprising at least one signal generator signal path, and at least one receiver comprising at least two receiver signal paths. In this context, a signal of a first signal generator signal path of the at least one signal generator signal path and/or a signal of a first receiver signal path of the at least two receiver signal paths is adaptively phase-shifted and/or amplitude-modified with respect to a signal of a second receiver signal path of the at least two receiver signal paths.
Measurement system and method for matching and/or transmission measurements
A measurement system for matching and/or transmission measurements with respect to a device under test comprising an interface is provided. Said measurement system comprises at least one signal generator comprising at least one signal generator signal path, and at least one receiver comprising at least two receiver signal paths. In this context, a signal of a first signal generator signal path of the at least one signal generator signal path and/or a signal of a first receiver signal path of the at least two receiver signal paths is adaptively phase-shifted and/or amplitude-modified with respect to a signal of a second receiver signal path of the at least two receiver signal paths.
AUTOMATED RESONANT WAVEGUIDE CAVITY SYSTEM FOR COMPLEX PERMITTIVITY MEASUREMENTS
An automated resonant waveguide cavity system for determining one or complex permittivity measurements of a sample is provided. The automated resonant waveguide cavity system includes a resonant cavity, a waveguide coupled to the resonant cavity, a programmable network analyzer (PNA) coupled to the waveguide, and a computing device. The computing device includes a memory storing processor executable code for a determination engine and a processor executing the processor executable code to cause the determination engine to obtain data from the PNA. The data is respective to the sample within the resonant cavity. The determination engine further integrates a plurality of analytical and modeling functions in determining the complex permittivity values of the sample from the data.
Observation circuit for observing an input impedance at a high frequency connector of a mobile device terminal and mobile device terminal comprising such an observation circuit and vehicle comprising the mobile device terminal
The disclosure is directed to an observation circuit for observing an input impedance at a high frequency connector of a mobile device terminal, the observation circuit comprising a measurement circuitry, wherein the measurement circuitry comprises the high frequency connector, a reference impedance, a voltage source, and a voltage meter. A first output electrode of the voltage source is connected to both a first electrode of the high frequency connector and a first input electrode of the voltage meter over the reference impedance, and a second output electrode of the voltage source is connected to both a second electrode of the high frequency connector and a second input electrode of the voltage meter.
Anisotropic constitutive parameters for launching a Zenneck surface wave
Various examples are provided related to anisotropic constitutive parameters (ACPs) that can be used to launch Zenneck surface waves. In one example, among others, an ACP system includes an array of ACP elements distributed over a medium such as, e.g., a terrestrial medium. The array of ACP elements can include one or more horizontal layers of radial resistive artificial anisotropic dielectric (RRAAD) elements positioned in one or more orientations over the terrestrial medium. The ACP system can include vertical lossless artificial anisotropic dielectric (VLAAD) elements distributed over the terrestrial medium in a third orientation perpendicular to the horizontal layer or layers. The ACP system can also include horizontal artificial anisotropic magnetic permeability (HAAMP) elements distributed over the terrestrial medium. The array of ACP elements can be distributed about a launching structure, which can excite the ACP system with an electromagnetic field to launch a Zenneck surface wave.
Anisotropic constitutive parameters for launching a Zenneck surface wave
Various examples are provided related to anisotropic constitutive parameters (ACPs) that can be used to launch Zenneck surface waves. In one example, among others, an ACP system includes an array of ACP elements distributed over a medium such as, e.g., a terrestrial medium. The array of ACP elements can include one or more horizontal layers of radial resistive artificial anisotropic dielectric (RRAAD) elements positioned in one or more orientations over the terrestrial medium. The ACP system can include vertical lossless artificial anisotropic dielectric (VLAAD) elements distributed over the terrestrial medium in a third orientation perpendicular to the horizontal layer or layers. The ACP system can also include horizontal artificial anisotropic magnetic permeability (HAAMP) elements distributed over the terrestrial medium. The array of ACP elements can be distributed about a launching structure, which can excite the ACP system with an electromagnetic field to launch a Zenneck surface wave.
Automated resonant waveguide cavity system for complex permittivity measurements
An automated resonant waveguide cavity system for determining one or complex permittivity measurements of a sample is provided. The automated resonant waveguide cavity system includes a resonant cavity, a waveguide coupled to the resonant cavity, a programmable network analyzer (PNA) coupled to the waveguide, and a computing device. The computing device includes a memory storing processor executable code for a determination engine and a processor executing the processor executable code to cause the determination engine to obtain data from the PNA. The data is respective to the sample within the resonant cavity. The determination engine further integrates a plurality of analytical and modeling functions in determining the complex permittivity values of the sample from the data.
Automated resonant waveguide cavity system for complex permittivity measurements
An automated resonant waveguide cavity system for determining one or complex permittivity measurements of a sample is provided. The automated resonant waveguide cavity system includes a resonant cavity, a waveguide coupled to the resonant cavity, a programmable network analyzer (PNA) coupled to the waveguide, and a computing device. The computing device includes a memory storing processor executable code for a determination engine and a processor executing the processor executable code to cause the determination engine to obtain data from the PNA. The data is respective to the sample within the resonant cavity. The determination engine further integrates a plurality of analytical and modeling functions in determining the complex permittivity values of the sample from the data.
Method of measuring impedance using Gaussian white noise excitation
A method of impedance measurement of a device under test (DUT) is disclosed based on a random excitation signal, the method comprising the steps of generating the random excitation signal, applying the generated random excitation signal to the DUT through two points of a data acquisition board (DAQ) and re-structuring the converted random excitation signal through a plurality of iterative calibration loops, wherein spectral phase of the random excitation signal is derived from a discrete uniform distribution and its time domain amplitude is controllable. The random excitation signal is a structured Gaussian White Noise (GWN) signal or sequence, which is generated based on the user-defined input parameters such as white noise power level, frequency range between the minimum and maximum frequencies (F.sub.min and F.sub.max), and frequency step (F.sub.step).