Abstract: 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 above 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 above the terrestrial medium. The ACP system can include vertical lossless artificial anisotropic dielectric (VLAAD) elements distributed above 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 above the terrestrial medium. The array of ACP elements can be distributed about a launching structure, which can be excited with an electromagnetic field to facilitate the launch of a Zenneck surface wave.

Abstract: 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 above 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 above the terrestrial medium. The ACP system can include vertical lossless artificial anisotropic dielectric (VLAAD) elements distributed above 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 above the terrestrial medium. The array of ACP elements can be distributed about a launching structure, which can be excited with an electromagnetic field to facilitate the launch of a Zenneck surface wave.

Abstract: 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.

Abstract: 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.

Abstract: The present invention provides a system and method of detecting the presence of a foreign substance, such as ice, in an air-flow path within an operating jet engine by providing one or more electromagnetic sensors that are tuned to receive electromagnetic waves at one or more frequencies generated by the operating jet engine that change upon the presence of the foreign substance. In at least one embodiment, the waves can be transmitted to the electromagnetic sensor through an electromagnetically transparent window in a wall of the jet engine. In at least another embodiment, the electromagnetic sensor can be coupled with a connector that penetrates an operating chamber in the jet engine to measure the electromagnetic parameters of one or more components from within the chamber of the jet engine. In some embodiments, the amount of ice or other foreign substances can be measured or estimated.

Abstract: The present invention provides a system and method of detecting the presence of a foreign substance, such as ice, in an air-flow path within an operating jet engine by providing one or more electromagnetic sensors that are tuned to receive electromagnetic waves at one or more frequencies generated by the operating jet engine that change upon the presence of the foreign substance. In at least one embodiment, the waves can be transmitted to the electromagnetic sensor through an electromagnetically transparent window in a wall of the jet engine. In at least another embodiment, the electromagnetic sensor can be coupled with a connector that penetrates an operating chamber in the jet engine to measure the electromagnetic parameters of one or more components from within the chamber of the jet engine. In some embodiments, the amount of ice or other foreign substances can be measured or estimated.

Abstract: The disclosure provides a sensor and method for the measurement of fluid properties, such as steam energy and steam quality, and/or multiphase and multicomponent fluids and their flow regime profiles in a single instrument, and in some embodiments can include the mass flow rate. The invention can incorporate an orifice function that permits the measurement of fluid energy and a flow profile across at least a portion of the flow path with an electromagnetic sensing method combined with a standard mass flow rate measurement using an orifice differential pressure measurement system.

Abstract: The disclosure provides a sensor and method for the measurement of fluid properties, such as steam energy and steam quality, and/or multiphase and multicomponent fluids and their flow regime profiles in a single instrument, and in some embodiments can include the mass flow rate. The invention can incorporate an orifice function that permits the measurement of fluid energy and a flow profile across at least a portion of the flow path with an electromagnetic sensing method combined with a standard mass flow rate measurement using an orifice differential pressure measurement system.

Abstract: The disclosure provides an electromagnetic (EM) sensor system and method that permits rapid and non-invasive measurement of blood glucose or other biological characteristics that exhibits a unique spectral signature, such as its complex electrical permittivity within the frequency range from near DC to microwave frequencies. Low-level EM signals are coupled through the skin and modified by electrical properties of the sub dermal tissues. These tissues essentially integrate with the sensor circuit as they interact with the transmitted EM energy. The guided-wave signal can be sampled and converted to a digital representation. The digital information can be processed and analyzed to determine the frequency-sensitive permittivity of the tissues and a determination of blood glucose level is made based upon the sensor output. The sensor design and method has wide-ranging applicability to a number of important measurement problems in industry, biology, medicine, and chemistry, among others.

Abstract: The disclosure provides an electromagnetic (EM) sensor system and method that permits rapid and non-invasive measurement of material properties using measurements of the dispersion of EM energy signals over a wide band of frequencies, including second and higher order moments. The EM energy can be a pulse signal, including an ultra-wide band (“UWB”) pulse signal. A plurality of signals can be incrementally projected through the material in a grid. The grid can generally include a series of projections through the material of an object at different angles. The further analysis of the dispersion characteristics of the EM energy signal provides a measure of added features that assist in improved characterization of the material properties. In at least one embodiment, the results of processed pulses through the object can be used to form a two-dimensional or three-dimensional image of the material for the particular property being measured.

Abstract: The disclosure provides an electromagnetic (EM) sensor system and method that permits rapid and non-invasive measurement of blood glucose or other biological characteristics that exhibits a unique spectral signature, such as its complex electrical permittivity within the frequency range from near DC to microwave frequencies. Low-level EM signals are coupled through the skin and modified by electrical properties of the sub dermal tissues. These tissues essentially integrate with the sensor circuit as they interact with the transmitted EM energy. The guided-wave signal can be sampled and converted to a digital representation. The digital information can be processed and analyzed to determine the frequency-sensitive permittivity of the tissues and a determination of blood glucose level is made based upon the sensor output. The sensor design and method has wide-ranging applicability to a number of important measurement problems in industry, biology, medicine, and chemistry, among others.

Abstract: Embodiments cause interaction of an ultra-wide band signal with a substance over a broad range of frequencies simultaneously to obtain a response signal whose distortion is indicative of a composition of the substance.

Abstract: Apparatus and methods of obtaining information concerning a substance (57) is provided by applying pulses (91, 92, 93) of electromagnetic energy to the substance (57) and evaluating the response of the substance to the electromagnetic energy. The pulses (91, 92, 93) generated by a source (51) are of sufficiently short duration to generate a very broad frequency band of energy. The pulsed energy is directed to the substance (57) to be processed and energy pulses (91, 92, 93) passing through the substance (57) are received (56) and analyzed (66) to determine the properties of substance (57).

Abstract: Apparatus and methods of obtaining information concerning a substance (57) is provided by applying pulses (91, 92, 93) of electromagnetic energy to the substance (57) and evaluating the response of the substance to the electromagnetic energy. The pulses (91, 92, 93) generated by a source (51) are of sufficiently short duration to generate a very broad frequency band of energy. The pulsed energy is directed to the substance (57) to be processed and energy pulses (91, 92, 93) passing through the substance (57) are received (56) and analyzed (66) to determine the properties of substance (57).

Abstract: A novel microwave sensor (10, 60, 70, 90, 200, 250, 280) provides low-cost, robust measurement of the electrical properties of fluid substances. The sensor is suitable for use in an industrial vessel or pipe and employs parallel electrical transmission paths (12,14) that differ in electrical or physical length. The electrical length of each transmission path, which may be a two-way path caused by placing a reflective element in each path, is further determined by the electrical properties of the material under test. The frequency (f) of the signal being applied to the sensor is varied in a known manner such that the difference in the electrical lengths (&Dgr;L) of the transmission paths (12, 14) is caused to correspond to an odd integral multiple of a half wavelength. When the frequency is so adjusted and the signals that have traversed the transmission paths are allowed to coherently interfere with one another, then a minimum resultant signal or null is obtained.