Sensors are interrogated without physical connection to a power source, microprocessor, data acquisition equipment, or electrical circuitry.
A measurement- acquisition system uses magnetic fields to power sensors and to acquire measurements from sensors. The system alleviates many shortcomings of traditional measurement acquisition systems, which include a finite number of measurement channels, weight penalty associated with wires, use limited to a single type of measurement, wire degradation due to wear or chemical decay, and the logistics needed to add new sensors. Eliminating wiring for acquiring measurements can alleviate potential hazards associated with wires, such as damaged wires becoming ignition sources due to arcing.
The sensors are designed as electrically passive inductive-capacitive or passive inductive-capacitive-resistive circuits that produce magnetic-field responses. One or more electrical parameters (inductance, capacitance, and resistance) of each sensor can be variable and corresponds to a measured physical state of interest. The magnetic-field-response attributes (frequency, amplitude, and bandwidth) of the inductor correspond to the states of physical properties for which each sensor measures.
For each sensor, the measurement acquisition system produces a series of increasing magnetic-field harmonics within a frequency range dedicated to that sensor. For each harmonic, an antenna electrically coupled to an oscillating current (the frequency of which is that of the harmonic) produces an oscillating magnetic field. Faraday induction via the harmonic magnetic fields produces an electromotive force and therefore a current in the sensor. Once electrically active, the sensor produces its own harmonic magnetic field as the inductor stores and releases magnetic energy. The antenna of the measurement- acquisition system is switched from a transmitting to a receiving mode to acquire the magnetic-field response of the sensor. The rectified amplitude of the received response is compared to previous responses to prior transmitted harmonics, to ascertain if the measurement system has detected a response inflection. The “transmit-receive-compare” of sequential harmonics is repeated until the inflection is identified. The harmonic producing the amplitude inflection is the sensor resonant frequency. Resonant frequency and response amplitude are stored and then correlated to calibration data.
Multiple sensors can be interrogated using a single acquisition system. Each sensor must have a dedicated frequency partition of the antenna bandwidth, and the interrogation system must be augmented with a measurement correlation table for each sensor. The method eliminates the need for a data acquisition channel dedicated to each sensor. Any existing inductive or capacitive sensor can also be modified to be interrogated using this method.
The use of magnetic fields for powering sensors and for acquiring the measurements from them eliminates the need for physical connection from the sensors to a power source and data acquisition equipment. Because magnetic fields are used to power the sensors that, in turn, respond with their own magnetic fields, the attributes of which are dependent upon the physical properties being measured, this class of sensors is referred to as magnetic-field response sensors.
Because the functionality of the magnetic- field-response sensors is based upon magnetic fields, the sensors can be used under such conditions as in caustic environments, acids, high temperatures, cryogenic temperatures, high pressures, and radiative environments. Furthermore, the method allows acquiring measurements that were previously unattainable or logistically difficult because there was no practical means of getting power and data-acquisition electrical connections to a sensor. A novel feature of the method is that an individual sensor can be used to measure simultaneously more than one physical state. This is achieved by correlating combinations of different physical states to combinations of different sensor response attributes. Another novel feature of the method is that a sensor can be used to measure a permanent transition of one physical state to another. Once the new physical state has been achieved (e.g., material phase transition), the sensor can simultaneously measure other physical states.