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Development of metallic digital strain gauges

机译:金属数字应变仪的开发

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摘要

Metallic resistive strain gauges are widely used in measuring devices for physical quantities such as load, pressure and torque. The gauges are bonded to the surface of the sensing structure at strategic points to obtain an appropriate level of strain. Typically in a load cell the strains at the gauges do not exceed 1500 micros-train at the rated load. With a four-gauge fully active Wheatstone bridge circuit, a nominal output signal is about 3 mV/V of bridge excitation for the maximum level of 1500 microstrain at the full load, based upon a gauge factor of 2. If the bridge excitation voltage is 10 V, which is determined by the gauge resistance, the gauge grid area and the heat-sink characteristics of the load cell material, the maximum output voltage of the bridge at the full load will be about 30 mV. Despite many favourable factors of the metallic resistive strain gauges, the limiting factors are that the output signals are quite low and very often the measurement accuracy is limited by the signal-to-noise ratio. Also the installation of strain gauges is normally labour intensive. Furthermore, to obtain a measurable output signal, the surface strain is usually designed to approach the proportional elastic limit of the sensing structure. For this reason strain-gauges-based load cells can seldom withstand overloads of more than double the rated full range load. Strain gauges have for many years been the primary sensors in the fields of measurement for load, pressure and torque. However, some instrument manufacturers of load, pressure and torque measurement devices have moved away from using resistive strain gauges. Since early 1980's, Shinko Denshi Co. Ltd. has developed metallic resonant tuning fork balance and since early 1990's, Avery Berkel and Weigh-Tronix (now Avery Weigh-Tronix) have developed quartz resonant tuning fork weighing scales, and Druck Ltd has developed silicon resonant pressure sensors. Further commercial developments are taking place to enhance device manufacturability, to enable wireless/batteryless operation of the resonant sensors, and to make measurement on stiff structures at much lower strain levels possible.
机译:金属电阻应变仪广泛用于测量诸如负载,压力和扭矩等物理量的设备。量规在关键点结合到传感结构的表面以获得适当的应变水平。通常,在称重传感器中,在额定载荷下,应变片的应变不超过1500微应变。对于四轨全有源惠斯通电桥电路,在满载条件下,基于规格系数2,最大输出电平为1500微应变时,标称输出信号约为3 mV / V的桥激励。 10 V是由标称电阻,标称栅格面积和称重传感器材料的散热特性决定的,满载时电桥的最大输出电压约为30 mV。尽管金属电阻应变仪有许多有利因素,但限制因素是输出信号非常低,并且测量精度经常受信噪比限制。而且,应变仪的安装通常是劳动密集型的。此外,为了获得可测量的输出信号,通常将表面应变设计为接近传感结构的比例弹性极限。因此,基于应变仪的称重传感器很少能承受超过额定全范围载荷两倍以上的过载。多年来,应变仪一直是负载,压力和扭矩测量领域的主要传感器。但是,一些负载,压力和扭矩测量设备的仪器制造商已不再使用电阻应变仪。从1980年代初期开始,Shinko Denshi Co. Ltd.开发了金属共振音叉天平,从1990年代初期开始,Avery Berkel和Weigh-Tronix(现为Avery Weigh-Tronix)开发了石英共振音叉秤,而Druck Ltd开发了硅。共振压力传感器。正在进行进一步的商业开发,以增强设备的可制造性,以使谐振传感器能够进行无线/无电池操作,并能够以低得多的应变水平对刚性结构进行测量。

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