A high-accuracy 10 Hz-1 MHz automatic AC voltage calibration system

1987 ◽  
Vol IM-36 (4) ◽  
pp. 883-887 ◽  
Author(s):  
Nile M. Oldham ◽  
M. E. Parker ◽  
Albert M. Young ◽  
Alan G. Smith
Sensors ◽  
2018 ◽  
Vol 18 (7) ◽  
pp. 2382 ◽  
Author(s):  
Antonio Vidal-Pardo ◽  
Santiago Pindado

In this work, a new and low-cost Arduino-Based Data Acquisition System (ABDAS) for use in an aerodynamics lab is developed. Its design is simple and reliable. The accuracy of the system has been checked by being directly compared with a commercial and high accuracy level hardware from National Instruments. Furthermore, ABDAS has been compared to the accredited calibration system in the IDR/UPM Institute, its measurements during this testing campaign being used to analyzed two different cup anemometer frequency determination procedures: counting pulses and the Fourier transform. The results indicate a more accurate transfer function of the cup anemometers when counting pulses procedure is used.


ACTA IMEKO ◽  
2017 ◽  
Vol 6 (2) ◽  
pp. 70 ◽  
Author(s):  
Eric Carl Benck ◽  
Corey Stambaugh ◽  
Edward Mulhern ◽  
Patrick Abbott ◽  
Zeina Kubarych

<p><span style="font-size: small;">The kilogram is the unit of mass in the International System of units (SI) and has been defined as the mass of the International Prototype Kilogram (IPK) since 1889.  </span><span style="font-size: small;">In the future, a new definition of the kilogram will be realized by fixing the value of the Planck constant.</span><span style="font-size: small;">  </span><span style="font-size: small;">The new definition of the unit of mass will occur in a vacuum environment by necessity, so the National Institute of Standards and Technology (NIST) is developing a mass calibration system in which a kilogram artefact in air can be directly compared with a kilogram realized in a vacuum environment.</span><span style="font-size: small;">  </span><span style="font-size: small;">This apparatus uses magnetic suspension to couple the kilogram in air to a high accuracy mass balance in vacuum.</span><span style="font-size: small;"> </span></p><p> </p>


2014 ◽  
Vol 36 (6) ◽  
pp. 734-742 ◽  
Author(s):  
Zhenhua Li ◽  
Hongbin Li ◽  
Zhi Zhang ◽  
Pandian Luo ◽  
Hongfeng Li ◽  
...  

ACTA IMEKO ◽  
2015 ◽  
Vol 4 (2) ◽  
pp. 52 ◽  
Author(s):  
Christiaan Smith Veldman

The National Metrology Institute of South Africa (NMISA) has implemented a system to measure the transverse sensitivity of vibration transducers. As a mechanical device, the principle sensing axis of an accelerometer is not 100 % perpendicular to the mounting axis. This gives rise to the effect that the accelerometer will produce an electrical output even when a mechanical input perpendicular to the principle measurement axis is applied. The quantification of this "defect" parameter is of importance when high accuracy acceleration measurements are performed using accelerometers. This paper gives a brief overview of the system developed by the NMISA to measure the transverse sensitivity of vibration transducers. The paper then explores the validation of the system along with the uncertainty of measurement associated with the calibration system.


1991 ◽  
Vol 81 (4) ◽  
pp. 1360-1372
Author(s):  
P. Bernard ◽  
J.-F. Karczewski ◽  
M. Morand ◽  
B. Dole ◽  
B. Romanowicz

Abstract The sensitivity of the Streckeisen's very broadband (VBB) accelerometers is routinely measured on tilt tables by the manufacturer, with an announced accuracy of about 1 per cent. Nevertheless, the transportation of the station or different in situ environmental conditions may modify the sensitivity. As one may expect that a high accuracy in the wave amplitude will be required in the future by seismologists, we developed and tested an in situ absolute calibration method, which does not require the seismometers to be moved. Its principle is simple: A mass is moving in the vicinity of the force-balance accelerometer, and the perturbation of the gravitational field is measured. This calibration method, because it requires the use of G, the gravitational constant, is termed the G-calibration. At a distance of 0.5 m, the gravitational field of a 30 kg mass is 8 × 10−9 m.sec−2, which is 2 order of magnitude greater than the instrumental noise. At the test station of SBB, this acceleration is still 50 times above the seismic noise level for the vertical component, but little above the seismic horizontal noise. The calibration system consists into a small telescope platform (diameter 0.5 m) supporting a horizontal bar of 1 m. Two metallic cylinders of equal mass (about 30 kg) are placed at the two ends of the bar, symmetrically with respect to the vertical rotation axis of the platform. The rotation velocity of the system is controlled with a high accuracy. The accelerometers are located at less than 1 m from the system axis. For the vertical component, we measured the sensitivity at various periods between 2000 and 50 sec, and the result was within 10 per cent of the specified sensitivity; this difference was of the same order as the expected accuracy. For the horizontal component, a slight asymmetry of the two masses with respect to the rotation center and an irregular coupling of the platform to the ground induced a periodic variation of the tilt, dominating over the gravitational signal of the masses at the frequencies of interest, which made the sensitivity measurement less accurate. Nevertheless, the result was still close to the announced sensitivity. We expect that an improved version of our calibration system will allow an accuracy of 1 per cent for the vertical, with a few hours of calibration. This will require an accuracy of a few millimeters in the geometry of the calibration system. Improving the results for the horizontal component will require a careful installation in order to eliminate the tilt perturbation and should lead to an accuracy of a few per cent.


1993 ◽  
Vol 5 (5) ◽  
pp. 448-452 ◽  
Author(s):  
Tadashi Masuda ◽  
◽  
Makoto Kajitani ◽  

This paper describes an automatic calibration system for various angular encoders with high resolution and high accuracy. The system has a photoelectric encoder as a reference standard with 225000 P/R, and object encoders are compared with the reference standard. Using the time conversion method, the relative angle position errors are detected with 0.001"" resolution, and all graduations are automatically measured. The reference standard is automatically calibrated by the self-checking method used the other encoder. As the calibration results, the calibration values of the reference standard were obtained with an accuracy of approximately ±0.5 arc second, and the accuracy of the calibration values were presumed to be approximately 0.05 arc seconds.


MAPAN ◽  
2016 ◽  
Vol 31 (2) ◽  
pp. 119-127 ◽  
Author(s):  
Zhen-hua Li ◽  
Su-hong Yan ◽  
Wei-zhong Hu ◽  
Zhen-xing Li ◽  
Yan-chun Xu

Robotica ◽  
2011 ◽  
Vol 29 (1) ◽  
pp. 23-34 ◽  
Author(s):  
Mahmoud Tavakoli ◽  
Lino Marques ◽  
Aníbal T. de Almeida

SUMMARYHigh accuracy is usually difficult to obtain with a robotic arm installed on a mobile base, since the errors of the base are transferred to the manipulator. This paper proposes a method to address this problem through integration of a self-calibration algorithm and low-cost sensors. The self-calibration algorithm might be repeated several times during execution of a mission by the robot and is only based on the internal sensors of the robot, meaning that external observers or reference point transceivers (e.g., ultrasonic transceivers) are not used. The proposed self-calibration system was implemented on a pole climbing robot and effectively improved the positioning accuracy of the climbing arm.


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