Torsion balance-based system for high-precision force measurement in horizontal plane: part II. Static and dynamic improvement

2019 ◽  
Vol 30 (5) ◽  
pp. 055104
Author(s):  
Na Yan ◽  
Suren Vasilyan ◽  
Thomas Fröhlich
1949 ◽  
Vol Original Series, Volume 31 (4) ◽  
pp. 286-307
Author(s):  
A. Green ◽  
W. A. Jennings ◽  
F. Bush

2005 ◽  
Vol 04 (04) ◽  
pp. 689-694
Author(s):  
HSIEN-CHI YEH ◽  
SWEE HOCK YEO ◽  
SHEAU-SHI PAN ◽  
JUN LUO

To increase the accuracy of mechanical characterizations of microstructures and nanomaterials on the molecular- and nano-scale, the measurement standard of microforce ranging from 10-6 N to 10-9 N must be realized for calibrating the testing and measuring instruments. In this paper, a new scheme based on the equal-arm torsion balance is proposed. This precision torsion balance detects accurately the gravitational force between two mass standards, and links the small force measurement to the International System of Units and Newtonian gravitational constant G. Such a balance might serve as a force standard machine operating in the regime below 10-6 N with an accuracy of 0.1%.


1949 ◽  
Vol 31 (4) ◽  
pp. 273-285 ◽  
Author(s):  
Anthony Green ◽  
W. Alan Jennings ◽  
F. Bush

Sensors ◽  
2022 ◽  
Vol 22 (2) ◽  
pp. 641
Author(s):  
Yang Xiao ◽  
Feng Hu ◽  
Yuchen Zhang ◽  
Jiaxing Zheng ◽  
Shiqiao Qin

In this paper, a novel two-axis differential resonant accelerometer based on graphene with transmission beams is presented. This accelerometer can not only reduce the cross sensitivity, but also overcome the influence of gravity, realizing fast and accurate measurement of the direction and magnitude of acceleration on the horizontal plane. The simulation results show that the critical buckling acceleration is 460 g, the linear range is 0–89 g, while the differential sensitivity is 50,919 Hz/g, which is generally higher than that of the resonant accelerometer reported previously. Thus, the accelerometer belongs to the ultra-high sensitivity accelerometer. In addition, increasing the length and tension of graphene can obviously increase the critical linear acceleration and critical buckling acceleration with the decreasing sensitivity of the accelerometer. Additionally, the size change of the force transfer structure can significantly affect the detection performance. As the etching accuracy reaches the order of 100 nm, the critical buckling acceleration can reach up to 5 × 104 g, with a sensitivity of 250 Hz/g. To sum up, a feasible design of a biaxial graphene resonant accelerometer is proposed in this work, which provides a theoretical reference for the fabrication of a graphene accelerometer with high precision and stability.


1949 ◽  
Vol Original Series, Volume 31 (4) ◽  
pp. 308-320
Author(s):  
A. Green ◽  
W. A. Jennings ◽  
F. Bush

1949 ◽  
Vol Original Series, Volume 31 (4) ◽  
pp. 273-285
Author(s):  
A. Green ◽  
W. A. Jennings ◽  
F. Bush

1949 ◽  
Vol 31 (4) ◽  
pp. 308-320
Author(s):  
Anthony Green ◽  
W. Alan Jennings ◽  
F. Bush

Author(s):  
Wladyslaw Koc

The analysis presented in the paper explains computational issues related to the use of a new method of determining the curvature of the track axis – the so-called moving chord method. It indicates the versatility of this method – it may be used both in a horizontal and vertical plane. It also draws attention to its very high precision, as evidenced by the exemplary geometric cases under consideration. The focus here is on the computational foundations of the discussed method regarding the angles of inclination of the moving chord. It was found that for a circular arc in the horizontal plane, the inclination angles of the moving chord depend on the track turning angle, while the difference in inclination angles depends only on the radius of the arc. In the case of a circular arc in the vertical plane, the moving chord inclination angles are much smaller than in the horizontal plane, which is connected with the range of the applied radii of the arcs. As in the horizontal plane, the radius of the vertical curve is the only factor that determines the discrepancy in the inclination angles of the moving chord.


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