Journal articles: 'Wheatstone bridges'

1

Overney, Frédéric, and Blaise Jeanneret. "Impedance bridges: from Wheatstone to Josephson." Metrologia 55, no. 5 (July 27, 2018): S119—S134. http://dx.doi.org/10.1088/1681-7575/aacf6c.

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POIRIER, W., and F. SCHOPFER. "QUANTUM HALL EFFECT AND OHM METROLOGY." International Journal of Modern Physics B 23, no. 12n13 (May 20, 2009): 2779–89. http://dx.doi.org/10.1142/s0217979209062360.

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The quantum Hall effect (QHE) discovery has revolutionized the ohm metrology: the representation of the unit of resistance is now universal and the ohm can be maintained in each national metrology institute with a relative uncertainty of one part in 109. This breakthrough also results from the development of resistance comparison bridges using cryogenic current comparator (CCC). The fundamental properties of the QHE allow the realization of Quantum Hall Array Resistance Standards (QHARS) by combining a large number of single Hall bars connected in series and/or in parallel. These standards can be as accurate as a single Hall bar. More generally, the multiple connection technique allows metrologists to design useful circuits based on quantum Hall resistors like voltage dividers or Wheatstone bridges. The QHE Wheatstone bridge is particularly suitable for comparing quantum standards. By detecting the unbalance current of this bridge with a CCC, new universality tests of the QHE with a target uncertainty less than 1011 can be realized.

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Cahay, M., G. Qian, and R. Kothari. "Current‐voltage characteristics of unbalanced superconducting Wheatstone bridges." Journal of Applied Physics 78, no. 4 (August 15, 1995): 2581–84. http://dx.doi.org/10.1063/1.360117.

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4

Giordano, José Luis. "On the sensitivity, precision and resolution in DC Wheatstone bridges." European Journal of Physics 18, no. 1 (January 1, 1997): 22–27. http://dx.doi.org/10.1088/0143-0807/18/1/006.

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Gosciniak, Jacek, Michael G. Nielsen, Laurent Markey, Alain Dereux, and Sergey I. Bozhevolnyi. "Power monitoring in dielectric-loaded plasmonic waveguides with internal Wheatstone bridges." Optics Express 21, no. 5 (February 25, 2013): 5300. http://dx.doi.org/10.1364/oe.21.005300.

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Kähler, J., A. Stranz, L. Doering, S. Merzsch, N. Heuck, A. Waag, and E. Peiner. "Fabrication, packaging, and characterization of p-SOI Wheatstone bridges for harsh environments." Microsystem Technologies 18, no. 7-8 (December 17, 2011): 869–78. http://dx.doi.org/10.1007/s00542-011-1396-6.

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Castaño, F. J., B. G. Ng, I. A. Colin, D. Morecroft, W. Jung, and C. A. Ross. "Magnetoresistance of submicrometre multilayer Wheatstone bridges as a probe of magnetic reversal mechanism." Journal of Physics D: Applied Physics 41, no. 13 (June 13, 2008): 132005. http://dx.doi.org/10.1088/0022-3727/41/13/132005.

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8

Zhong, Liang, Feifei Li, Yuxin Peng, Qiang Yang, Mingming Zhang, and Jian Wang. "Design and characterization of a T-shaped two-axis force sensor." Sensor Review 39, no. 6 (November 18, 2019): 776–82. http://dx.doi.org/10.1108/sr-01-2019-0013.

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Purpose This paper aims to propose a type of T-shaped two-axis force sensor for measuring the forces in x- and z-axes. The developed sensor has a simple structure and can be effectively assembled into compact devices. Design/methodology/approach A T-shaped plate, with both ends fixed on a base, is used as the substrate of the sensor. Eight strain gauges are placed in the root of the plate or near the sensor head, which can construct two full Wheatstone bridges on the upper and lower surfaces of the plate. When the x- or z-axes forces are applied to the sensor head, different deformation can be generated to the strain gauges. Therefore, the two Wheatstone bridges can be constructed with a different configuration for measuring the forces in x- or z-axes, respectively. Findings A prototype was designed and constructed and experiments were carried out to test the basic performance of the sensor. It has been verified that the developed sensor could measure the x- and z-axes forces independently with a high resolution of 2.5 and 5 mN, respectively. Originality/value Only one thin plate was used in the design, the forces in x- and z-axes could be measured independently and simultaneously, which made the sensor with a simple structure and compact size. Experiments were also verified that there was no crosstalk error occurred in one axis when the force was applied to the other axis.

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Ferreira, Ricardo, Elvira Paz, Paulo P. Freitas, João Ribeiro, José Germano, and Leonel Sousa. "2-Axis Magnetometers Based on Full Wheatstone Bridges Incorporating Magnetic Tunnel Junctions Connected in Series." IEEE Transactions on Magnetics 48, no. 11 (November 2012): 4107–10. http://dx.doi.org/10.1109/tmag.2012.2202381.

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10

Geddes, L. A. "Did Wheatstone build a bridge? (Wheatstone's bridge circuit)." IEEE Engineering in Medicine and Biology Magazine 25, no. 3 (May 2006): 88–90. http://dx.doi.org/10.1109/memb.2006.1636359.

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11

Huang, Z., Wei Zhao, Ning He, and Liang Li. "Structure Optimization Design and Application of a Strain Based Dynamometer." Materials Science Forum 770 (October 2013): 385–90. http://dx.doi.org/10.4028/www.scientific.net/msf.770.385.

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A strain based dynamometer used for the prediction and measurement of three-component cutting forces for milling operations has been designed on the basis of the principle of additional elastic element theory. Meanwhile, four Wheatstone bridges, considerable amplifier and data acquisition software based on LabVIEW are also used to compose a whole system acquiring the cutting force signals. In order to obtain higher natural frequency and magnification, this paper focuses on the calculation and optimization of the dimensions of the special structure, and finally its first natural frequency can be stabilized at more than 14kHz, which are high enough to precisely measure the cutting forces, and the magnification can also achieve up to 15. The dynamic characteristics of the dynamometer are studied theoretically and experimentally, the results show that the developed dynamometer is able to measure the dynamic force component in high-speed cutting.

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12

Zhao, Wang, and Wen. "Fabrication and Characteristics of a SOI Three-Axis Acceleration Sensor Based on MEMS Technology." Micromachines 10, no. 4 (April 9, 2019): 238. http://dx.doi.org/10.3390/mi10040238.

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A silicon-on-insulator (SOI) piezoresistive three-axis acceleration sensor, consisting of four L-shaped beams, two intermediate double beams, two masses, and twelve piezoresistors, was presented in this work. To detect the acceleration vector (ax, ay, and az) along three directions, twelve piezoresistors were designed on four L-shaped beams and two intermediate beams to form three detecting Wheatstone bridges. A sensitive element simulation model was built using ANSYS finite element simulation software to investigate the cross-interference of sensitivity for the proposed sensor. Based on that, the sensor chip was fabricated on a SOI wafer by using microelectromechanical system (MEMS) technology and packaged on a printed circuit board (PCB). At room temperature and VDD = 5.0 V, the sensitivities of the sensor along x-axis, y-axis, and z-axis were 0.255 mV/g, 0.131 mV/g, and 0.404 mV/g, respectively. The experimental results show that the proposed sensor can realize the detection of acceleration along three directions.

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13

Rocha, Álvaro B. da, Eisenhawer de M. Fernandes, Carlos A. C. dos Santos, Júlio M. T. Diniz, and Wanderley F. A. Junior. "Development and Validation of an Autonomous System for Measurement of Sunshine Duration." Sensors 20, no. 16 (August 16, 2020): 4606. http://dx.doi.org/10.3390/s20164606.

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This paper presented an autonomous electronic system for sunshine duration (SD) monitoring based on the contrast method and developed to operate on a horizontal surface. The prototype uses four photoresistors arranged at 90° in a 20 mm diameter circumference separated by a shading structure used to create a shadow pattern on the detection element. Photoresistors are inserted in individual signal conditioning circuits based on the association between Wheatstone bridges and operational amplifiers to provide an analog signal to the microcontroller unit. The determination of SD occurs through the implementation of fuzzy logic with numerical calculation methods to estimate the probability (f) of solar disk obstruction and estimate SD values. The system does not require additional adjustments after installation or use of energy sources for operation due to the use of an internal battery with charge recovery by solar panels. Experimental results of the proposed system were validated with the ones provided by a government meteorology station. Statistical analysis of the results showed a confidence index (c) greater than 90%, with a precision of 94.26%. The proposed system is a feasible low-cost solution to the available commercial systems for the measurement of sunshine duration.

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Wang, Ying, Xiaofeng Zhao, and Dianzhong Wen. "Fabrication and Characteristics of a Three-Axis Accelerometer with Double L-Shaped Beams." Sensors 20, no. 6 (March 24, 2020): 1780. http://dx.doi.org/10.3390/s20061780.

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A three-axis accelerometer with a double L-shaped beams structure was designed and fabricated in this paper, consisting of a supporting body, four double L-shaped beams and intermediate double beams connected to two mass blocks. When applying acceleration to the accelerometer chip, according to the output voltage changes of three Wheatstone bridges constituted by twelve piezoresistors on the roots of the beams, the corresponding acceleration along three axes can be measured based on the elastic force theory and piezoresistive effect. To improve the characteristics of the three-axis accelerometer, we simulated how the width of the intermediate double beams affected the characteristics. Through optimizing the structure size, six chips with different widths of intermediate double beams were fabricated on silicon-on-insulator (SOI) wafers using micro-electromechanical systems (MEMS) technology and were packaged on printed circuit boards (PCB) by using an electrostatic bonding process and inner lead bonding technology. At room temperature and VDD = 5.0 V, the resulting accelerometer with an optimized size (w = 500 μm) realized sensitivities of 0.302 mV/g, 0.235 mV/g and 0.347 mV/g along three axes, with a low cross-axis sensitivity. This result provides a new strategy to further improve the characteristics of the three-axis accelerometer.

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15

Vordos, Nick, Despoina Gkika, and Dimitrios Bandekas. "Wheatstone Bridge and Bioengineering." Journal of Engineering Science and Technology Review 13, no. 5 (2020): 4–6. http://dx.doi.org/10.25103/jestr.135.02.

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Wheatstone bridge is a circuits that has been used in many applications. In these lecture notes, a brief history, the basic circuits and mathematical expressions, a side wide bridge as well as the connection of Wheatstone bridge with biomechanics are presented. A representative application for hand movement and a variation in microfluidics are described.

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16

Greenslade, Thomas B. "Wheatstone's Bridge." Physics Teacher 43, no. 1 (January 2005): 18–20. http://dx.doi.org/10.1119/1.1845984.

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17

Ammann, Christine, Paul Erdös, and Stephen B. Haley. "Superconducting micronets: The Wheatstone bridge." Physical Review B 51, no. 17 (May 1, 1995): 11739–47. http://dx.doi.org/10.1103/physrevb.51.11739.

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18

Ekelof, S. "The genesis of the Wheatstone bridge." Engineering Science & Education Journal 10, no. 1 (February 1, 2001): 37–40. http://dx.doi.org/10.1049/esej:20010106.

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19

Li, Yue, Iñigo Liberal, and Nader Engheta. "Metatronic analogues of the Wheatstone bridge." Journal of the Optical Society of America B 33, no. 2 (February 1, 2016): A72. http://dx.doi.org/10.1364/josab.33.000a72.

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20

Masiulionis, Ričardas. "INVESTIGATION OF ELECTRONIC DEVICES FOR STRAIN MEASUREMENT / ELEKTRONINIŲ ĮTAISŲ TYRIMAS DEFORMACIJOMS MATUOTI." Mokslas - Lietuvos ateitis 3, no. 1 (August 22, 2011): 63–67. http://dx.doi.org/10.3846/mla.2011.013.

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Importance of strain measuring for safety of buildings is shown. The strain monitoring should be one of the buildings security systems. Often used balanced and non-balanced Wheatstone bridge strain measurement methods are analyzed. The Wheatstone bridge method with feedback is improved. A new method based on small resistance changes by the digital balancing currents is presented. Computer and experimental models of measurement are investigated. The received results confirm theoretical assumptions.

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21

Jin, Zhenhu, Muhamad Arif Ihsan Mohd Noor Sam, Mikihiko Oogane, and Yasuo Ando. "Serial MTJ-Based TMR Sensors in Bridge Configuration for Detection of Fractured Steel Bar in Magnetic Flux Leakage Testing." Sensors 21, no. 2 (January 19, 2021): 668. http://dx.doi.org/10.3390/s21020668.

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Thanks to high sensitivity, excellent scalability, and low power consumption, magnetic tunnel junction (MTJ)-based tunnel magnetoresistance (TMR) sensors have been widely implemented in various industrial fields. In nondestructive magnetic flux leakage testing, the magnetic sensor plays a significant role in the detection results. As highly sensitive sensors, integrated MTJs can suppress frequency-dependent noise and thereby decrease detectivity; therefore, serial MTJ-based sensors allow for the design of high-performance sensors to measure variations in magnetic fields. In the present work, we fabricated serial MTJ-based TMR sensors and connected them to a full Wheatstone bridge circuit. Because noise power can be suppressed by using bridge configuration, the TMR sensor with Wheatstone bridge configuration showed low noise spectral density (0.19 μV/Hz0.5) and excellent detectivity (5.29 × 10−8 Oe/Hz0.5) at a frequency of 1 Hz. Furthermore, in magnetic flux leakage testing, compared with one TMR sensor, the Wheatstone bridge TMR sensors provided a higher signal-to-noise ratio for inspection of a steel bar. The one TMR sensor system could provide a high defect signal due to its high sensitivity at low lift-off (4 cm). However, as a result of its excellent detectivity, the full Wheatstone bridge-based TMR sensor detected the defect even at high lift-off (20 cm). This suggests that the developed TMR sensor provides excellent detectivity, detecting weak field changes in magnetic flux leakage testing.

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22

Tanyeri, Melikhan, Mikhil Ranka, Natawan Sittipolkul, and Charles M. Schroeder. "Microfluidic Wheatstone bridge for rapid sample analysis." Lab on a Chip 11, no. 24 (2011): 4181. http://dx.doi.org/10.1039/c1lc20604d.

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23

Greenslade, Thomas B. "A different sort of Wheatstone bridge experiment." Physics Teacher 52, no. 6 (September 2014): 326. http://dx.doi.org/10.1119/1.4893079.

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Lee, Chiun-Peng, Mei-Feng Lai, Hao-Ting Huang, Chi-Wen Lin, and Zung-Hang Wei. "Wheatstone bridge giant-magnetoresistance based cell counter." Biosensors and Bioelectronics 57 (July 2014): 48–53. http://dx.doi.org/10.1016/j.bios.2014.01.028.

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Pang, Yu, Yuxing Li, Xuefeng Wang, Chenjie Qi, Yi Yang, and Tian-Ling Ren. "A contact lens promising for non-invasive continuous intraocular pressure monitoring." RSC Advances 9, no. 9 (2019): 5076–82. http://dx.doi.org/10.1039/c8ra10257k.

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26

KOKLU, Nigmet, Dundar Yener, and Hamdi Sukur KILIC. "Simulation of Wheatstone Bridge for Measurement of Resistances." International Journal of Applied Mathematics, Electronics and Computers 3, no. 1 (March 10, 2015): 78. http://dx.doi.org/10.18100/ijamec.80135.

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27

Morgenshtein, Arkadiy, Liby Sudakov-Boreysha, Uri Dinnar, Claudio G. Jakobson, and Yael Nemirovsky. "Wheatstone-Bridge readout interface for ISFET/REFET applications." Sensors and Actuators B: Chemical 98, no. 1 (March 2004): 18–27. http://dx.doi.org/10.1016/j.snb.2003.07.017.

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28

Pernick, Benjamin J. "Optimum setting of a slide wire Wheatstone Bridge." Physics Teacher 29, no. 1 (January 1991): 35. http://dx.doi.org/10.1119/1.2343199.

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Salmon, Octavio R., Bráulio T. Agostini, and Fernando D. Nobre. "Ising spin glasses on Wheatstone–Bridge hierarchical lattices." Physics Letters A 374, no. 15-16 (April 2010): 1631–35. http://dx.doi.org/10.1016/j.physleta.2010.02.022.

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30

Zhao, Yongtao. "Measuring Fabric Moisture Content with Improved Wheatstone Bridge." Journal of Fiber Bioengineering and Informatics 7, no. 2 (June 2014): 209–22. http://dx.doi.org/10.3993/jfbi06201408.

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31

Wang, X. "CORRECTIONS FOR GAGE FACTOR AND WHEATSTONE BRIDGE NONLINEARITY." Experimental Techniques 21, no. 3 (May 1997): 33–34. http://dx.doi.org/10.1111/j.1747-1567.1997.tb00521.x.

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32

Van Putten, A. F. P. "A constant voltage constant current wheatstone bridge configuration." Sensors and Actuators 13, no. 2 (February 1988): 103–15. http://dx.doi.org/10.1016/0250-6874(88)80033-7.

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33

Bobylev, Y. V., A. I. Gribkov, and R. V. Romanov. "WHEATSTONE BRIDGE: HISTORY, THEORY, APPLICATION, MODELING, AND TRAINING." Physics in School, no. 1 (2021): 44–55. http://dx.doi.org/10.47639/0130-5522_2021_1_44.

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34

Zhang, Yunfan, Bowen Li, Hui Li, Shengnan Shen, Feng Li, Wentao Ni, and Wan Cao. "Investigation of Potting-Adhesive-Induced Thermal Stress in MEMS Pressure Sensor." Sensors 21, no. 6 (March 12, 2021): 2011. http://dx.doi.org/10.3390/s21062011.

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Thermal stress is one of the main sources of micro-electro-mechanical systems (MEMS) devices error. The Wheatstone bridge is the sensing structure of a typical piezoresistive MEMS pressure sensor. In this study, the thermal stress induced by potting adhesive in MEMS pressure sensor was investigated by experiments, calculated by analytics and analyzed by simulations. An experiment system was used to test the sensor at different air pressures and temperatures. The error becomes greater with the decrease in pressure. A set of novel formulas were proposed to calculate the stress–strain on Wheatstone bridge. The error increases with the temperature deviating from 25 °C. A full-scale geometric model was developed, and finite element simulations were performed, to analyze the effect of the stress on MEMS pressure sensor induced by different temperatures and thicknesses of potting adhesive. Simulation results agree well with the experiments, which indicated that there is a 3.48% to 6.50% output error in 0.35 mm potting adhesive at 150 °C. With the thickness of potting adhesive increasing, the variations of output error of the Wheatstone bridge present an N-shaped curve. The output error meets a maximum of 5.30% in the potting adhesive of 0.95 mm and can be reduced to 2.47%, by increasing the potting adhesive to 2.40 mm.

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35

Shao, Zhuang, Zhi Xia He, Ze Peng Wang, and Liang Zhang. "Measurement of Thermal Conductivity of Liquid Based on Transient Double-Hot Wire Technique." Advanced Materials Research 694-697 (May 2013): 1183–86. http://dx.doi.org/10.4028/www.scientific.net/amr.694-697.1183.

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A new experimental apparatus has been developed for measuring the thermal conductivity of liquid by the two transient hot-wire method, which is based on the theory of one-dimensional unsteady heat conduction in infinite medium. The glass tubes, the heating line source and temperature measurement devices are designed in this experiment. As the temperature controller, low-temperature bath provides a constant water bath environment and current calibrator is the power source. Wheatstone bridge is used to test the relation between the temperature changes and resistance. Data acquisition and control unit is data acquisition devices of the Wheatstone bridge. As the temperature coefficient of platinum wire resistance is calibrated. It can be used to measure 32 groups of data from 10°C to 40°C at the every 10°C according to the experimental steps.

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36

Li, Yong-Jiang, Yu-Nong Yang, Hai-Jun Zhang, Chun-Dong Xue, De-Pei Zeng, Tun Cao, and Kai-Rong Qin. "A Microfluidic Micropipette Aspiration Device to Study Single-Cell Mechanics Inspired by the Principle of Wheatstone Bridge." Micromachines 10, no. 2 (February 16, 2019): 131. http://dx.doi.org/10.3390/mi10020131.

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The biomechanical properties of single cells show great potential for early disease diagnosis and effective treatments. In this study, a microfluidic device was developed for quantifying the mechanical properties of a single cell. Micropipette aspiration was integrated into a microfluidic device that mimics a classical Wheatstone bridge circuit. This technique allows us not only to effectively alter the flow direction for single-cell trapping, but also to precisely control the pressure exerted on the aspirated cells, analogous to the feature of the Wheatstone bridge that can precisely control bridge voltage and current. By combining the micropipette aspiration technique into the microfluidic device, we can effectively trap the microparticles and Hela cells as well as measure the deformability of cells. The Young’s modulus of Hela cells was evaluated to be 387 ± 77 Pa, which is consistent with previous micropipette aspiration studies. The simplicity, precision, and usability of our device show good potential for biomechanical trials in clinical diagnosis and cell biology research.

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37

Guo, Xiao Peng. "Wireless Bridge Strain Data Acquisition System." Applied Mechanics and Materials 722 (December 2014): 299–302. http://dx.doi.org/10.4028/www.scientific.net/amm.722.299.

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Bridge health monitoring has become an important means of transportation for bridge management, and the bridge strain is an important health detection index of bridge. In order to simplify the wiring complexity of test site, this paper aims to research a wireless bridge strain acquisition system based on Wheatstone bridge. The instrument can realize accurate acquisition of bridge strain data, then collects and transmits data remotely to the monitoring data processing system of PC through WIFI. This paper will make a detailed introduction of the system through two aspects of hardware and software.

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38

Jiang, Hongchuan, Xiaoyu Tian, Xinwu Deng, Xiaohui Zhao, Luying Zhang, Wanli Zhang, Jianfeng Zhang, and Yifan Huang. "Low Concentration Response Hydrogen Sensors Based on Wheatstone Bridge." Sensors 19, no. 5 (March 4, 2019): 1096. http://dx.doi.org/10.3390/s19051096.

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The PdNi film hydrogen sensors with Wheatstone bridge structure were designed and fabricated with the micro-electro-mechanical system (MEMS) technology. The integrated sensors consisted of four PdNi alloy film resistors. The internal two were shielded with silicon nitride film and used as reference resistors, while the others were used for hydrogen sensing. The PdNi alloy films and SiN films were deposited by magnetron sputtering. The morphology and microstructure of the PdNi films were characterized with X-ray diffraction (XRD). For efficient data acquisition, the output signal was converted from resistance to voltage. Hydrogen (H2) sensing properties of PdNi film hydrogen sensors with Wheatstone bridge structure were investigated under different temperatures (30 °C, 50 °C and 70 °C) and H2 concentrations (from 10 ppm to 0.4%). The hydrogen sensor demonstrated distinct response at different hydrogen concentrations and high repeatability in cycle testing under 0.4% H2 concentration. Towards 10 ppm hydrogen, the PdNi film hydrogen sensor had evident and collectable output voltage of 600 μV.

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39

Kaabi, H., and S. J. Azhari. "AZKA cell, the current-mode alternative of Wheatstone bridge." IEEE Transactions on Circuits and Systems I: Fundamental Theory and Applications 47, no. 9 (2000): 1277–84. http://dx.doi.org/10.1109/81.883322.

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Ami, S., M. Hliwa, and C. Joachim. "Balancing a four-branch single-molecule nanoscale Wheatstone bridge." Nanotechnology 14, no. 2 (January 23, 2003): 283–89. http://dx.doi.org/10.1088/0957-4484/14/2/335.

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41

Ghallab, Y. H., and W. Badawy. "A new topology for a current-mode wheatstone bridge." IEEE Transactions on Circuits and Systems II: Express Briefs 53, no. 1 (January 2006): 18–22. http://dx.doi.org/10.1109/tcsii.2005.854589.

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42

DiBartolomeo, D., and J. H. Klems. "Simple phase‐sensitive detector for Wheatstone bridge resistance measurements." Review of Scientific Instruments 56, no. 5 (May 1985): 755–57. http://dx.doi.org/10.1063/1.1138164.

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Zavornitsyn, R. S., L. I. Naumova, M. A. Milyaev, A. Y. Pavlova, I. K. Maksimova, V. V. Proglyado, and V. V. Ustinov. "Spin valve based sensor elements for full Wheatstone bridge." Journal of Physics: Conference Series 1389 (November 2019): 012157. http://dx.doi.org/10.1088/1742-6596/1389/1/012157.

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44

Kibble, Bryan P., and D. J. Legg. "A generalized wheatstone bridge for comparing 1-Ω resistors." IEEE Transactions on Instrumentation and Measurement IM-34, no. 2 (June 1985): 282–84. http://dx.doi.org/10.1109/tim.1985.4315325.

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45

Ahn, Jun-Hyung, Chang-Sin Park, and Dong-Weon Lee. "Fabrication of a Wheatstone-Bridge Integrated SU-8 Cantilever." Japanese Journal of Applied Physics 49, no. 6 (June 21, 2010): 06GN01. http://dx.doi.org/10.1143/jjap.49.06gn01.

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46

Wu, Guoqiang, Dehui Xu, Bin Xiong, and Yuelin Wang. "Wheatstone bridge piezoresistive sensing for bulk-mode micromechanical resonator." Applied Physics Letters 101, no. 19 (November 5, 2012): 193505. http://dx.doi.org/10.1063/1.4766441.

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47

Tan, X., Y. J. Lv, X. Y. Zhou, Y. G. Wang, X. B. Song, G. D. Gu, P. F. Ji, et al. "AlGaN/GaN pressure sensor with a Wheatstone bridge structure." AIP Advances 8, no. 8 (August 2018): 085202. http://dx.doi.org/10.1063/1.4996257.

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48

Vasudevan, Arun, Soyoun Jung, Taeksoo Ji, and Simon S. Ang. "Quasi-Symmetric Wheatstone Bridge Zinc Oxide Nanorod UV Detectors." IEEE Sensors Journal 14, no. 9 (September 2014): 3310–18. http://dx.doi.org/10.1109/jsen.2014.2328871.

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Feng, Fei, Huihui Zhu, Min Liu, Xudong Wei, Xiaohong Ge, Yuelin Wang, and Xinxin Li. "Uncooled infrared detector based on silicon diode Wheatstone bridge." Microsystem Technologies 23, no. 3 (October 26, 2015): 669–76. http://dx.doi.org/10.1007/s00542-015-2692-3.

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50

Beggs, Edwin J., José Félix Costa, and John V. Tucker. "Physical Oracles: The Turing Machine and the Wheatstone Bridge." Studia Logica 95, no. 1-2 (May 16, 2010): 279–300. http://dx.doi.org/10.1007/s11225-010-9254-6.

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Journal articles on the topic 'Wheatstone bridges'

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