| 000 | 04254nlm0a2200421 4500 | ||
|---|---|---|---|
| 001 | 657631 | ||
| 005 | 20231030041519.0 | ||
| 035 | _a(RuTPU)RU\TPU\network\24216 | ||
| 090 | _a657631 | ||
| 100 | _a20180228a2017 k y0engy50 ba | ||
| 101 | 0 | _aeng | |
| 102 | _aGB | ||
| 105 | _ay z 100zy | ||
| 135 | _adrcn ---uucaa | ||
| 181 | 0 | _ai | |
| 182 | 0 | _ab | |
| 200 | 1 |
_aThe stabilization system of primary oscillation for a micromechanical gyroscope _fP. F. Baranov [et al.] |
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| 203 |
_aText _celectronic |
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| 300 | _aTitle screen | ||
| 320 | _a[References: 19 tit.] | ||
| 330 | _aThe mode of primary oscillations of a micromechanical gyroscope (MMG) sensor is provided by an electrostatic comb-drive actuator in which the interaction between the micromechanical structures and electronics occurs by means of a single or differential capacitive sensor. Two pairs of capacitive sensors are traditionally used for frequency stabilization of MMG primary oscillations. The first pair of capacitive sensors excites primary oscillations, while the second measures the amplitude of primary oscillations. The stabilization system provides a continuous frequency tuning of primary oscillations that increases the duration of transition processes, the time of operational readiness, and the instability of the output signal from the secondary oscillation channel of the MMGs. This paper presents a new approach to the primary oscillation control system of the two-component MMG. The method of calculating the natural resonant frequency is based on measurements of the total current passing through the comb-driver actuator capacitances, and a lock-in detection is suggested. This paper consists of the results of the numerical analysis, the description of the proposed approach to the frequency control of the primary MMG oscillations, and the Simulink model of the behaviour of the MMG stabilization system, depending on its mechanical-and-physical properties with regard to a 2% shift of the natural resonant frequency. The frequency control of the primary oscillations at 2% frequency detuning is performed within 0.11s. | ||
| 461 | _tMeasurement Science and Technology | ||
| 463 |
_tVol. 28, № 6 : New Perspectives in Measurements, Tools and Techniques for systems _oThe 14th IMEKO TC10 Workshop on Technical Diagnostics, 27-28 June 2016, Milan, Italy _v[064004, 9 p.] _d2017 |
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| 610 | 1 | _aэлектронный ресурс | |
| 610 | 1 | _aтруды учёных ТПУ | |
| 610 | 1 | _aтехническая диагностика | |
| 610 | 1 | _aдатчики | |
| 610 | 1 | _aстабилизаторы | |
| 610 | 1 | _aколебания | |
| 701 | 1 |
_aBaranov _bP. F. _cspecialist in the field of control and measurement equipment _cAssociate Professor of Tomsk Polytechnic University, Candidate of technical sciences _f1987- _gPavel Fedorovich _2stltpush _3(RuTPU)RU\TPU\pers\34618 |
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| 701 | 1 |
_aNesterenko _bT. G. _cspecialist in the field of mechanical engineering _cAssociate Professor of Tomsk Polytechnic University, Candidate of technical sciences _f1946- _gTamara Georgievna _2stltpush _3(RuTPU)RU\TPU\pers\30970 |
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| 701 | 1 |
_aTsimbalist _bE. I. _cspecialist in the field of control and measurement equipment _cAssociate Professor of Tomsk Polytechnic University, Candidate of technical sciences _f1938- _gEdvard Ilyich _2stltpush _3(RuTPU)RU\TPU\pers\34617 |
|
| 701 | 1 |
_aVtorushin _bS. E. _gSergey Evgenjevich |
|
| 712 | 0 | 2 |
_aНациональный исследовательский Томский политехнический университет _bИнженерная школа неразрушающего контроля и безопасности _bОтделение электронной инженерии _h7977 _2stltpush _3(RuTPU)RU\TPU\col\23507 |
| 712 | 0 | 2 |
_aНациональный исследовательский Томский политехнический университет _bИнженерная школа информационных технологий и робототехники _bОтделение автоматизации и робототехники (ОАР) _h7952 _2stltpush _3(RuTPU)RU\TPU\col\23553 |
| 801 | 2 |
_aRU _b63413507 _c20180228 _gRCR |
|
| 856 | 4 | _uhttps://doi.org/10.1088/1361-6501/aa66c6 | |
| 942 | _cCF | ||