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поискавой системы для электроныых деталей |
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поискавой системы для электроныых деталей |
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ISM330BX датащи(PDF) 13 Page - STMicroelectronics |
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ISM330BX датащи(HTML) 13 Page - STMicroelectronics |
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13 / 150 page  Symbol Parameter Test conditions Min.(1) Typ.(2) Max.(1) Unit RMS Accelerometer RMS noise in low-power mode(10) LPM2 mg RMS 2.1 LPM3 1.4 LA_ODR Linear acceleration output data rate 1.875(11) 7.5 15 30 60 120 240 480 960 1.92 k 3.84 k Hz G_ODR Angular rate output data rate 7.5 15 30 60 120 240 480 960 1.92 k 3.84 k LA_F0 Accelerometer resonant frequency X,Y-axis 2.8 kHz Z-axis 2.2 LA_BW Signal bandwidth SPI/I²C/I3C interface ±3 dB point High-performance mode 1.8 kHz TDM interface ±3 dB point 1 Vst Linear acceleration self-test output change(12)(13) 20 1700 mg Angular rate self-test output change(14) FS = ±250 dps 20 80 dps FS = ±2000 dps 150 700 dps Top Operating temperature range -40 +85 °C 1. Min/Max values are based on characterization results at 3σ on a limited number of samples, not tested in production and not guaranteed. 2. Typical specifications are not guaranteed. 3. Sensitivity values after factory calibration test and trimming. 4. Value after calibration. 5. Measurements are performed in a uniform temperature setup and they are based on characterization data in a limited number of samples. Not measured during final test for production. 6. Gyroscope rate noise density in high-performance mode is independent of the ODR and FS setting. Gyroscope noise density is computed starting from measured noise RMS and considering BW = ODR/2. 7. Gyroscope RMS noise in low-power mode is independent of the ODR and FS setting. 8. Accelerometer noise density in high-performance mode is independent of the selected ODR and FS. Accelerometer noise density is computed starting from measured noise RMS and considering BW = ODR/2. 9. Noise density is between 10 Hz and 1 kHz. ISM330BX Module specifications DS14588 - Rev 2 page 13/150 |
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