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Accelerometer approaches

Accelerometer approaches. Piezoelectric. Measure F Compression Bending. Piezoresistive. Stress/force based. Parallell plate. Comb. AC. Capacitive. DC. FP. (Optical). Measure x. Measure v. (Magnetic). Inductive. Thermal. ADXL150. Partitioning and choice of variables (z,v).

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Accelerometer approaches

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  1. Accelerometer approaches Piezoelectric • Measure F • Compression • Bending Piezoresistive Stress/force based Parallell plate Comb AC Capacitive DC FP (Optical) Measure x Measure v (Magnetic) Inductive Thermal

  2. ADXL150

  3. Partitioning and choice of variables (z,v) Find values for the parameters (m,k,γ) Couple Analyze Parameter extraction z

  4. Utbøyning Quasi static sensitivity of a displacement based accelerometer Mechanical part of the sensitivity z

  5. Doubly clamped beam with point load at midpoint • Spring constant: • z-central beam displacement • W beam width (poly thickness) • H beam thickness (lithography) • Stiffness of folded spring: 2.8 N/m • Stiffness of two springs: 5.6 N/m • Spring softening due to applied voltage gives: 5.2 N/m

  6. Mass and mechanical sensitivity Estimate: Analog devices: Mechanical sensitivity: sm=

  7. Partitioning and choice of variables (z,v) Find values for the parameters (m,k,γ) Couple Analyze Dynamics z

  8. Position – velocity - acceleration Oscillatory motion • Position • Velocity • Acceleration

  9. x Second order system with forced oscillations

  10. Block function F

  11. Block function from Senturia x/f v/f

  12. Resonance frequency For zero damping, the response diverges when hence, we introduce the resonance frequency:

  13. Sensitivity vs. bandwidth

  14. Q-factor definition

  15. Q-factor appears as • Stored energy divided by energy dissipated during one cycle at resonance • Number of oscillations before the amplitude is reduced by a factor 1/e • Eigenfrequency divided by the Full Width at Half Maximum for the transfer function squared (power)

  16. Experiment Q,f

  17. Q from power function FWHM HM f0

  18. Contributions to damping = 5 = 7 µN/(m/s)

  19. Consequence of damping Brownian motion of the accelerometer results in: Force noise: Equivalent acceleration Measured noise:

  20. Capacitor as a two port element

  21. Capacitor cofiguration

  22. Differential read out

  23. Capacitance Capacitance from parallel plate approximation: • Capacitance including fringing fields about 100 fF

  24. System configuration

  25. Specifications

  26. Construction

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