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Published byEvan Taylor Modified over 8 years ago
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Accelerometer approaches Measure F Compression Bending Stress/force based Piezoelectric Piezoresistive Measure x Capacitive (Optical) (Magnetic) AC DC FP Thermal Parallell plate Comb Measure v Inductive
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ADXL150
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Parameter extraction Partitioning and choice of variables (z,v) Find values for the parameters (m,k,γ) Couple Analyze z
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Quasi static sensitivity of a displacement based accelerometer Utbøyning z Mechanical part of the sensitivity
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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
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Mass and mechanical sensitivity Estimate: Analog devices: Mechanical sensitivity: sm=sm=
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Dynamics Partitioning and choice of variables (z,v) Find values for the parameters (m,k,γ) Couple Analyze z
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Position – velocity - acceleration Oscillatory motion Position Velocity Acceleration
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Second order system with forced oscillations x
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Block function F
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Block function from Senturia x/f v/f
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Resonance frequency For zero damping, the response diverges when hence, we introduce the resonance frequency:
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Sensitivity vs. bandwidth
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Q-factor definition
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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)
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Experiment Q,f
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Q from power function FWHM HM f0f0
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Contributions to damping = 7 µN/(m/s) = 5
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Consequence of damping Brownian motion of the accelerometer results in: Force noise: Equivalent acceleration Measured noise:
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Capacitor as a two port element
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Capacitor cofiguration
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Differential read out
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Capacitance Capacitance from parallel plate approximation: Capacitance including fringing fields about 100 fF
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System configuration
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Specifications
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Construction
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