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Dimensionless frequency offset values can be converted to units of frequency Hz if the nominal frequency is known.. To illustrate this, consider an oscillator with a nominal frequency of

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Dimensionless frequency offset values can be converted to units of frequency (Hz) if the nominal frequency is known To illustrate this, consider an oscillator with a nominal frequency of 5 MHz and a frequency offset of +1.16 × 10-11 To find the frequency offset in hertz, multiply the nominal frequency

by the offset:

(5 × 106) (+1.16 × 10-11)=5.80 × 10-5=+0.0000580 Hz Then, add the offset to the nominal frequency to get the actual frequency:

5,000,000 Hz + 0.0000580 Hz = 5,000,000.0000580 Hz

Stability

Stability indicates how well an oscillator can produce the same time or frequency offset over a given time

interval It doesn’t indicate whether the time or frequency is “right” or “wrong,” but only whether it stays the same In contrast, accuracy indicates how well an oscillator has been set on time or on frequency To

understand this difference, consider that a stable oscillator that needs adjustment might produce a frequency with a large offset Or, an unstable oscillator that was just adjusted might temporarily produce

a frequency near its nominal value Figure 17.7 shows the relationship between accuracy and stability

Stability is defined as the statistical estimate of the frequency or time fluctuations of a signal over a given time interval These fluctuations are measured with respect to a mean frequency or time offset

Short-term stability usually refers to fluctuations over intervals less than 100 s Long-term stability can

refer to measurement intervals greater than 100 s, but usually refers to periods longer than 1 day

Stability estimates can be made in either the frequency domain or time domain, and can be calculated from a set of either frequency offset or time interval measurements In some fields of measurement, stability is estimated by taking the standard deviation of the data set However, standard deviation only

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Dimensionless frequency offset values can be converted to units of frequency (Hz) if the nominal frequency is known To illustrate this, consider an oscillator with a nominal frequency of 5 MHz and a frequency offset of +1.16 × 10-11 To find the frequency offset in hertz, multiply the nominal frequency

by the offset:

(5 × 106) (+1.16 × 10-11)=5.80 × 10-5=+0.0000580 Hz Then, add the offset to the nominal frequency to get the actual frequency:

5,000,000 Hz + 0.0000580 Hz = 5,000,000.0000580 Hz

Stability

Stability indicates how well an oscillator can produce the same time or frequency offset over a given time

interval It doesn’t indicate whether the time or frequency is “right” or “wrong,” but only whether it stays the same In contrast, accuracy indicates how well an oscillator has been set on time or on frequency To

understand this difference, consider that a stable oscillator that needs adjustment might produce a frequency with a large offset Or, an unstable oscillator that was just adjusted might temporarily produce

a frequency near its nominal value Figure 17.7 shows the relationship between accuracy and stability

Stability is defined as the statistical estimate of the frequency or time fluctuations of a signal over a given time interval These fluctuations are measured with respect to a mean frequency or time offset

Short-term stability usually refers to fluctuations over intervals less than 100 s Long-term stability can

refer to measurement intervals greater than 100 s, but usually refers to periods longer than 1 day

Stability estimates can be made in either the frequency domain or time domain, and can be calculated from a set of either frequency offset or time interval measurements In some fields of measurement, stability is estimated by taking the standard deviation of the data set However, standard deviation only

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Sensor and Actuator

Characteristics

18.1 Range

18.2 Resolution

18.3 Sensitivity

18.4 Error

18.5 Repeatability

18.6 Linearity and Accuracy

18.7 Impedance

18.8 Nonlinearities

18.9 Static and Coulomb Friction

18.10 Eccentricity

18.11 Backlash

18.12 Saturation

18.13 Deadband

18.14 System Response

18.15 First-Order System Response

18.16 Underdamped Second-Order System Response

18.17 Frequency Response

Mechatronic systems use a variety of sensors and actuators to measure and manipulate mechanical, electrical, and thermal systems Sensors have many characteristics that affect their measurement capa-bilities and their suitability for each application Analog sensors have an output that is continuous over

a finite region of inputs Examples of analog sensors include potentiometers, LVDTs (linear variable differential transformers), load cells, and thermistors Digital sensors have a fixed or countable number

of different output values A common digital sensor often found in mechatronic systems is the incremental encoder An analog sensor output conditioned by an analog-to-digital converter (ADC) has the same digital output characteristics, as seen in Fig 18.1

18.1 Range

The range (or span) of a sensor is the difference between the minimum (or most negative) and maximum inputs that will give a valid output Range is typically specified by the manufacturer of the sensor For example, a common type K thermocouple has a range of 800∞C (from -50∞C to 750∞C) A ten-turn potentiometer would have a range of 3600degrees

Joey Parker

University of Alabama

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Sensors

19.1 Linear and Rotational Sensors

Contact • Infrared • Resistive • Tilt (Gravity) • Capacitive • AC Inductive • DC Magnetic • Ultrasonic • Magnetostrictive Time-of-Flight • Laser Interferometry 19.2 Acceleration Sensors

Overview of Accelerometer Types • Dynamics and Characteristics of Accelerometers • Vibrations • Typical Error Sources and Error Modeling • Inertial

Accelerometers • Electromechanical Accelerometers • Piezoelectric Accelerometers • Piezoresistive Accelerometers • Strain-Gauge Accelerometers • Electrostatic Accelerometers • Micro- and Nanoaccelerometers • Signal Conditioning and Biasing 19.3 Force Measurement

General Considerations • Hooke’s Law • Force Sensors 19.4 Torque and Power Measurement

Fundamental Concepts • Arrangements of Apparatus for Torque and Power Measurement • Torque Transducer Technologies • Torque Transducer Construction, Operation, and Application • Apparatus for Power Measurement 19.5 Flow Measurement

Introduction • Terminology • Flow Characteristics • Flowmeter Classification • Differential Pressure Flowmeter • The Variable Area Flowmeter • The Positive Displacement Flowmeter • The Turbine Flowmeter • The Vortex Shedding Flowmeter • The Electromagnetic Flowmeter • The Ultrasonic Flowmeter • The Coriolis Flowmeter • Two-Phase Flow • Flowmeter

Installation • Flowmeter Selection 19.6 Temperature Measurements

Introduction • Thermometers That Rely Upon Differential Expansion Coefficients • Thermometers That Rely Upon Phase Changes • Electrical Temperature Sensors and Transducers • Noncontact Thermometers • Microscale Temperature Measurements • Closing Comments 19.7 Distance Measuring and Proximity Sensors

Distance Measuring Sensors • Proximity Sensors 19.8 Light Detection, Image, and Vision Systems

Introduction • Basic Radiometry • Light Sources • Light Detectors • Image Formation • Image Sensors • Vision Systems

19.9 Integrated Microsensors

Introduction • Examples of Micro- and Nanosensors • Future Development Trends • Conclusions

Kevin M Lynch

Northwestern University

Michael A Peshkin

Northwestern University

Halit Eren

Curtin University of Technology

M A Elbestawi

McMaster University

Ivan J Garshelis

Magnova, Inc.

Richard Thorn

University of Derby

Pamela M Norris

University of Virginia

Bouvard Hosticka

University of Virginia

Jorge Fernando Figueroa

NASA Stennis Space Center

H R (Bart) Everett

Space and Naval Warfare Systems Center

Stanley S Ipson

University of Bradford

Chang Liu

University of Illinois

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