314,99 €
Modern sensors working on new principles and/or using new materials and technologies are more precise, faster, smaller, use less power and are cheaper. Given these advantages, it is vitally important for system developers, system integrators and decision makers to be familiar with the principles and properties of the new sensor types in order to make a qualified decision about which sensor type to use in which system and what behavior may be expected. This type of information is very difficult to acquire from existing sources, a situation this book aims to address by providing detailed coverage on this topic. In keeping with its practical theme, the discussion concentrates on sensor types used or having potential to be used in industrial applications.
Sie lesen das E-Book in den Legimi-Apps auf:
Seitenzahl: 568
Veröffentlichungsjahr: 2013
Chapter 1. Pressure Sensors
1.1. Introduction
1.2. Pressure
1.3. Pressure ranges
1.4. Main physical principles
1.5. Calibration: pressure standards
1.6. Choosing a pressure sensor
1.7. References
1.8. Other pressure sensors manufacturers
1.9. Bibliography
Chapter 2. Optical Sensors
Introduction
2.1. Optical waveguides and fibers
2.2. Light sources and detectors
2.3. Sensors of position and movement
2.4. Optical sensors of dimensions
2.5. Optical sensors of pressure and force
2.6. Optical fiber sensors
2.7. Optical chemical sensors
2.8. Bibliography
Chapter 3. Flow Sensors
3.1. Introduction
3.2. Flow measurements based on the principle of difference in pressure
3.3. Flow measurements based on variable passage
3.4. Turbine flow meter
3.5. The mechanical flow meter (positive displacement)
3.6. Magnetic flow meter
3.7. The vortex flow meter
3.8. Ultrasonic flow meter
3.9. Coriolis mass-flow meters
3.10. Flow measurements for solid substances
3.11. Flow measurement for open channels with weirs
3.12. Choice and comparison of flow measurements
3.13. Bibliography
3.14. Website references
Chapter 4. Intelligent Sensors and Sensor Networks
4.1. Introduction
4.2. Intelligent sensors
4.3. Sensor networks and interfaces
Chapter 5. Accelerometers and Inclinometers
5.1. Introduction
5.2. Acceleration
5.3. Application ranges
5.4. Main models of accelerometers
5.5. The signal processing associated with accelerometers
5.6. Manufacturing process
5.7. The calibrations:
5.8. Examples of accelerometers and inclinometers
5.9. List of Manufacturers of Accelerometers
5.10. References
5.11. Bibliography
Chapter 6. Chemical Sensors and Biosensors
6.1. Introduction
6.2. What is involved in developing a sensor?
6.3. Electrochemical sensors
6.4. Optical sensors
6.5. Acoustic (mass) sensors
6.6. Biosensors
6.7. Future trends
6.8. Conclusions
6.9. References
Chapter 7. Level, Position and Distance
7.1. Introduction
7.2. Resistive LPD sensors
7.3. Inductive LPD sensors
7.4. Magnetic LPD sensors
7.5. Capacitive LPD sensors
7.6. Optical LPD sensors
7.7. Ultrasonic sensors
7.8. Microwave distance sensors (radar)
7.9. Level measurement
7.10. Conclusions and trends
7.11. References
7.12. Online references
Chapter 8. Temperature Sensors
8.1. Introduction
8.2. Thermal measuring techniques
8.3. Physical or direct temperature measurement
8.4. Thermoelectric measurements (thermocouples)
8.5. Resistance temperature detectors (RTDs)
8.6. Thermistors
8.7. Monolithic temperature sensors (IC sensor)
8.8. Pyrometers
8.9. References
8.10. Bibliography
Chapter 9. Solid State Gyroscopes and Navigation
9.1. Introduction
9.2. The angular rate
9.3. Different ranges of rate gyro
9.4. Main models of rate gyro
9.5. Calibration of rate sensors
9.6. General features of the gyrometers
9.7. The main manufacturers
9.8. References
9.9. Bibliography
Chapter 10. Magnetic Sensors
10.1. Introduction
10.2. Hall sensors
10.3. AMR sensors
10.4. GMR sensors
10.5. Induction and fluxgate sensors
10.6. Other magnetic field sensors
10.7. Magnetic position sensors
10.8. Contactless current sensors
10.9. References
Chapter 11. New Technologies and Materials
11.1. Introduction: MEMS
11.2. Materials
11.3. Silicon planar IC technology
11.4. Deposition technologies
11.5. Etching processes
11.6. 3-D microfabrication techniques
11.7. References
List of Authors
Index
First published in Great Britain and the United States in 2007 by ISTE Ltd
Apart from any fair dealing for the purposes of research or private study, or criticism or review, as permitted under the Copyright, Designs and Patents Act 1988, this publication may only be reproduced, stored or transmitted, in any form or by any means, with the prior permission in writing of the publishers, or in the case of reprographic reproduction in accordance with the terms and licenses issued by the CLA. Enquiries concerning reproduction outside these terms should be sent to the publishers at the undermentioned address:
ISTE Ltd6 Fitzroy SquareLondon W1T 5DXUKwww.iste.co.ukISTE USA 4308 Patrice RoadNewport Beach, CA 92663USA© ISTE Ltd, 2007
The rights of Pavel Ripka and Alois Tipek to be identified as the authors of this work have been asserted by them in accordance with the Copyright, Designs and Patents Act 1988.
Library of Congress Cataloging-in-Publication Data
Modern sensors handbook/edited by Pavel Ripka, Alois Tipek.
p. cm.
ISBN 978-1-905209-66-8
1. Detectors--Handbooks, manuals, etc. I. Ripka, Pavel. II. Tipek, Alois.
TA165.M585 2007
681'.2--dc22
2007003344
British Library Cataloguing-in-Publication Data
A CIP record for this book is available from the British Library
ISBN 13: 978-1-905209-66-8
Together with temperature, pressure is one of the most important physical quantities in our environment. Pressure is a significant parameter in such varied disciplines as thermodynamics, aerodynamics, acoustics, fluid mechanics, soil mechanics and biophysics. As an example of important industrial applications of pressure measurement we may consider power engineering. Hydroelectric, thermal, nuclear, wind and other plants generating mechanical, thermal or electrical energy require the constant monitoring and control of pressures: overpressure could cause the deterioration of enclosures or drains and cause very significant damage.
As a significant parameter, pressure enters into the control and operation of manufacturing units that are automated or operated by human operators. Pressure measurement is also used in robotics, either directly in controls or indirectly as a substitute for touch (artificial skin for example), for pattern recognition or for determining strength of grip. All these activities require instrument chains in which the first element is the pressure sensor, delivering data relating to the pressure of compressed air, gas, vapor, oil or other fluids, determining the correct operation of machines or systems.
The variety of mentioned applications demands a great diversity of sensors. This diversity also derives from the fact that pressure covers a very wide range from ultra-high vacuums to ultra-high pressures. It can be expressed as an absolute value (compared to vacuum) or as a relative value (compared to atmospheric pressure); it can also represent a difference between two pressures or relate to various media and fluids whose physical characteristics (e.g. temperature) or chemical characteristics (e.g. risk of corrosion) are very varied. Pressure units are summarized in Table 1.1.
In what follows, we will consider the different physical characteristics necessary to understand pressure sensors: pressure as a physical quantity, and various sensor models with absolute, relative or differential pressure sensors. We will take a brief look at the physical properties of fluids.
From a phenomenological point of view, pressure, p, as a macroscopic parameter is defined starting with element of force , exerted perpendicularly on an element of surface of the wall, by the fluid contained in the container:
(1.1)
The element of force caused by pressure p is perpendicular to the element of surface .
For pressure p inside the fluid with free surface we may write:
(1.2)
p0: atmospheric pressure
ρgh: hydrostatic pressure
ρ: density
g: acceleration of gravity at the place of measurement
h: distance from the free surface
Table 1.1.Units of pressure
An absolute pressure sensor measures static, dynamic or total pressure with reference to a vacuum (see Figure 1.1).
Figure 1.1.Absolute pressure sensor
A relative pressure sensor measures static, dynamic or total pressure with reference to ambient atmospheric pressure (Figure 1.2).
Figure 1.2.Relative pressure sensor
A sealed relative pressure sensor measures static, dynamic or total pressure with reference to ambient atmospheric pressure, sealed at the time of manufacture of the sensor (see Figure 1.3).
Figure 1.3.Sealed Relative pressure sensor
A differential pressure sensor measures a static, dynamic or total pressure with reference to an unspecified variable pressure p2 (Figure 1.4).
Figure 1.4.Differential pressure sensor
In static fluids, the pressure force F is exerted on the surface originates only from the random kinetic energy of molecules. In dynamic fluids force F originates from the random and directed kinetic energy of the molecules.
We generally distinguish between two main fluid families: gases and liquids.
The total pressure is the sum of the static pressure, the pressure due to external forces and the dynamic pressure. This has the same value in all points for a fluid moving horizontally (incompressible, negligible viscosity, like liquids), following Bernoulli’s theorem:
(1.3)
with:
pt: total pressure
ps: static pressure
pd: dynamic pressure
v: local velocity
ρ: density
The pressure of a gas in a tank is the force exerted by gas on the walls of the tank per unit of area. When a tank contains a mixture of gases, we can define a partial pressure for each of them. The sum of the partial pressures is equal to the total pressure. The equation of an ideal gas is:
(1.4)
p: pressure
n: number of molecules
T: temperature
V: volume
kB: Boltzmann constant
According to the kinetic theory, the molecules of a gas are driven in a continual and random manner and bump into each other. The trajectory of a molecule between two shocks is a right-hand side segment traversed at constant speed and the direction of a segment after a shock has no correlation with the direction of the segment before the shock. The trajectory of a molecule is therefore a broken line, the average value l of the length of its segments being the free mean course.
When the gas is contained in an enclosure, the molecules also have collisions with the walls and the pressure that they exert on them results from the average effect of these collisions.
Lesen Sie weiter in der vollständigen Ausgabe!
Lesen Sie weiter in der vollständigen Ausgabe!
Lesen Sie weiter in der vollständigen Ausgabe!
Lesen Sie weiter in der vollständigen Ausgabe!
Lesen Sie weiter in der vollständigen Ausgabe!
Lesen Sie weiter in der vollständigen Ausgabe!
Lesen Sie weiter in der vollständigen Ausgabe!
Lesen Sie weiter in der vollständigen Ausgabe!
Lesen Sie weiter in der vollständigen Ausgabe!
Lesen Sie weiter in der vollständigen Ausgabe!
Lesen Sie weiter in der vollständigen Ausgabe!
Lesen Sie weiter in der vollständigen Ausgabe!
