Analog Sensors Intro and Explanation ppt

107
Chap 3 Analog sensors

Transcript of Analog Sensors Intro and Explanation ppt

Page 1: Analog Sensors Intro and Explanation ppt

Chap 3 Analog sensors

Page 2: Analog Sensors Intro and Explanation ppt

3.1 Introduction

● to prevent error ⇒ error measurement sensor are used (type and

characteristics have to be found) ● size (length) measurement is important in precision machines sensors measuring length error are mostly studied (in the course)

● sensor limitations sometimes machine structure can be changed

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3.1 Introduction

● sensor is a device that responds to or detects a physical quantity and transmits the resulting signal to a controller

● transducer: transforms energy types

▶ piezo material: electric E ⇔ mechanical E (sensor or actuator)▶ shape memory alloy: thermal E ⇒ mechanical E (transform: change to original shape)

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Definitions

● absolute: output is always relative to a fixed reference regardless of the initial condition● incremental: output is a series of binary pulses ● analog: continuous output (proportional to physical quantity being measured)● digital: discrete output ▶ series of binary pulses▶ each pulse represents sensor’s resolution

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Sensor performance

ex) accuracy, resolution, repeatability  ● average outputaverage value of sensor output from many data ⇒ As N increases, random error decreases at the ratio of (N)1/2 (noise level decrease) ⇒ resolution increases

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sampling rate

● v: max. slew rate (related to measurand change)● increase resolution() by a factor of N (resolution δ is limited by random noise) ● total sampling time: ttotal sampling = δ/Nv(during this time, measurand will not change by more than 1/N times the resolution)● in order to increase resolution by averaging random noise ⇒ N2 data points have to be taken⇒⇒ minimum required sampling period

tsample = /N3v

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frequency response

● effect on the output of sensor of the physical quantity being measured

frequency()

1

Sensor outputphys quan

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Definitions● hysteresis: maximum difference in sensor output between measurements made from 0 to 100% full scale output and 100 to 0%● linearity: variation in proportionality constant (between output signal and measured physical quantity)● mapping: measuring sensor response to a known input under known conditions and storing results in a look-up table or fitting mathematical expression to the data⇒ nonlinearity, hysteresis, and temperature effects can be compensated

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Definitions ● noise: magnitude of any part of the sensor output that is not directly related to the physical quantity being measured ● noise input margin: maximum noise input level (ex, deviation in supply voltage) that can be tolerated without affecting desired sensor performance ● resolution: smallest detectable change in the measured physical quantity

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Definitions

● sensitivity: variation in sensor output caused by a variation of physical quantity

● slew rate error: how the accuracy of sensor changes with the rate of change of measured physical quantity ● standoff distance: distance between sensor and target 

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Definitions● step response: time-varying change in sensor output given a step change in the measured physical quantity

Delay timeRise time

Storage time

Fall time

Time

Sen

sor

oup

ut

10%

90%

100%

Ideal response to a step input

Actual response to a step input

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3.1.2 System dynamics

● sensor frequency response ⇒ system’s ability to respond to changes in the measurand(fast process ⇒ inaccurate measurement) ⇒ frequency that a sensor’s output tends to decrease because it can no longer accurately detect changes in a rapidly changing measurand ⇒ determined experimentally or analytically How quickly system accuracy can be degraded with increasing frequency

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Mathematical modeling of a Dynamic system

● sensor system (complicated in machine tools)

2

'' ' ( )

( )( )

mx bx kx u t

U sG s

ms bs k

( )( )

( )

log ( ) log ( ) log ( )

i

j

i j

N sG s

D s

G s N s D s

log-log ⇒ graphical addition

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Mathematical modeling of a Dynamic system

● Most sensor frequency response is given in terms of 3 dB response pt (1st order system)- = n

- response = 0.707 of the response at zero frequency input(dc) (30% error)- Operates well before its -3dB frequency

● response (dB) = 20 /log10G

frequency()

1

센서출력물리량

0.7

n frequency()n

phaselag

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3.2 Nonoptical sensor systems

● generating analog signals or digital pulses in response to a physical process by other than optical means

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3.2.1 capacitance sensors

● determines the distance (gap) between probe and target surface ⇒ measures capacitance formed by two parallel plates● non-contact● performance (accuracy, linearity) determined primarily by probe capacitance

▶ large probe: 10∼100 pF ▶ small probe: 0.01∼0.1 pF

target

sensor

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3.2.1 capacitance sensors ● target material: metal (conductor), dielectric, semiconductor ⇒ affects the sensor output ▶ metal : affects sensor output equallyex) calibrated over STS measurement over brass and aluminum▶ dielectric material : different calibrations

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Applications of capacitance sensors

● motion of rotating parts (spindles, bearings)● mapping flatness of delicate objects (lens, silicon wafers)● thickness (two probes are used)

- metal thicknessl1 l2

t

1 2( )t l l l

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Applications of capacitance sensors

● thickness of dielectric plateone probe is used in conjunction with a grounded metal surface dielectric material is introduced into the gap resultant change in capacitance thickness of material is determined

metal metal대상

부도체

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Applications of capacitance sensors

● pressure measurementrigid frame + diaphragmThe diaphragm deforms due to pressure ⇒ capacitance change between diaphragm and sensor  

- proximity (presence/no presence) of nonmetal and liquid level (cf, cheap inductive proximity sensor for metal)

diaphragm

p

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probe design for capacitance sensors

● depends on application and electronic circuit configuration- matching probe shape to target surface ⇒ performance improve ● stray capacitance (between probe sensor and outer body) – removed or reduced by using guard electrode (10-14∼10-16 F) ▶ operate guard and electrode by same voltage waveform ⇒ reduce stray capacitance effect▶ collimate electric field line between sensor and target ⇒⇒ capacitance between parallel plates

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probe design for capacitance sensors

body guard

CGB

target

CGT

CSGCST

sensor

bodyguard

sensor

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Dielectric constant

● dielectric constant, ε ⇒ how easily electromagnetic waves can travel through a medium

ε = f(temp, pressure, humidity, media type)

/C A d

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probe design for capacitance sensors

● temperature, humidity ⇒ easy to control● pressure ⇒ difficult to control ⇒ reference gage (against a fixed gap) is used to compensate pressure change● cutting oil, oil shower (affecting ε) should not affect guard can be used ● A (area) ⇒ affecting accuracy▶ depending on temperature (temperature affects machine and sensor)▶ As A/d increases, accuracy, resolution better ▶ A’s surface finish large average effect

small topography effect

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3.2.2 Hall effect sensors

● Lorentz's law: charged particle moves in a magnetic field ⇒ force acting ⇒ motion trajectory of the particle changes ⇒ Lorentz force  ● Hall effect: result of Lorentz force acting on electrons flowing through a semiconductor ⇒ potential produced in direction orthogonal to the excitation current and magnetic fieldOutput voltage ∼ order of millivolts ⇒ electronics is necessary to amplify voltage⇒ combination of (Hall element + amplifier electronics) into one: Hall effect transducer

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3.2.2 Hall effect sensors

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3.2.2 Hall effect sensors

Design Hall effect sensors to be sensitive to magnetic pole (triggering)

V=0

V=VHall

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3.2.2 Hall effect sensors

bipolar digital on/off Hall effect sensor  ● combined with transistor⇒ ‘+’ (south pole) maximum trigger pt, ‘-’ (north pole) release pt ● with a magnet, Hall effect sensor produces an analog voltage proportional to the magnetic field strength⇒ distance measuring sensor (voltage is proportional to magnetic strength, and the magnetic strength is related to the distance)

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Characteristics

● magnet is needed (attached to the target)- strength changes depending on time ⇒ inadequate to ultra high precision (resolution > 5 m)- other magnets and electric field magnetic strength changes● inexpensive compared with capacitance sensor by 2 orders of magnitude● accuracy depends on the accuracy of power supply (supply voltage to semiconductor: 5V±0.001V)

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Typical applications

● unipolar head-on modeone magnet triggers Hall effect sensor (moving parallel to the direction of magnetic field)

G1

G2

D1 D2

S

B

Gau

ss

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Typical applications

● unipolar slide-by modeone magnet triggers Hall effect sensor (perpendicular, large motion)

S

B

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Typical applications

● bipolar slide-by mode

Have directionality- analog : voltage = f(distance)- digital : trigger, release

Gau

ss

Distance

B

NS

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Typical applications

● bipolar slide-by mode

B

NN

S

B

S

S

NN

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Typical applications

● Hall effect sensor can be used as a digital on/off proximity sensor

- Monitors position of objects hidden from view as long as the barrier does not block magnetic field lines⇒ sensing through dielectric and nonferrous metals

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3.2.3 Inclinometers

● electromechanical levelPrecisely measures small angle of a body (wrt horizontal or vertical reference)

▶ movement data during construction▶ motion of local geologic formation▶ machine platform stability measurement▶ machine orientation, slope measurement 

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Types

● precision pendulums are used

● mercury bubble wets a linear resistor (the more device tilts, the more resistor wet and the greater the change in the output voltage)▶ surface tension low resolution▶ inexpensive

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inclinometer● inclinometer tilts ⇒ position sensor generates an electric signal (amplified and fed back to galvanometer ⇒ galvanometer produces torque ⇒ mass to original position ⇒ current applied to galvanometer to generate balancing torque is proportional to sinθ(current x resistance = voltage) ● natural frequency depends on (g/l)1/2

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3.2.4 Inductive digital on/off proximity sensors

● consists of wire-wound ferrite (iron) core, oscillator, detector, solid-state switch    

● oscillatorproduces (high-frequency) electromagnetic field centered on core

Metal target

Coil and core

Oscillator

Detector

Output

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3.2.4 Inductive digital on/off proximity sensors

Target motion

Housing

Ferrite core

Shield

Target motion

Housing

Ferrite core

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3.2.4 Inductive digital on/off proximity sensors

● metal object moves inside electromagnetic field ⇒ eddy current inside object ⇒ receives energy from field ⇒ amplitude of oscillation decreases ⇒ if amplitude change > a value, transistor in sensor is triggered on- Object is removed⇒ transistor is back to original state (off) ● sensor response time depends on effective inductance of circuit (L), resistance(R) time delay occurs (analogous to mechanical mkb system)

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3.2.4 Inductive digital on/off proximity sensors

● other trigger, release pt ⇒ the difference is embeddied in the sensor- Small sensitive to noise- normally 2∼15% of full-scale range (decided by manufacturer) ● sensor diameter – proportional to allowable standoff distance (larger longer distance) 

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head on sensor

● shield to make field in front of sensor sharp⇒ count parts

Targer motion

Housing

Ferrite core

Shield

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slide-by sensor

● wide field without shield (oscillating field of sensor recovered after target passes ⇒ should be released before next object triggers)

Targer motion

Housing

Ferrite core

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inductive digital on/off proximity sensor

● no magnet (cf, Hall effect sensor) ● metal powder should not be attached● non-contact (cheap)● large standoff distance(∼25mm) is possible● conductive targets are needed● no moving parts ⇒ low failure possibility(replacing mechanical switch)

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3.2.5 Inductive distance measuring sensors

Target

referencecoil

active coil

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3.2.5 Inductive distance measuring sensors

● apply AC current to reference coil⇒ electromagnetic field occurs⇒ current is inducted in conductor⇒ inductive current generates magnetic field and reduces intensity of original field⇒ changes effective impedance of active coil⇒ impedance change is detected⇒ analog voltage (related to distance between sensor and target) is produced

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3.2.5 Inductive distance measuring sensors

● performance depends on material properties- Homogeneous electric properties- Good conductivity, small magnetic permeability (good for aluminum, copper, brass) requiredFerrous metal is not good ⇒ thin target material is plated or bonded (epoxy)

- 0.5mm (gold, silver, copper, aluminum)

- 1.3mm (magnesium, brass, bronze, lead)

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Characteristics ● output affected by conductive material - dirt (if nonmetal) has no problem (in optical, big problem)● thickness, diameter measurement, concentricity, 2 axis alignment● range ↑ resolution ↑

Sheet thickness

Orbit tracing and shaft error motions diameter

Shaft and dynamic displacement

ConcentricityTwo axis alignment

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Precision measurement

differential mode sensor is used for precision measurement (2 sensors)

● one against fixed object only environmental effect occurs

● difference between outputs of two sensors error compensated

● two sensors should have similar characteristics (environmental effect to be similar)

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3.2.6 Inductosyns

● copper sheet on metal plate by insulating adhesive (0.07mm), square wave ● inductive coupling is used between two coils (many overlapping windings used ⇒ error averaging) ● linear Inductosyn is a linear motion transducer having scale and slider

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3.2.6 Inductosyns

Slider

Scale

Slider

Two windings 90 out of phase

Scale

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scale

● thin STS plate is covered with insulating adhesive

● wire strip is attached onto insulating surface by printed circuit technology⇒ continuous square wave (pitch = 0.1", 0.2", 2mm)

● fixed onto machine axis

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slider

● attached onto carriage (table)

● moving above scale surface (0.1mm)(required straightness of slider = 10∼20μm)

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Slider output ● scale is excited by 5∼10kHz signal (A sint) ⇒ slider output 

B, X determined from two outputsB: amplitudeX: linear displacementS: waveform period – known

13

24

sin sin(2 / )

sin cos(2 / )

S B t X S

S B t X S

13 24/ tan(2 / )S S X S

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● precision, resolution (∼ 0.12 μm) depends on number of waveforms per unit length

● overlapping of many coils in slider, scale averaging effect noise removed, high precision ● coarse/fine position sensing system

- waveform: coarse position information- sine wave interpolation: fine position resolution

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Characteristics ● most simple (almost no problem)

● performance is affected only when dirt particle breaks circuit(dirt is fatal in optical sensors)

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Tyes of commercial linear Inductosyn

● standard (∼ 250mm)

● tape-type- One end attached to machine element and the other mounted for tension control- Tension adjustment when installed ⇒ precision is fine adjustable

● adjustable InductosynClamp and tension adjusting screw at each 3”, and adjustable independently

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rotary Inductosyn ● stator (slider)- Two separated square waveforms (sine track, cosine track are repeated) ⇒ two tracks cover entire stator

● rotor (scale)- square waveform covers entire circumference (overlapping occurs) extremely good random noise reduction (∵averaging effect)- Periodic error does not decrease ⇒ compensated by mapping

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rotary Inductosyn ● many sine, cosine waveforms

- averaging effect error reduction- High resolution (0.1 μrad)- high repeatability (0.5 μrad) ⇒ used in precision rotary table

● if too many ⇒ sine, cosine waveforms are crowded ⇒ coupling between two occurs ⇒ resolution↑, accuracy ↓

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3.2.7 Linear and rotary variable differential transformers (LVDT,

RVDT) ● electromagnetic induction principle is used- linear motion detection (<10∼20 cm)- rotary motion detection (1 rotation)

Vout

Vreference

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3.2.7 Linear and rotary variable differential transformers (LVDT,

RVDT)

core

e1 e2

e1- e2

Linear operating region

X motion

Output (e1- e2)

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LVDT components

● armature (or core) – made of ferritic (magnetic) alloy

● stem - nonmagnetic alloy- fix core to object

● transformer- Consists of a primary ac excited coil and 2 secondary coils

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LVDT components

● armature moves in coil (noncontact)  ● if primary is excited by AC power⇒ armature position affects output voltages of two secondary coil(one +, the other - ⇒ directionality determined) ● relative distance between two objects ⇒ core fixed on one, and transformer fixed on the other

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Characteristics of operation

● non-contact between winding and armature ⇒ no friction, wear, hysteresis ⇒ theoretically infinite life, extremely high reliability

● if core is properly supported, no stick/slip ⇒ theoretically infinite resolution(accuracy, resolution depends on signal conditioning electronics and A/D converter)

● stable AC excitation source is needed

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Characteristics of operation

● signal conditioner converts AC voltage in secondary coil to DC

● high output ⇒ simple circuit

● measurement length can be easily increased

● less sensitive to core radial motion

● simple, shock resistant ⇒ theoretically no maintenance is necessary

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RVDT

● similar to small electric motor ⇒ generates output voltage varying linearly depending on shaft angle

● rotation is analogous to linear motion in LVDT

● generates output voltage in secondary coil depending on shaft angle

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3.2.8 Magnetic scales

● sliding sensing head is used ⇒ detects magnetic field strength from magnetically recorded scale (sine and cosine outputs) ● scale: wire (many north, south pole pairs)  wire imprinted scale

sliding sensing head

N S S N N S

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3.2.8 Magnetic scales

                                     

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3.2.8 Magnetic scales

● merit (compared with optical sensors) – less affected by dirt, fluid contamination ● incremental⇒ slide produces two waves ⇒ electronics interprets moving distance and produces digital signal ● magnitude scale: thin wire ⇒ scale minor misalignment (0.1mm wrt moving axis) causes measurement error, irrelevant to wear

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3.2.9 Magnetostrictive sensors

● "magnetostriction" - length change of ferromagnetic material in magnetic field- magnetization change under mechanical stress

● non-contact torsion sensormeasures torsional stress of a rotating shaft ⇒ power measurement (to prevent excessive stress in rotating shaft)

● strain gage was used (attached on shaft)(expensive, electric noise, unreliable due to wear)

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Villari effect

● magnetic field change in the direction of mechanical strain (shaft twiated ⇒ strain in 45°) ● several Villari differential torque transformers along circumference ⇒ torsional stress can be precisly measured ● initial calibration is necessary (ferrous material behaves differently under similar conditions) ● sensor mounted close to the shaft ⇒ large output signal (∼ mV)

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Villari effect

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Guillemen effect

● magnetic material is in magnetic field size changes ● diameter of a long small rod changes locally

v

L

2L=vt

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Guillemen effect

⇒ diameter change stress wave reflecting point

⇒ ultrasonic transducer sends stress wave and measures time (wave reflected)

⇒ time is related to distance (magnetic field and ultrasonic transducer)

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3.2.11 Piezo material bonded sensors

● force is applied to crystalline structure oscillation ⇒ high-energy electrons emits (current flow) ⇒ stress is predicted by measuring current ● examples) accelerometer, precision loadcell, ultrasnic transducer

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piezoelectric accelerometer

● speed control, vibration sensing, position measurement

● resolution (1 μg)

● frequency response ∼ 100 kHz (good response)

● small size

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precision load cells

● thin film crystalline piezo material is used ⇒ measures nanostrains

● more sensitive than metal strain gage (2∼3 orders of magnitude)

● load range limit (maximum strain level ~ μ strain)

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ultrasonic piezoelectric sensors

● piezoelectric, magnetostrictive and electrostatic are possible

● stress wave generating/receiving sends pressure wave and receives echo pulse measure time determines distance to impurities or shape change

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3.2.12 Potentiometers

● change in electric resistance resulting from change in physical process ⇒ definition of “potentiometer” ● consists of coil or high-resistance film and wiper (used mostly)

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3.2.12 Potentiometers

● wiper position target motion

● DC voltage is applied to entire length of coil ⇒ wiper picks off intermediate voltage (variable resistance) ⇒ determine wiper position ● plastic film (large resistance)Film is continuous, potentiometers are analog devices ⇒submicron resolution is possible, but relies on DC power supply and D/A converter

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potentiometer

● most expensive

● high output voltage (no amplification necessary)

● mechanical contact between wiper and film ⇒ contaminated by dust or oil ⇒ resistance change, error ⇒ preventing contamination by using various seals

● friction and wear exist

● very small overhead compared with size

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3.2.13 Synchros and resolvers

● electromagnetic induction ⇒ (rotary) transformer (between 1st and 2nd coil)

● used in shaft positioning

● can measure infinite revolutions

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Characteristics

● high precision, inexpensive, insensitive to contamination (compared with potentiometer or optical sensor)

● disadvantage: analog device (∵ mostly used with digital control system)

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synchro

● variable transformer (output voltage is varying):The magnitude of the electromagnetic coupling between primary and secondary coils (which determines output voltage) varies with the relative angular position of the coils ● 2 modes- control synchro: electric signal depending on shaft rotation- torque synchro: shaft rotation depending on electric signal

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control synchro

● transmitters, differentials, controltransformers, receivers

● used in servo control axes

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torque synchro

● transmitters, differentials, receivers

● dial of instrument is rotated by transferring rotating angle from transmitter

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synchro applications

● long distance transmission from transmitter to receiver (up to 4km)

● used in remote devices

ex) remote steering in ships, opening/closing water gates in a power plant

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transmitters and receivers

● single-phase rotorpower supply via a slip ring (brush)● three-phase stator (electromagnetically coupled with rotor )● rotor winding is excited by AC (60∼400Hz) ⇒ voltage is inducted in stator winding (proportional to cone of angle between rotor coil and stator coil)

rotor

statorS1

S2

S3

R1

R2

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transmitters and receivers

● accuracy, repeatability and linearity depends on winding quality● exciting voltage at the rotor

2 1

2 1

2 1

2 1

1 3

2 1

3 2

max

sin

sin

sin( / 3)

sin( / 3)

/out

rotor o

rotor

rotor

rotor

in

V V t

V kV

V kV

V kV

k V V

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transmitters and receivers

● transmitter sends information

● receiver receives information- analog signal- converted to digital signal ⇒ information decoding device

synchro-to-digital converter (SDC)

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torque synchro

● torque transmitter and receiver are the same● angle information is transferred electrically (not mechanically)● a gage dial is rotated by the angle

Vin

S2

S1

S3

S2

S1

S3R1

R2

R1

R2

CG CR

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control synchro

● control transmitter, control transformer, control differential transmitter are used ⇒ signals are combined electrically and amplified ⇒ rotates motor(because of being amplified, control transmitter winding does not have to be as good as torque synchro)

● synchro performance- positioning accuracy: ±10 arcminutes- Maximum torque: 3 g-mm per receiver angle

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differential

● used with transmitter and receiver● three-phase stator, three-phase rotor● via slip rings (brushes) current is transferred to rotor winding

rotorstator

S2

S3 R1

R2

S1 R3

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control transformer

● stator, rotor coil structures are the same as in transmitter

● transmitter sends position information through 3 wires to control transformer transformed to voltage and amplified to drive the motor

● angle of motor axis is mechanically coupled to angular motion of the control transformer

● if the angles of motor and transmitter are different the shaft rotates because voltage is applied

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control transformer

Vin

S2

S1

S3

S2

S1

S3R1

R2

R1

R2

CG CR motorAmp

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resolver

● special form of synchro● better accuracy, resolution than synchro● resolver transmitter: ends of rotor windings connected ⇒ one frequency excitation is needed

rotor

R1

R2

S2

S1

S4

S3

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resolver

● windings added ⇒ resolution ↑

13

24

13

24

sin

sin sin

sin cos

tan

V A t

S kA t

S kA t

S

S

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synchro, resolver-to-digital converters

● device to transform signal to digital (in order to be used in digital control) ● SDC, RDC 16 bit resolution ⇒ total rangeis divided into 216

⇒ resolution = total range/216

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3.2.14 ultrasonic sensors

● stress wave generating/ receiving ⇒ pressure wave to medium ⇒ measures amplitude and return time of the echo

Time is related to the distance to impurities or shape change in material ● piezoelectric transducers

- used in NDT (∼100 kHz) - measurement of thickness and surface

roughness (resolution: 10 to 12 bits)

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3.2.14 ultrasonic sensors

● magnetostriction transducers ● electrostatic transducers- Use metal film, metallic backing dish- oscillating applied to film ⇒ inductive current in dish due to electric field ⇒ current in field generates force ⇒ attracting and pusjing forces between dish and metalized film act repeatedly ⇒ ultrasonic wave occurs

- dish, film are small mass ⇒ fast response

- high frequency used ⇒ high precision, high resolution in small range

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3.2.15 Velocity sensors

● velocity feedback is needed for position, velocity control ● position signal differentiated ⇒ noise spikes● relative motion between magnet and (moving) coil induces voltage- Proportional to relative velocity between coil and magnet and rate of magnetic flux change (due to moving magnet)

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Linear velocity transducers (LVT)

● measures linear velocity

● similar to LVDT, but does not use excitation voltage ● uses two coils ⇒ voltage difference represents speed, and sign of voltage represents direction

Page 103: Analog Sensors Intro and Explanation ppt

Linear velocity transducers (LVT)

● modeled as pure inductance, resistor ⇒ behaves as 1st order system

= 2 L/R (time constant: ~0.001 sec) ● speed ↑ ⇒ time lag ↓⇒ linearity ↓

N S

V1 V2

Page 104: Analog Sensors Intro and Explanation ppt

Tachometer

● velocity transducer

● types: - permanent magnet stator dc tachometers- drag-torque tachometers- capacitor tachometers- digital tachometers- dc brushless tachometers

Page 105: Analog Sensors Intro and Explanation ppt

permanent-magnet stator dc tachometers

● consists of rotor winding, commutator assembly● armature (rotor winding) rotates ⇒ windings passes stator magnetic field ⇒ voltage is induced in windings proportional to rotational speed● reverse of dc motor● voltage is transferred by brush, slip-ring● number of armature coils is discrete ⇒ ripple occurs ⇒To reduce ripple, filtering techniques and many coils are used● other error source: commutator interface contamination, temperature change, magnetic field

Page 106: Analog Sensors Intro and Explanation ppt

permanent-magnet stator dc tachometers

                                        

Page 107: Analog Sensors Intro and Explanation ppt

brushless tachometers

● magnetic rotor, wound stator ⇒ rotor and stator in brushed tachometer are switched

● no problem of brush wear

● to produce homogeneous DC signal proportional to speed, switching to other windings is required ⇒ expensive, complicated, noise reduction, no brush wear