METHODS OF MEASUREMENT Direct comparison :

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V. Rouillard 2003 1 Introduction to measurement and statistical analysis METHODS OF MEASUREMENT Direct comparison: Compare unknown quantity (measurand) against a known quantity (standard). Eg: tape measure. Direct comparison not always possible or practical. Eg: measuring sound levels. Indirect comparison (calibrated system): Makes use of a sensor or transducing device (transducer) to transform the measurand into an analogous form. The sensor is connected to a series of instruments which convert the output of the sensor into a useful analogous form which presents the measurand in a useful and practical format.

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METHODS OF MEASUREMENT Direct comparison : Compare unknown quantity (measurand) against a known quantity (standard). Eg: tape measure. Direct comparison not always possible or practical. Eg: measuring sound levels. Indirect comparison (calibrated system): - PowerPoint PPT Presentation

Transcript of METHODS OF MEASUREMENT Direct comparison :

Page 1: METHODS OF MEASUREMENT Direct comparison :

V. Rouillard 2003

1 Introduction to measurement and statistical analysis

METHODS OF MEASUREMENT

Direct comparison:

• Compare unknown quantity (measurand) against a known quantity (standard). Eg:

tape measure.

• Direct comparison not always possible or practical. Eg: measuring sound levels.

Indirect comparison (calibrated system):

• Makes use of a sensor or transducing device (transducer) to transform the measurand

into an analogous form.

• The sensor is connected to a series of instruments which convert the output of the

sensor into a useful analogous form which presents the measurand in a useful and

practical format.

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2 Introduction to measurement and statistical analysis

METHODS OF MEASUREMENT

• Processing of the analogous signal is often necessary to extract the desired information

from the signal.

• For reasons related to signal processing, automatic recording and process control, the

majority of measuring systems convert the measurand into an analogous electrical form.

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THE GENERALISED MEASURING SYSTEM

Most measuring systems consist of three stages:

1. Detection-transduction stage (sensor-transducer)

2. Intermediate stage (signal conditioning)

3. Terminating stage (readout, display, recorder)

Sensor-transducer

Indicator

Signal conditione

r

Recorder

Processor

Controller

Human (eyes, pen,

paper)

measurandConditioned

signal(raw) signal

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THE GENERALISED MEASURING SYSTEM

Detection-transduction stage (sensor-transducer)

• Function: to detect or sense the measurand without affecting it.

• Ideally, must also be insensitive to other variables. Eg: Pressure sensor must be

insensitive to acceleration, strain gauge must be insensitive to temperature.

• Unwanted sensitivity is a measuring error.

• Noise: high frequency (fast)

• Drift: low frequency (slow)

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THE GENERALISED MEASURING SYSTEM

Signal conditioning stage

• Function: to modify (improve) the transduced information for compatibility with the

terminating (readout / recording/ processing) stage

• These include amplification (most common) , filtering (noise removal), offset

adjustment, differentiation, integration, telemetry….

• Sometimes also used to provide electrical power or excitation signal required by

sensor.

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THE GENERALISED MEASURING SYSTEM

Terminating stage (readout, display, recorder)

• Function: to provide information on measurand in a format suitable for the

application.

• For (immediate) human recognition, the display usually comprises:

1. A relative displacement indicator. Eg: needle, / pointer, trace in a screen

(oscilloscope), stylus on a chart, a level change (thermometer)…

2. In digital (numeric) form. Eg: counter (odometer), numeric LCD etc..

• For recording or processing purposes, the terminating stage may comprise of

magnetic recorders, chart (paper) recorders, digital recorders (PC-based data

acquisition systems, digital storage oscilloscopes), process controllers (PLCs,

computer-based control systems).

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7 Introduction to measurement and statistical analysis

THE GENERALISED MEASURING SYSTEM

Example: Pressure gauge

Sensor-transducer: Piston/cylinder

(pressure to force) and spring

(force to displacement)

Indicator: Visual

scale

Signal conditioning:

none

measurand: Pressure

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THE GENERALISED MEASURING SYSTEM

Example: Rocket velocity

Accelero-meter

Low-pass filter

Sensor-transducer Signal conditioning

Integrator

Amplifier

Recording & display

PC Data acquisitio

n

Printer

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THE GENERALISED MEASURING SYSTEM

Example: Rocket velocity

Accelero-meter

Low-pass filter

Sensor-transducer Signal conditioning

Integrator

Amplifier

Recording & display

PC Data acquisitio

n

Printer

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Dial Gauge

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MEASURING SYSTEMS : SELECTED EXAMPLES

Displacement / distance: micrometer

Micrometer

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MEASURING SYSTEMS : SELECTED EXAMPLES

Displacement / distance: Linear Variable Differential Transformer (LVDT)

                          

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MEASURING SYSTEMS : SELECTED EXAMPLES

Displacement / distance: Linear Variable Differential Transformer (LVDT)

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MEASURING SYSTEMS : SELECTED EXAMPLES

Displacement / distance: Linear Variable Differential Transformer (LVDT)

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MEASURING SYSTEMS : SELECTED EXAMPLES

Displacement / distance: Laser (triangulation)

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MEASURING SYSTEMS : SELECTED EXAMPLES

Displacement / distance: Laser (triangulation)

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MEASURING SYSTEMS : SELECTED EXAMPLES

Displacement / distance: Time-of-flight distance sensors:

Ultrasonic (Sonar), Radio waves (Radar), Optical (Ladar),

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MEASURING SYSTEMS : SELECTED EXAMPLES

Displacement / distance: Time-of-flight distance sensors:

Ultrasonic (Sonar), Radio waves (Radar), Optical (Ladar),

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MEASURING SYSTEMS : SELECTED EXAMPLES

Displacement / distance: Time-of-flight distance sensors:

Ultrasonic (Sonar), Radio waves (Radar), Optical (Ladar),

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MEASURING SYSTEMS : SELECTED EXAMPLES

Displacement / distance: Time-of-flight distance sensors:

Ultrasonic (Sonar), Radio waves (Radar), Optical (Ladar),

• Laser diode is pulsed every microsecond

• The reflection is detected by a photo diode

Animation courtesy Banner Engineering

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MEASURING SYSTEMS : SELECTED EXAMPLES

Strain: (resistance strain gauge)

• When the conductor (wire) is strained (extended), its cross-sectional area reduces and

the total electrical resistance increases.

• The change in resistance is used to measure the strain of the material or component

onto which the strain gauge is bonded.

Bi-axial gaugeTri-axial gauge

(rosette) for Principal strains

Bi-axial gauge for normal or shear

strains

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R = L/A or R = L/CD2 C=1 O: C=� /4 (1)

When the conductor is strained, its geometry will change. Differentiating (1)

dR = CD2(L d + dL) – 2C LD dD / (CD2)2

= [(L d + dL) - 2 L dD/D] / CD2 (2)

Dividing (2) by (1)

dR/R = dL/L - 2dD/D + d/ (3)

Dividing by dL/L throughout:

(dR/R) / (dL/L) = 1 – 2(dD/D)/(dL/L) + (d/)/(dL/L) (4)

Since dL/L = a = axial strain, dD/D = L = lateral strain and = Poisson’s Ratio =

(dD/D)/(dL/L), Eqn. (4) can be written to define the Gauge Factor, G:

G = (dR/R)/(dL/L) = (dR/R)/ a or a = (dR/R)/G (5)

MEASURING SYSTEMS : SELECTED EXAMPLES

Strain: (resistance strain gauge)

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MEASURING SYSTEMS : SELECTED EXAMPLES

Force

Strain gauge type load cells

                          

• Force and torque are often measured by

bonding a number of strain gauges on a

carefully designed component called a load

cell. The load cell is usually manufactured

using steel which has very linear (elastic)

properties as well as having a high elastic

modulus (low deformation under load).

• Load cells can be designed to measure a

wide variety of forces such as

compression, bending, tension, shear and

torque.

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MEASURING SYSTEMS : SELECTED EXAMPLES

Strain: (resistance strain gauge)

The Wheatstone bridge

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MEASURING SYSTEMS : SELECTED EXAMPLES

Strain gauge type load cells

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MEASURING SYSTEMS : SELECTED EXAMPLES

Strain gauge type load cells

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MEASURING SYSTEMS : SELECTED EXAMPLES

Strain gauge type load cells

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MEASURING SYSTEMS : SELECTED EXAMPLES

Strain gauge type load cells

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MEASURING SYSTEMS : SELECTED EXAMPLES

Strain gauge type load cells

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MEASURING SYSTEMS : SELECTED EXAMPLES

Strain gauge type load cells

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MEASURING SYSTEMS : SELECTED EXAMPLES

Strain gauge type load cells

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MEASURING SYSTEMS : SELECTED EXAMPLES

Strain gauge type load cells

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MEASURING SYSTEMS : SELECTED EXAMPLES

Strain gauge type load cells

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MEASURING SYSTEMS : SELECTED EXAMPLES

Time response

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MEASURING SYSTEMS : SELECTED EXAMPLES

Time response

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MEASURING SYSTEMS : SELECTED EXAMPLES

Time response

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MEASURING SYSTEMS : SELECTED EXAMPLES

Time response

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MEASURING SYSTEMS : SELECTED EXAMPLES

Temperature

• Thermocouples are based on the principle that when two dissimilar metals are joined

a predictable voltage will be generated that relates to the difference in temperature

between the measuring junction and the reference junction (connection to the

measuring device).

• RTDs are wire wound and thin film devices that work on the physical principle of the

temperature coefficient of electrical resistance of metals. They are nearly linear over a

wide range of temperatures and can be made small enough to have response times

of a fraction of a second. They require an electrical current to produce a voltage drop

across the sensor that can be then measured by a calibrated read-out device.

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MEASURING SYSTEMS : SELECTED EXAMPLES

Velocity: Interferometry (Michelson interferometer)

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MEASURING SYSTEMS : SELECTED EXAMPLES

Velocity: Interferometry

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MEASURING SYSTEMS : SELECTED EXAMPLES Piezoelectric sensors

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MEASURING SYSTEMS : SELECTED EXAMPLES Piezoelectric sensors

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MEASURING SYSTEMS : SELECTED EXAMPLES Piezoelectric sensors

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MEASURING SYSTEMS : SELECTED EXAMPLES Piezoelectric sensors

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MEASURING SYSTEMS : SELECTED EXAMPLES Piezoelectric sensors

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MEASURING SYSTEMS : SELECTED EXAMPLES Piezoelectric sensors

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Sensitivity (Pc/g or V/g) Range Resolution Transverse sensitivity Amplitude linearity Frequency response or

frequency range

MEASURING SYSTEMS : SELECTED EXAMPLES Piezoelectric sensors

Accelerometer performance:

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MEASURING SYSTEMS : SELECTED EXAMPLES Piezoelectric sensors

Accelerometer performance:

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Temperature – may affect sensitivity, natural frequency and damping.

Effects sometimes characterised by manufacturer.

Humidity – mainly affects high impedance transducers.

Acoustic noise.

Strain sensitivity – may generate spurious signals when the case is

strained or distorted (ie. badly mounted)

MEASURING SYSTEMS : SELECTED EXAMPLES Piezoelectric sensorsEnvironmental effects:

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MEASURING SYSTEMS : SELECTED EXAMPLES Piezoelectric sensors

Accelerometer mounting:

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The vibrational characteristics of a structure can be altered by adding

mass to that structure. An accelerometer that is too heavy, with respect

to the test structure, will affect the vibrational behaviour of the structure

and give erroneous measurements. Care must be used when selecting

an accelerometer and mounting hardware to avoid the effects of mass

loading.

MEASURING SYSTEMS : SELECTED EXAMPLES Piezoelectric sensors

Accelerometer mass loading:

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MEASURING SYSTEMS : SELECTED EXAMPLES Piezoelectric sensors

Charge amplifiers

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MEASURING SYSTEMS : SELECTED EXAMPLES Piezoelectric sensorsFrequency Response:

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MEASURING SYSTEMS : SELECTED EXAMPLES(Ref: Mechanical Measurements 5th ed. Beckwith, Marangoni & Leinhard)

Instrument type Measurand Method Typical hardware

Potentiometer Displacement Electrical Resistance DC power supply - voltage divider (metre - ohms - volt)

LVDT Displacement Inductance AC excitation signal (Modulator) & Demodulator (metre - henry - volt)

Ultrasonic Displacement Time of flight Ultrasonic generator, ultrasonic microphone & Clock (metre - second - volt)

Laser - Triangulation

Displacement Geometrical variations

Laser light source & photodiode array (metre - count - volt)

Optical encoder Displacement Optical masking Optical source, counter (metre - count s- pulses)

Laser - Interferometer

Displacement / velocity

Optical interference Laser light source, optical splitters, photodiode, frequency counter / converter. (metre - count/rate - volt)

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Instrument type Measurand Method Typical hardwareAccelerometer Acceleration Piezoelectric effect Charge amplifier (g -coulomb

- volt)Pressure sensor Fluid pressure Piezoelectric effect Charge amplifier (Pascal -

coulomb - volt)Force sensor Dynamic force Piezoelectric effect Charge amplifier (Newton -

coulomb - volt)Pressure sensor Fluid pressure Capacitive (distance) Capacitance bridge -

modulator/demodulator (metre - Farad - volt)

Water surface elevatuion (waves)

Surface elevation (displacement )

Change in permitivity -capacitance

Capacitance bridge - modulator/demodulator (metre - Farad - volt)

Load cell Force Component strain (dimentional change)

Resistance bridge (newton -metre - ohm - volt)

MEASURING SYSTEMS : SELECTED EXAMPLES(Ref: Mechanical Measurements 5th ed. Beckwith, Marangoni & Leinhard)

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Instrument type Measurand Method Typical hardwareThermocouple Temperature Seedbeck effect

(emf across different metals)

Amplifier / lineariser (C -microvolt - volt)

RTD (Resistance Temperature Detector)

Temperature Thermo-resistive effect

Weathstone bridge & amplifier (C -ohm - volt)

Semiconductor-Junction Temperature sensors

Temperature Semiconductor junction

Integrated circuit (C - volt)

Fluid flow rate Flow rate Obstruction effect : pressure drop across venturi, flow nozzle, orifice plate

(m^3/s - pascal -volt)

Fluid flow rate Flow rate Turbine speed Pulse / frequency counter (m^3/s - hertz -volt)

Fluid flow rate Flow rate Magnetic induction (Faraday's law)

(m^3/s - gauss -volt)

Fluid flow rate Flow rate Vortex shedding frequency

Pulse / frequency counter (m^3/s - hertz -volt)

MEASURING SYSTEMS : SELECTED EXAMPLES(Ref: Mechanical Measurements 5th ed. Beckwith, Marangoni & Leinhard)