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ME 220 Measurements & ME 220 Measurements & Sensors Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

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Page 1: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

ME 220 Measurements & SensorsME 220 Measurements & Sensors

Mechanical Measurements Applications

Chapters # 8, 9,10, 11 ( Figliola)

and 18 (Beckwith)

Page 2: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Thermometer

Thermometry based on thermal expansion

Liquid-in-glass thermometers (accuracy from ±0.2 to ±2°C)

CH. # 8 Temperature MeasurementsCH. # 8 Temperature Measurements

Page 3: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Bimetallic ThermometersIf you take two metals with different thermal expansion coefficients and bond them together, they will bend in one direction

Page 4: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Resistance Temperature Detectors RTD

R1

R2

R3 r1RRTD r3

RRTD R3 r1 r3

RR0 1 A T T0

Page 5: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Thermistors

RR0e 1/T 1/T0

Usually made of a semiconductor and have Much larger dR/dT (more sensitive) than RTD and has Fast Response

Page 6: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Thermocouple (Thermoelectric) (Thermoelectric)

Page 7: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Thermoelectric EffectsSeebeck effect: Generates voltages across two dissimilar materials when

a temperature difference is present.

Peltier effect: Moves heat through dissimilar materials when current is applied.

Page 8: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

ThermocouplesThermocouples measure the difference in temperature between two points. One of those points at a known temperature.

Page 9: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Thermocouples in Series and in Parallel

Page 10: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

THERMOCOUPLE TIME CONSTANT • The conservation of energy:

m cp dT / dt = h A (To – T) m : mass of thermocouple junction, Cp: specific heat of thermocouple junction h : heat transfer coefficient , A : surface area of thermocouple

T : junction temperature , To : environs temperature

θ =T – To / Ti - ToTi = initial measurement junction temperature, then the solution is

θ = e (-t / τ )

The time constant for this process is

τ = m cp /h A

Page 11: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Error Sources in Temperature Measurements

Conduction: Your probe can conduct heat to/from the environment to/from your desired measurement location

Page 12: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Radiative Temperature Radiative Temperature Measurements (Pyrometry)Measurements (Pyrometry)

Eb T 4

Temperatures greater than 500ºC

= 5.67•10-8 W/m2K4

Page 13: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Optical Pyrometer

Page 14: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

CH. # 9 Pressure and Velocity MeasurementsCH. # 9 Pressure and Velocity MeasurementsDynamic Pressure = Total Pressure - Static Pressure

Use of Manometers

Page 15: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Pitot Tube Principles

Page 16: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Deadweight Testers

Page 17: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Elastic Pressure Transducers

Page 18: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Bourdon Tube Gauge

Page 19: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

INCLINED MANOMETER

Page 20: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Flow velocity measurementsThermal Anemometry

Page 21: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Laser Doppler Anemometer (LDA)

Page 22: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Particle Image Velocimetry (PIV)

Page 23: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

CH. # 10 Flow Measurements Turbine

Page 24: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Obstruction Flow Meter

Page 25: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Obstruction Meters

P1 P2

V2

2 V12

2gc

Qideal V2A2 A2

1 A2 /A1 2 1/ 2

2gc P1 P2

Page 26: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Rotameter or Area meter

Page 27: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Rotameter

Page 28: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

CH. # 11 Strain Measurements

a dL

LL2 L1

L1

LL1

Page 29: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Strain Gauges

RLA

LCD2

The resistance across that conductor is

Where conductor of resistivity

If you strain this conductor axially, its length will increase while its cross sectional area will decrease. Taking the total differential of R,

dRRd R

LdL R

CD2 d CD2

1

CD2Ld dL 2L dD

D

dR

RdL

L 2dD

Dd

Page 30: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

dR /R

dL /L1 2

dD /D

dL /L d /dL /L

dR

RdL

L 2dD

Dd

a dLL

L dD

D

La

F dR /R

dL /LdR /R

a1 2v

d /dL /L

For most strain gauges, = 0.3. If the resistivity is not a function of strain, then F only depends on poisson’s ratio, and F ~ 1.6.

Gage factor

Page 31: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Strain Gauge

lateral strain

axial strain

La

F dR /R

dL /LdR /R

a1 2v

d /dL /L

1

F

RR

F and R are supplied by the manufacturer, and we measure ∆R.

Page 32: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Strain Gage

Page 33: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Strain Gage [Gage Factor = (∆R/R)/(∆L/L)

& Young’s Modulus = (P/A) / (∆L/L) ]

Page 34: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Strain Gage Bridge CircuitStrain Gage Bridge Circuit

eoei

R1 /R

4 2 R1 /R

1

F

RR

eo eiF

4 2F

Page 35: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Wheatstone Bridge

eo eiR2

R1 R2

R4

R3 R4

make R2 = R4 = R

eo eiR

R1 R

R

R3 R

eo eiR

R1

1R

R3

1

eoei

R1

R1

1

R3

Page 36: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Multiple Gauge BridgeMost strain gauge measurement systems allow us to make 1, 2, 3 or all 4 legs of the bridge strain gauges.

Eo E iR1

R1 R2

R3

R3 R4

Say that unstrained, all of these have the same value. If they are then strained, the resultant change is Eo is

dEo EoRii1

4

dRi

Eo

Page 37: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Multiple Gauges•All gauges have the same nominal resistance (generally true)

•All gauges have matched gauge factors

EoE i

F

41 2 4 3

Eo

Page 38: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Force Measurements

Page 39: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Torque & Power MeasurementsTorque T = FRPower P = T

Page 40: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

ACOUSTICS

• Acoustics is the study of Sound.

• Sound is caused by variations in Pressure transmitted through air or other materials.

• The pressure, and the resulting sound, can vary in both Amplitude and Frequency.

• Humans can detect sound over a wide range of frequencies and amplitudes.

Page 41: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

What is Sound?• Sound is a propagating disturbance in a fluid or in

a solid. The disturbance travels as a longitudinal wave.

• Airborne sound Sound in air is called airborne sound generated by

a vibrating surface or a turbulent fluid stream. • Structure borne sound Sound in solids is generally called structure borne

sound.• Sound: is measured by a microphone and has

Amplitude and Frequency

Page 42: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

SOUND WAVESrapid pressure variation

cycles of compressions and rarefactions

Page 43: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

SOUND WAVES• Sound energy is transmitted through air as a pressure wave.• Frequency : The frequency of a sound (cycles / sec.) hertz (Hz). f = 1/T (Hz) The range for human hearing is from 20 to 20.000 Hz. • Wavelength :The distance between analogous points of two

successive waves. λ = c / f where c = speed of sound (m/s)

f = frequency (Hz)

Frequency (Hz) 63 125 250 500 1K 2K 4K 8K Wavelength (m) 5,46 2,75 1,38 0,69 0,34 0,17 0,085 0,043

Page 44: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Frequency Independent of sound-pressure level.

Page 45: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

The speed of sound in air = 344 m/s fn (Temp)

The speed of sound in water = 1000 m/s

The speed of sound in solid = 3000 m/s

Speed of Sound and Wavelength

Page 46: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Sound Waves

Page 47: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Pure Tone and Noise

Page 48: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Human Ear

Page 49: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

External, Middle and Inner Ear

Page 50: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Middle &Inner ear

Page 51: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Hearing

Page 52: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Noise to Outside

• From Machines such as Airplanes, Pumps, Compressors and generators.

• From Air conditioning such as condensers, Chillers, Ventilation Opening, Louvers

• Nose Control by: Relocation, Use of Vibration Damping, Use of Attenuator and Use of Enclosure.

Page 53: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Typical Noise Sources

Page 54: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

The Decibel (dB) & Sound Power LevelThe Decibel (dB) & Sound Power Level

dB = ten times the logarithm to base 10 of the ratio of two quantities.

Power Level = 10 log (w1 / w2) dB

where w1 and w2 are the two powers.

SWL = 10 log (sound power)/(ref. power)

Reference power  (Watt) = 10-12 W, which is the threshold of hearing ( lowest detectable sound).

Page 55: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Sound Energy Decreases with (distance)2

Page 56: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Sound intensity• Sound intensity, power per unit area.• The intensity passing a spherical surface around source in a

free field is: I = W / A = W / 4 π r2   = p2 / ρ c   (W/m2)where W = power     (W)

A = area   ( m2) r = radius   (m) p = root mean square pressure  (N/m2) ρ = density     (kg/m3) c = velocity of sound   (m/s)

   

• SOUND INTENSITY LEVEL LI = 10 log (I / I0)  (dB)Where Io = reference intensity  = 10-12 W/m2.

Page 57: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Sound pressure level (SPL)• Sound measuring device respond to sound pressure .

• Sound pressure level in decibels vary with distance from source.

• SPL = 10 log (p2 / p02) = 20 log (p / p0)

where p= rms pressure (N/m2)

& po = 20x10-6 N/m2.

For Free Field : SWL=SPL +20 log r +11 dB

Page 58: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Sound Pressure

The reference value used for calculating sound-pressure level is 2 ×10-5 Pa.

Note the unit of the equation

Page 59: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Sound Level Meter

Page 60: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Adding two sound pressure levels

Diff between 2-Levels Total= Larger +

0 or 1 3

2 or 3 2

4 or 9 1

10 or more 0

Total SPL =

10

SPLloglog10 i1

10

ni

1i10

Page 61: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Addition of two sound pressure levels Addition of two sound pressure levels

Page 62: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

Noise criteria (NC)

1) NC relates SPL with frequency to show how SPL varies with frequency

2) The highest curve crossed by the data determines the NC rating. NC-39

Page 63: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

A , B, and C - Weighting

Page 64: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

A- Weighting (dBA)The ear is less sensitive with decreasing frequency.To simulate ear response use A weighting (dBA).

63 125 250 500 1kHz 2kHz 4kHz Fan Octave Band dB: 85 86 85 80 73 70 60 A-weighted : -25 -16 -9 -3 0.0 +1 +1 60 70 76 77 73 71 67 70 80 75 67 80 76

81 dBA

Page 65: ME 220 Measurements & Sensors ME 220 Measurements & Sensors Mechanical Measurements Applications Chapters # 8, 9,10, 11 ( Figliola) and 18 (Beckwith)

SOUND INSULATION• Source - Transmission Path- and Receiver

• Air-borne noise and Structure-borne noise

• Reduction of Air-borne sound:

- Relocation of source and/or receiver

- Use floating floors, Use absorbent material

- Use local insulation, and local attenuators

- Use fans with backward curved impellers

- Lined duct work and avoid crosstalk