Understanding Infrared Thermography Reading 3

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Figure 1.8: Spectral distribution of a blackbody, graybody and nongraybody 100 Blackbody at 300 K Q) Q) .. > Ctl - Q) 90 u c: 80 .!!:! "0 ns 70 a: - ns 60 ... u c. 50 en Q) 40 a: ... ... 30 Q) 20 r::n ns 1- 10 L -I ~ Graybody at 300 K H- Nongray(body at 300 K 1 5 10 15 20 Wavelength (llm) Charlie Chong/ Fion Zhang
Referring back to Figure 1.5, the total exitance available to the measuring instrument has three components: • emitted energy (We), • reflected energy (Wr) from the environment and other reflecting sources, and • for nonopaque targets, energy transmitted through the target (Wt) from sources behind the target. Because a theoretical blackbody has an emissivity Ɛ of 1.00, it will reflect and transmit no energy ρ = 0, τ = 0. Real targets, however, are not blackbodies. and figure 1.9 shows the three components that comprise Wx, the total exitance that an instrument sees when aimed at a real Ufe target surface. Because only the emitted component, We, is related to the temperature of the target surface, it becomes apparent that a significant part of the measurement problem is eliminating or compensating for the other two components. This is discussed in greater detail in Chapter 4. Charlie Chong/ Fion Zhang
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Infrared Thermal Testing Reading II
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Infrared Thermography ~-- ... ... .
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Infrared Thermography Charlie Chong
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See Through & Fun Thermal Camera Ex
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How to see through clothing 2 I'
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Apache IR Thermal Weaponry ■ http
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Charlie Chong/ Fion Zhang
Page 15 and 16: Greek alphabet Letter Name Sound An
Page 17 and 18: Greek letter l fl 0 I1 p u w Charli
Page 19 and 20: SGuide-IRT Content Part 1 of 2 ■
Page 21 and 22: 1.1 Introduction to Principles & Th
Page 23 and 24: The infrared thermal imaging equipm
Page 25 and 26: The three modes of heat transfer ar
Page 27 and 28: The three modes of heat transfer ar
Page 29 and 30: Temperature and Temperature Scales
Page 31 and 32: Boston Tea Party - New governances
Page 33 and 34: The Mighty Fahrenheit & ⅝”, Eng
Page 35 and 36: Absolute zero is equal to - 273.16
Page 37 and 38: The Fourier conduction Law expresse
Page 39 and 40: The Fourier conduction Law ( One di
Page 41 and 42: Convective Heat Transfer Convective
Page 43 and 44: Figure 1.2: Convective heat flow T
Page 45 and 46: Newton's cooling law defines the co
Page 47 and 48: Radiative Heat Transfer Radiative h
Page 49 and 50: Figure 1.4: Infrared radiation leav
Page 51 and 52: Thermal infrared radiation impingin
Page 53 and 54: Reflections off Specular and Diffus
Page 55 and 56: Reflections off Specular and Diffus
Page 57 and 58: Radiant Energy Related to Target Su
Page 59 and 60: The Stefan-Boltzmann law: W= σƐT
Page 61 and 62: Figure 1.6: Typical blackbody distr
Page 63 and 64: 1.4 Practical Infrared Measurements
Page 65: Characteristics of the Target Surfa
Page 69 and 70: Characteristics of the Transmitting
Page 71 and 72: Figure 1.10; Transmission of 10m (3
Page 73 and 74: Figure 1.11: Transmission, absorpti
Page 75 and 76: Figure 1.12: Transmission curves of
Page 77 and 78: Chapter 1 Review Questions Q&A 1. b
Page 79 and 80: Q4. Heat can only flow in the direc
Page 81 and 82: Q10. The follow ing spectral band i
Page 83 and 84: Q16. In forced convection, the boun
Page 85 and 86: Q22. In the 8 to 14 μm spectral re
Page 87 and 88: 2.1 Materials Characteristics A kno
Page 89 and 90: For an emissivity reference table t
Page 91 and 92: Errors because of point source refl
Page 93 and 94: View Angle The angle between the in
Page 95 and 96: Thermal Conductivity Thermal conduc
Page 97 and 98: Thermal Diffusivity As in emissivit
Page 99 and 100: Partial 2.1 Table 2.1: d i'ffusivit
Page 101 and 102: Partial Table 2.2 Table 2.2: Normal
Page 103 and 104: Chapter 2 Review Questions Q&A 1. c
Page 105 and 106: 4. When measuring the temperature o
Page 107 and 108: 10. A highly textured surface is sa
Page 109 and 110: 3.1 Thermal Instrumentation Overvie
Page 111 and 112: Thermopile- Thermoelectric Seebeck
Page 113 and 114: What is a IR Thermopile? (non-conta
Page 115 and 116: IR Thermopile Quad Sensor (non-cont
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Thermocouple A thermocouple is a te
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Bourdon Gas Thermometers 5 f\G.3 0
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Liquid Crystal Thermometer A liquid
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Bimetallic Thermometers Dial Spiral
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In RTD devices; Copper, Nickel and
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Platinum Resistance Thermometer Cha
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RTD Materials Different materials u
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Operations of RTD An RTD takes a me
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Benefits of Thin Film RTD There are
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Thermistor +V r===~ Op A p V to A I
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3.2 Contacting Thermal Measuring De
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■ Thermocouple Thermocouples are
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■ Thermistors Thermistors arc als
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3.3 Optical Pyrometers Optical pyro
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Pyrometer A pyrometer is a type of
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Brightness Pyrometers -Wien’s Law
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The processing electronics unit amp
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Infrared Detector An infrared detec
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Figure 3.2: Response Curves of Vari
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The mercury cadmium telluride (HgCd
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Infrared Optics - Lenses, Mirrors a
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Field of View (FOV) A field of view
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What is IFOV? A measure of the spat
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Instantaneous Field of View (IFOV)
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3.5 Scanning and Imaging When probl
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Line Scanning When the measurement
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Two-dimensional Scanning - Thermal
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Figure 3.5: Optomechanlcally scanne
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Pyroelectric Vidicon Thermal Imager
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Figure 3.6: Typical uncooled infrar
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IRFPA Charlie Chong/ Fion Zhang htt
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3.6 Performance Parameters of Infra
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Performance parameters of qualitati
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Temperature Range Temperature range
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Temperature Sensitivity Temperature
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Speed of Response Speed of response
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Figure 3.7: Instrument speed to res
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Figure 3.8: Instrument field-of-vie
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D ≡ αd D = spot size (approximat
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Output Requirements Output requirem
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Spectral Range Spectral range denot
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Spectrall y selective instrumems us
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Figure 3.9: Spectral response of an
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3.7 Performance Characteristics of
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The total field of view for a line
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Instantaneous Field of View IFOV In
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Recalling! Temperature sensitivity
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IFOV - MTF The 0.35 MTF refers to:
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Fig. 2a. Slit Response Function. Ca
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Minimum Resolvable Temperature Diff
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EXAM score! D=σ∙d IFOV ratio = d
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Charlie Chong/ Fion Zhang
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Answer: D= σ•d, IFOV ration= 1/
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Break Time - Kenya Coffee Picker Ch
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Portable Handheld Devices Charlie C
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Temperature sensitivity and readabi
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Hand Held Infrared Module Charlie C
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Note that the laser beam docs not r
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Emissivity set controls, located in
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IR Sensor Module Charlie Chong/ Fio
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IR Sensor Module Charlie Chong/ Fio
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Two-color Pyrometers or Ratio Pyrom
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Phenomena which are non-dynamic in
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Some ratio thermometers use more th
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Infrared Radiometric Microscopes Ch
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Line Scanners Line scanners are div
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Special Purpose Devices Special pur
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FLIR- Forward Looking Infrared Char
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Typically, the total field of view
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Pyroelectric devices have no direct
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Figure 3.12: Infrared focal plane a
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Infrared focal plane array imager C
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Infrared focal plane array imager C
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On-board capabilities include isoth
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ccc Electron Microscope Image of mi
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Platinum Silicide IrFPA 19 t«lU 98
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Quantitative IR Image Charlie Chong
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Quantitative Thermal Measurements S
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In addition to the spot measurement
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Stored images can be retrieved, dis
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Calibration Accessories Infrared ra
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Online printers and plotters are re
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Q1. The thermal resolution of an in
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Q7. The 3 to 5 μm spectral region
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Q13. A line scanner can be used to
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Q19. For which of the following app
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Q25. Two-color (ratio) pyrometers m
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Chapter 4 Operating Equipment and U
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■ Emissivity Differences ∆τ Em
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Causes of Real Temperature Changes
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Mass Transport Differences (Fluid F
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Figure 4.1: An indication of water
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Thermal Capacitance Differences ∆
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■ Induced Heating Differences (by
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Induced Heating Differences Charlie
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■ Energy Conversion Differences E
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Figure 4.3: Catalytic reformer vess
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Infrared Thermogram Energy Conversi
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Infrared Thermogram Energy Conversi
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■ Combination of Heat Transfer Me
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Infrared Thermogram of a running mo
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■ Spectral Considerations in Prod
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Infrared Thermogram Charlie Chong/
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Infrared Thermogram ..... " I Charl
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Figure 4.5: Spectral selectivity fo
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Figure 4.7: temperature thermogram
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Figure 4.8 shows the transmission s
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Figure 4.9: Measuring temperature o
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IR Filter Charlie Chong/ Fion Zhang
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Figure 4.10: Line scanner for conti
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Preparation of Equipment for Operat
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If the instrument is out of cal ibr
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The batteries mentioned on the miss
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Comments: ■ ■ ■ Thermal resol
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Figure 4.11 : Test configuration fo
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3. Reduce the ΔT until the image i
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■ Imaging Spatial Resolution Imag
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A sample setup is illustrated in Fi
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5. If the modulation transfer funct
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Figure 4.13: Test configuration for
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4. Open slit until V meas = V max .
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■ Learning the Startup Procedure
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■ Setting the Correct Effective E
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Figure 4.14: Test configuration for
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■ Measuring and Reporting Tempera
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■ Recognizing and Avoiding Reflec
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■ Measuring the Appropriate Backg
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■ Temperature Differences Between
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■ Liquid and Compressed Gases Som
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Dewar Flask for LN Loosely fitting
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■ Electrical Safety Failure to re
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Table 4.1: Electric shock current t
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4.4 Record Keeping Keeping thorough
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Easily accessible and easily unders
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Q1. Apparent but not real temperatu
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Q5. The higher the temperature of a
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Q9. Differential thermography can b
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5.1 Overview of Applications Becaus
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Electrical Applications Electrical
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High electrical resistance is the m
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Excessive heating due to a defectiv
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Inductive currents flowing with in
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Moisture in Airframes The detection
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Process Control and Product Monitor
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The differences produced by this co
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Night Vision, Seareh, Surveillance,
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Thermogram of helicopter taken at n
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Aircraft Under IR Trap Charlie Chon
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Instruments used for these applicat
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8 to 12 μm spectral region over wh
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Animal Studies Body heat allows inf
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Injured equine foreleg (left) appea
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Work energy is expended by friction
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5.4 Fluid Flow Investigations For s
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Figure 1.7: Thermographs of valve (
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■ Building Insulation and Other F
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Figures 5.8 and 5.9 illustrate thes
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Figure 5.9: Example of air exfiltra
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Example of air exfiltration Charlie
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■ Refractory Systems Industrial s
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Refractory Thermogram Charlie Chong
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■ Subsurface Discontinuity Detect
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Figure 5.11: An example of passive
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The equipment necessary to perform
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Figure 5.12: Example of active (hea
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Typical failure modes of the materi
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Figure 5.13: Test of aircraft deici
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DC - 9 Charlie Chong/ Fion Zhang
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Figure 5.14: Conceptual sketch of t
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In this case. however, the heat pul
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Figure 5.15: Erosion/corrosion dama
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737 aircraft Charlie Chong/ Fion Zh
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When there has been adequate solar
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Liquid Level Detection Thermal capa
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Unstimulated and Stimulated Approac
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Subsurface Discontinuity Detection
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1. A major area of infrared nondest
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5. The diagnostics involved in dete
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9. Thermography has been successful
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Appendix A Glossary The following a
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Ambient temperature - Temperature o
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Figure A-1 Apparent ambient tempera
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13.Blackbody, blackbody radiator -
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Alas! Heat Capacity Volumetric = C
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27.Detector, infrared - A transduce
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Thermal Effusivity In Thermodynamic
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Alas! Exitance = Rodiosity for my A
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45.Frame repetition rate - The time
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Thermal Inertia Thermal inertia is
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Instantaneous field of View (lFOV)
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Laser pyrometer - Laser pyrometer -
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Figure 3.2: Response Curves of Vari
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Compare: Minimum resolvable tempera
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86.Radiation rererenee source - A b
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101. Sector - For a line scanner, a
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113. Subtense, angular - The angula
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121. Thermal wave imaging - A term
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125. Thermogram - A thermal map or
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Appendix B Cost Benefit Determinati
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Although the calculations are quite
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96 ASNT Level Ill Study Guide: Infr
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Appendix C, Commonly Used Infrared
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Appendix C, Commonly Used Infrared
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Peach - 我爱桃子 Charlie Cho
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Good Luck Charlie Chong/ Fion Zhang
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