User Manual
Table Of Contents
- 1 Disclaimers
- 2 Safety information
- 3 Notice to user
- 4 Customer help
- 5 Introduction
- 6 Quick start guide
- 7 A note about ergonomics
- 8 Camera parts
- 9 Screen elements
- 10 Navigating the menu system
- 11 Handling the camera
- 11.1 Charging the battery
- 11.2 Turning on the camera
- 11.3 Turning off the camera
- 11.4 Adjusting the viewfinder’s dioptric correction
- 11.5 Adjusting the angle of the lens
- 11.6 Adjusting the infrared camera focus manually
- 11.7 Autofocusing the infrared camera
- 11.8 Continuous autofocus
- 11.9 Operating the laser pointer
- 11.10 Using the digital zoom function
- 11.11 Assigning functions to the programmable buttons
- 11.12 Using the camera lamp as a flash
- 11.13 Changing lenses
- 11.14 Using the close-up lens
- 11.15 Changing the viewfinder eyecup
- 11.16 Calibrating the compass
- 12 Saving and working with images
- 13 Achieving a good image
- 14 Working with image modes
- 15 Working with measurement tools
- 15.1 General
- 15.2 Adding/removing measurement tools
- 15.3 Working with user presets
- 15.4 Resizing or moving a measurement tool
- 15.5 Changing object parameters
- 15.6 Displaying values in the result table and displaying a graph
- 15.7 Creating and setting up a difference calculation
- 15.8 Setting a measurement alarm
- 16 Working with color alarms and isotherms
- 17 Annotating images
- 18 Programming the camera (time lapse)
- 19 Recording video clips
- 20 Screening alarm
- 21 Pairing Bluetooth devices
- 22 Configuring Wi-Fi
- 23 Changing settings
- 24 Technical data
- 24.1 Online field-of-view calculator
- 24.2 Note about technical data
- 24.3 Note about authoritative versions
- 24.4 FLIR T1020 12°
- 24.5 FLIR T1020 28°
- 24.6 FLIR T1020 45°
- 24.7 FLIR T1030sc 12°
- 24.8 FLIR T1030sc 28°
- 24.9 FLIR T1030sc 45°
- 24.10 FLIR T1040 12°
- 24.11 FLIR T1040 28°
- 24.12 FLIR T1040 45°
- 24.13 FLIR T1050sc 12°
- 24.14 FLIR T1050sc 28°
- 24.15 FLIR T1050sc 45°
- 25 Mechanical drawings
- 26 Cleaning the camera
- 27 Application examples
- 28 About FLIR Systems
- 29 Glossary
- 30 Thermographic measurement techniques
- 31 History of infrared technology
- 32 Theory of thermography
- 33 The measurement formula
- 34 Emissivity tables
The measurement formula
33
magnitudes of the three radiation terms. This will give indications about when it is impor-
tant to use correct values of which parameters.
The figures below illustrates the relative magnitudes of the three radiation contributions
for three different object temperatures, two emittances, and two spectral ranges: SW and
LW. Remaining parameters have the following fixed values:
• τ = 0.88
• T
refl
= +20°C (+68°F)
• T
atm
= +20°C (+68°F)
It is obvious that measurement of low object temperatures are more critical than measur-
ing high temperatures since the ‘disturbing’ radiation sources are relatively much stron-
ger in the first case. Should also the object emittance be low, the situation would be still
more difficult.
We have finally to answer a question about the importance of being allowed to use the
calibration curve above the highest calibration point, what we call extrapolation. Imagine
that we in a certain case measure U
tot
= 4.5 volts. The highest calibration point for the
camera was in the order of 4.1 volts, a value unknown to the operator. Thus, even if the
object happened to be a blackbody, i.e. U
obj
= U
tot
, we are actually performing extrapola-
tion of the calibration curve when converting 4.5 volts into temperature.
Let us now assume that the object is not black, it has an emittance of 0.75, and the trans-
mittance is 0.92. We also assume that the two second terms of Equation 4 amount to 0.5
volts together. Computation of U
obj
by means of Equation 4 then results in U
obj
= 4.5 /
0.75 / 0.92 – 0.5 = 6.0. This is a rather extreme extrapolation, particularly when consider-
ing that the video amplifier might limit the output to 5 volts! Note, though, that the applica-
tion of the calibration curve is a theoretical procedure where no electronic or other
limitations exist. We trust that if there had been no signal limitations in the camera, and if
it had been calibrated far beyond 5 volts, the resulting curve would have been very much
the same as our real curve extrapolated beyond 4.1 volts, provided the calibration algo-
rithm is based on radiation physics, like the FLIR Systems algorithm. Of course there
must be a limit to such extrapolations.
Figure 33.2 Relative magnitudes of radiation sources under varying measurement conditions (SW cam-
era). 1: Object temperature; 2: Emittance; Obj: Object radiation; Refl: Reflected radiation; Atm: atmos-
phere radiation. Fixed parameters: τ = 0.88; T
refl
= 20°C (+68°F); T
atm
= 20°C (+68°F).
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