![D-Series Handheld IR Scanners](/images/new-backgrounds/143174/1431743x1.webp)
D-Series Handheld IR Scanners
The
Actual measurement area is in the center, well away from the area contacted by the edge of the cone.
Recessed cone traps all emitted surface radiation, and blocks out any radiation from environment.
Only a thin lip of material actually contacts the target, thus minimizing heat transfer.
Reflective cone automatically corrects for emissivity variations by creating an actual blackbody at the precise location of measurement.
Figure 1. Unique Automatic Emissivity Compensation System (AECS) produces accurate temperatures everywhere the infrared probe is placed, by creating its own blackbody.
1. Emissivity errors
The true emissivity of a surface is known only approximately. Conventional IR devices without Exergen’s Automatic Emissivity Compensation System can only display an approximate temperature over their entire temperature range.
The “accuracy” specifications given by most manufacturers are only for a “black body” calibration and do not hold outside laboratory conditions. Black body calibrations do not include emissivity shifts, ambient change effects on the target, and other phenomena that introduce significant errors.
Effect of Emissivity on Temperature Reading for a
500°F (260°C) Target in 70°F (21°C) ambient
550 |
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| 290 | ||
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500 |
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450 |
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deg F |
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400 |
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| 200 |
350 |
| Conventional Infrared |
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300 |
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| 150 |
1 | 0.8 | 0.6 | 0.4 | 0.2 | 0 |
Emissivity | Clean Metals | ||||
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Figure 2.
2. Emissivity shift errors
Even if an IR “gun” is set to the correct emissivity to read a surface
accurately at a particular temperature, it does not mean that the IR ε “gun” will read the same target correctly at other temperatures.
Emissivity of virtually all surfaces changes with temperature. A common assumption for conventional IR thermometry is that emissivity is constant with changes in target surface temperature. Real materials do not have this characteristic.
Actual emissivity
Conventional IR assumption
Temperature
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