Optris CT G5, PI 640 G7 User Manual

innovative infrared technology
Production
Quality Assurance
Research & Development
Test & Measurement
NON-CONTACT TEMPERATURE MEASUREMENT GLASS INDUSTRY
2 4 6 8 10 12 14 16
Wavelength in µm
Wavelengh [µm]
TECHNOLOGY AND PHYSICS
Inuence from the surroundings
The illustration shows that the transmissivity of air strongly
depends on the wavelength. Strong attening alternates with
areas of high transmissivity – the so-called atmospheric windows. The transmissivity in the longwave atmospheric window (8 – 14 µm) is constantly high whereas there are measurable alleviations by the atmosphere in the shortwave area, which may lead to false results. Typical measuring windows are 1.1 – 1.7 µm, 2 – 2.5 µm and 3 – 5 µm.
Additional inuences can arise from heat sources in the environment of the measuring object. To prevent wrong measu­ring results due to increased ambient temperatures, the infrared
thermometer compensates the inuence of ambient temperatures
beforehand (as e.g. when measuring temperatures of glass surfaces in heating areas whereby the walls are hotter than the glass surfaces). A second tem-perature sensing head helps to generate accurate measuring results by automatically compensating the ambient temperatures and a correctly adjusted emissivity.
100
Radiation
from
ambient
n
T
Object
amb
ρ
n
T
n
T
amb
obj
= α
ε
τ
Sensor
α = Absorption ρ = Reflectance τ = Transmission ε = Emissivity
Compensating ambient influences
Emissivity and temperature measurement
For the accurate measurement of temperatures, emissivity is a key factor. It is dependent on various inuences and must be adjusted according to the application.
75
Transmissivity in %
50
25
0
Spectral transmissivity of air (1 m, 32 °C (90 °F), 75 % r. F.)
Dust, smoke and suspended matter in the atmosphere can pollute the optics and result in false measuring data. Here air purge collars (which are installed in front of the optics with compressed air) help to prevent deposition of suspended matter in front of the optics. Accessories for air and water cooling support the use of infrared thermometers even in hazardous surroundings.
Emissivity theoretically depends on the material, its surface quali­ty, wavelength, the measuring angle and, in some cases, even
the applied measuring conguration.
Glass usually exhibits an emissivity of 0.85 in the longwave range
(8 – 14 μm). In processes with higher temperatures glass surfaces are measured with 5.0 μm or 7.9 μm because in those spectral ranges the emissivity is ≥0.95.
The main advantage of 7.9 µm is the lower angle dependency of the glass surface reection in this wavelength range. This means
that the surface temperature can be measured independently of
the reection even at an inclined viewing angle.
Emissivity
2
Spectral emissivity of glass
The CoolingJacket Advanced enables an operation within an ambient temperature of up to 315 °C (599 °F)
Temperature measurement of glass
Hot spot detection at glass bottle production
If you measure temperatures of glass with IR thermometers or the special IR camera optris PI G7 it implies that you take care of
reection and transmissivity. A careful selection of the wavelength
facilitates measurements of the glass surface as well as of the deeper layers of the glass. Wavelengths of 1.0 µm, 2.2 µm or
3.9 µm are appropriate for measuring deeper layers whereas 5 µm are recommended for surface measurements. If temperatu­res are low, you should use wavelengths between 8 and 14 µm in combination with an emissivity of 0.85 in order to compensate
reection. For this purpose a thermometer with short response
time should be used as glass is a bad heat conductor and can change its surface temperature quickly.
100
innovative infrared technology
Line scan with compact infrared camera
Optris infrared cameras are equipped with license­free PI Connect software. The software enables the cameras to operate as line scan cameras.
Line scanners are traditionally used in the glass industry for various measurement procedures. In these devices, a point detector is coupled with a rotating mirror to consequently generate a linear optical scan of the object. These devices are bulky and expensive.
When using an infrared camera as a line scanner, an arbitrary line is selected from the detector array. In addition to the more compact construction and the
lower price, there are two signicant benets: the line
to be scanned can be positioned anywhere using the software and the user receives a complete IR image quasi as additional information – these are important advantages, especially during system setup.
The cameras can accurately measure surface tempe­ratures of moving measurement objects using minimal
apertures. This function is of particular signicance in
the glass industry, since the glass temperature has a direct impact on the quality. During the production process, temperatures are measured accordingly at many points and it is possible to intervene in the process, when necessary, if there are deviations in setpoint temperatures.
For example, the Optris PI 450 G7, a special IR camera for glass applications, can scan the complete
glass width using in the oat process (Up to 4 m [13 ft])
with an 80° lens using the diagonals as scan line at a
height of 2.1 m (6.9 ft).
80
Transmissivity in %
60
40
20
0
2 3 4 5
Further information in our infrared basics brochure: www.optris.com/optris-downloads
Wavelengh [µm]
Lines have FOV of up to 111° for detailed process analysis.
111 °
any number of lines
800 Pixel
Up to 125 Hz data recording of unlimited lines which in turn produce a thermal image of any given resolution
3
Loading...
+ 5 hidden pages