Heitronics precision thermometers

Temperature: -25 °C - 3,000 °C
Spectral range: 2 µm - 14 µm
Response time: 5 ms

Brief description Radiation Thermometers (Pyrometers) in a robust stainless steel housing with highly stable measurement performance thanks to the HEITRONICS chopped radiation method which utilizes a pyroelectric detector. ...

Temperature: -50 °C - 1,000 °C
Spectral range: 8 µm - 14 µm
Response time: 30 ms - 15,000 ms

HEITRONICS transfer radiation thermometers guarantee precise and long-term stable temperature measurements. They are used for calibrating cavity blackbodies and plate radiation sources, radiation thermometers ...

Temperature: -100 °C - 3,000 °C
Spectral range: 0.9 µm - 20 µm
Response time: 5 ms - 600,000 ms

An application-rich Radiation Thermometer (Pyrometer) for industry, laboratory and research. The KT19 II is the reference class of Radiation Thermometers. A high-performance product for non-contact temperature ...

Temperature: 200 °C - 3,000 °C
Spectral range: 0.9 µm - 1.7 µm
Response time: 1 ms

The CT18 series are short-wave Radiation Thermometers (Pyrometers) making them suitable for measuring medium-to-high-temperature metals, refractory and much more. Process related radiation changes on the surface to be ...

Temperature: -100 °C - 3,000 °C
Resolution: 0 °C
Spectral range: 2 µm - 20 µm

A digital chopped Radiation Thermometer (Pyrometer) that leaves nothing to be desired. Close to 20 optimized spectral ranges and innovative technology make the KT15 IIP the most versatile HEITRONICS instrument. The KT15 ...

Temperature: 300 °C - 3,000 °C
Response time: 1 ms

The measurement is based on the ratio of energy received in two neighboring narrowband spectral ranges. This measuring principle eliminates radiation differences due to dust, smoke or dirty windows that affect both wavelengths equally. ...

Temperature: 500 °C
Resolution: 0.2 °C
Spectral range: 8 µm - 14 µm

A hard gold-plated parabolic mirror reflects the measuring spot onto itself. The radiation emitted from the object is “captured” in this way. Multiple reflections result in a significantly higher radiance in this area than the object ...