
| Model | Sensitivity (mV/(BTU/ft²sec)) | Max. mV Output | Impedance (Ω) | Max. Body Temperature | Accuracy |
|---|---|---|---|---|---|
| Mark IV-301 | 30 | 20 | 60 | 121°C (250°F) | ±3% |
| Mark IV-602 | 60 | 40 | 75 | 121°C (250°F) | ±3% |
| Mark IV-1004 | 100 | 70 | 100 | 121°C (250°F) | ±3% |
| Mark IV-601 | 60 | 40 | 120 | 121°C (250°F) | ±3% |
| Mark IV-1202 | 120 | 80 | 150 | 121°C (250°F) | ±3% |
| Mark IV-2004 | 200 | 140 | 200 | 121°C (250°F) | ±3% |
Mess-, Steuer- und Regenerate GmbH For Research, Laboratory and Industrie Features: • Non-contact temperature measurement • Choice of view angles: 150° or 75° • Impervious to pressure changes and vacuum • Self-generating utput (mV) • Flare & Flame radiation detector • Low Cost lts high sensitivity and rapid time response to heat Rux absorbed by the sensor surface distinguish the MARK IV models as top performance Radiometers. The self-generated thermoelectric output signal in millivolts (mV) is directly proportional to the incident heat flux. Various windows may be added for elimination of convective heat transfer and/or or selective spectral responses. For Non-Contact temperature measurement applications, one has to establish the temperature relation between the target and the Sensor empirically, or apply the classic relationship as expressed by the Stefan-Boltzmann equation: Q/A=.1714*10-8 *F*E* (T4target-T4sensor) BTU/ft2Hr Where: T: is the absolute temperature in Rankine (t"460) F: Form factor between Target and Sensor E: Emissivity of the target • Suitable for measuring Solar and other object's radiation in satellites and space vehicles (NASA) Aerospace • Radiant heat (IR) detection and control of various targets—broad range Window/Filter Material Quartz Sapphire BaF2 Germanium Mylar Others Transmission Range, pm 0.18 to 3.5 0.15 to 5.5 0.15 to 11.5 2 to 110.31 to 50 request Copyright© 2017 WUNTRONIC GmbH. All Rights Reserved
Open the catalog to page 12 Pages
2 Pages
8 Pages
4 Pages
2 Pages
4 Pages
7 Pages
2 Pages
5 Pages