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Thermal sensing · reference list

Literature

References for the Grid-EYE thermal channel. Links point to the original publisher or a freely available copy; no documents are re-hosted here.

Calibrating low-cost thermopile arrays beyond factory spec

Relevant to reducing the AMG8854's ±3.0 °C typical accuracy: two-point and multi-point non-uniformity correction, and die-temperature regression.

Water skin vs. bulk temperature (cool-skin effect)

An IR radiometer measures the water's radiating surface, not the bulk. A still, heated bowl on the bench showed a 10–20 °C skin-to-bulk difference.

The Temperature at the Ocean-Air Interface
P.M. Saunders · J. Atmospheric Sciences · 1967
Original theoretical treatment of the cool-skin effect; the basis for later models.

Validating IR against flowing water

Radiometric surface reading as a proxy for the temperature of moving water: calibration and validation methodology.

Windows and external optics in front of an IR sensor

A window bonded in the optical path both attenuates the scene radiance by its transmittance τ and adds its own emission at the window temperature. These references give the radiometric model, the measurement methods, the standardized procedures, and the physical limits. They are the basis for the Window Calibration work.

R. Danjoux · Infrared Training Center Technical Publication 60 (T560472_A) · free PDF
The six-component radiance balance for a window in the path, its reduction to R = ε·τw·Robj + (1 − ε·τw)·Renv under a single-temperature assumption, and a two-temperature contrasted-scene ratio method for τw that does not need a calibrated camera. States the limits used in this project: transmittance varies with window temperature, with target temperature through the spectral shift, and with pixel position for oblique rays; the environments on the two sides need not be equal.
R.P. Madding · InfraMation 2004 Proceedings, Infrared Training Center / FLIR Systems (ITC 104 A) · free PDF
Shows the band-averaged transmittance of a real (non-grey) window depends on both window and target temperature, and gives the two-target differencing equation for measuring it. Notes that the correction becomes indeterminate (0/0) when the window temperature equals the target temperature — the degeneracy encountered in the first warm-up run.
S.K. Sanders, C.T. Kuhs, T.P. Letsou, H.O. Everitt · Applied Physics Letters, 127(4):041104 · 2025 · DOI 10.1063/5.0266983 · abstract free
Defines a figure of merit that trades transmitted signal against window self-emission, and shows how anti-reflection coatings raise it and how that advantage falls off as the window heats. Sets the ceiling on what window treatment can buy.
C.S. Prasad, H.O. Everitt, G.V. Naik · Communications Engineering, 3:172 · 2024 · DOI 10.1038/s44172-024-00316-y · free full text
Companion treatment of recovering a scene behind a window whose own emission is significant.
UQG Optics · free PDF
The window in this work is a UQG ZSW-132 — Ø13 mm × 2 mm, multispectral ZnS, uncoated. This sheet gives the transmission curve (~70–72% across 3–10 µm, rolling off through the long wave), thermal conductivity 27 W/m·K, and the mechanical and optical constants. The spectral roll-off across the sensor's 8–14 µm band is the mechanism behind the target-temperature dependence of band-averaged τ noted above.
Still open: a measured band-averaged τ for this exact part, once a window-temperature probe closes the calibration and separates transmission from the window's self-emission.

Compiled by Eggert Gudmundsson. Subset of coap_GridEye/LITERATURE.md. Local copies not re-hosted. Updated 2026-09-01.