In this module we will learn about the gamut of thermal imaging. First we are going to learn about the across-track thermal scanning mechanism. Then we are going to learn about the thermal radiation principles, interpret thermal scanner imagery, analyse the geometric characteristics of across-track scanner imagery, temperature mapping with thermal scanner data, FLIR systems, and thermal scanners. We will know the radiant temperature, kinetic temperature, real body and black body radiations. We will learn about the geometric distortions found in thermal imagery. Then we will learn about thermal remote sensing, Planck Radiation Law, diurnal-heating effects, thermal properties of water, various thermal sensors. We will discuss heat capacity mapping mission and other weather satellites. Next we will learn what is hyperspectral remote sensing or understand the main concept of hyperspectral remote sensing, why it is necessary to find out certain subtle mineral composition of rocks, vegetation. We will discuss the usefulness of hyperspectral sensing in forestry applications and to understand the crown features and also we will learn some satellites carrying hyperspectral sensors. Finally the last topic we will study is the concept, fundamentals or principals of microwave remote sensing, the radar altimeter and microwave radiometer.
Thermal sensors generally have large IFOVs to ensure enough energy reaches the detector to make a reliable measurement, so the spatial resolution is usually fairly coarse
Civilian use of FLIR is increasing in applications such as firefighting, electrical transmission line maintenance, law enforcement, and nighttime vision for automobiles
The rate of flow of electromagnetic energy, commonly measured in Watts per square meter, emanating from a blackbody and related to its internal (kinetic) temperature Tk by the Stefan-Boltzmann Law
The radiant flux of a real (or 'greybody') material, which is always less than the blackbody flux FB, as calculated by FR = εσTk4, where ε is the emissivity
The resistance of a material to temperature change, indicated by the time dependent variations in temperature during a full heating/cooling cycle, defined as P = (Kcρ)^(1/2) = cρ(k)^(1/2)
Interpretingthermal data and images is complex due to factors like material composition, insolation angle, emissivity, geothermal heat flux, topography, soil moisture, and vegetation
The distribution of temperature over an area is complex. In many instances, we must look for patterns of relative temperature differences rather than the absolute values, because of the many complex factors that make quantitative determinations difficult