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Thermal remote sensing BY Hariom Ahlawat

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Page 1: Thermal remote sensing BY Hariom Ahlawat
Page 2: Thermal remote sensing BY Hariom Ahlawat

TO ACQUINT THE CLASS WITH CONCEPTS OF THERMAL REMOTE SENSING

AIM

Page 3: Thermal remote sensing BY Hariom Ahlawat

INTRODUCTIONPRINCIPLES OF THERMAL REMOTE SENSINGTHERMAL SENSORSAPPLICATIONS

CONTENTS

Page 4: Thermal remote sensing BY Hariom Ahlawat

INTRODUCTION

Page 5: Thermal remote sensing BY Hariom Ahlawat

REMOTE SENSING

Remote sensing is an art and science of

acquiring info about an object of interest

without coming in physical contact with it.

Page 6: Thermal remote sensing BY Hariom Ahlawat

Thermal remote sensing is based on the measuring of EM radiation in the infrared region of spectrum.Most commonly used intervals are 3-5 micro-meter and 8-14 micro-meter

THERMAL REMOTE SENSING

Page 7: Thermal remote sensing BY Hariom Ahlawat

Thermal IR and atmospheric window

Landsat 7Band 7

Landsat 7Band 6

Thermal energy emitted from the Earth is trapped by CO2, H2O, and O3.Global Warming!

Page 8: Thermal remote sensing BY Hariom Ahlawat

CERES—Cloud-Earth Radiant Energy System

Page 9: Thermal remote sensing BY Hariom Ahlawat

PRINCIPLES OF THERMAL REMOTE

SENSING

Page 10: Thermal remote sensing BY Hariom Ahlawat

Electromagnetic Radiance (EMR)

EMR – Energy emitted by the objects of which absolute temperature is above zero.The magnitude and spectral range of the emitted EMR are governed by the material’s:

Temperature, andEmissivity

Page 11: Thermal remote sensing BY Hariom Ahlawat

Review of Radiation Laws

All objects at temperature above absolute 0oK emit (-273.59oC, -459.67oF)

Stefan-Boltzmann law: W = sT4 W-total emitted radiation

s-a constant, T-temperature in oK

The total emitted radiation from a blackbody is proportional to the fourth power of its absolute temperature

Page 12: Thermal remote sensing BY Hariom Ahlawat

Radiation Laws

► Wien's displacement law: l = 2,897.8/T l-peak wavelength, T-temperature in oK

► As temperature of objects increases, the wavelength of peak emittance becomes shorter

Page 13: Thermal remote sensing BY Hariom Ahlawat
Page 14: Thermal remote sensing BY Hariom Ahlawat

► Emissivity: e = M/Mb e-emissivity

M-emittance of a given object Mb-emittance of blackbody e = 1 (blackbody) e = 0 (whitebody, perfect reflector)

► The ratio between the emittance of a given object and that of blackbody at the same temperature

Radiation Laws

Page 15: Thermal remote sensing BY Hariom Ahlawat

Emissivity of Common Materials

Clear water 0.98-0.99Wet snow 0.98-0.99Human skin 0.97-0.99Rough ice 0.97-0.98Vegetation 0.96-0.99Wet soil 0.95-0.98Asphalt concrete 0.94-0.97Brick 0.93-0.94Wood 0.93-0.94Basalt rock 0.92-0.96

Dry mineral soil 0.92-0.94paint 0.90-0.96Dry vegetation 0.88-0.94Dry snow 0.85-0.90Granite rock 0.83-0.87Glass 0.77-0.81Sheet iron (rusted) 0.63-0.70Polished metals 0.16-0.21Aluminum foil 0.03-0.07Highly polished gold 0.02-0.03

Page 16: Thermal remote sensing BY Hariom Ahlawat

Water, Ice and Snow

Water, ice, and snow generally have a high emissivity, 0.94 to 0.99, across the thermal infrared region. Snow is unusual in that it has a high reflectance in the solar (visible) region where most of the downwelling energy is during the day, and a very high emissivity in the thermal region.

Water

Ice

Snow

Page 17: Thermal remote sensing BY Hariom Ahlawat

Soil and Minerals

Soil, rocks, and Minerals show strong spectral features between 8 and 10 microns that depend on the grain size. Soil signature in the 3 to 5μm region depends on the water and organic content. The dryer, purer soils have lower emissivities in this region.

Page 18: Thermal remote sensing BY Hariom Ahlawat

Vegetation

Green vegetation typically has a very high emissivity because it contains water. Senescent (dry) vegetation has a more variable emissivity, especially in the 3 to 5μm region, which depends on the type and structure of the cover type, the dryness, etc.

Page 19: Thermal remote sensing BY Hariom Ahlawat

Man-made material

Manmade materials such as polished metals have among the lowest emissivity values, can be made less than 0.01 (better than 99% reflecting). “Rocky” materials such as asphalt and brick are high and range from 0.90 to 0.98

Page 20: Thermal remote sensing BY Hariom Ahlawat

(Wikipedia – Infrared)

Page 21: Thermal remote sensing BY Hariom Ahlawat

Thermal sensors

Page 22: Thermal remote sensing BY Hariom Ahlawat

TIROS (Television IR Operational Satellite), launched in 1960GOES (Geostationary Operational Environmental Satellite), TIR at 8km spatial resolution, full-disk of Earth, day and nightHCMM (Heat Capacity Mapping Mission), launched in 1978- 600m spatial resolution, 10.5 – 12.6 micron rangeCZCS (Coastal Zone Color Scanner) on Nimbus 7, launched in 1978, for SST (sea surface temperature).AVHRR (Advanced Very High Resolution Radiometer), 1.1 and 4 km TIR bandsTIMS (Thermal Infrared Multispectral Scanner), Airborne, 6 bandsATLAS (Airborne Terrestrial Applications Sensor), 15 bandsLandsat 4,5,7; Band 6- 10.4 – 12.5 m, 120 m (4,5), 60 m (7).ASTER (Advanced Spaceborne Thermal Emission and Reflection Radiometer) on Terra, 5 bands 8.125-11.65 micron range (14 total)

THERMAL SENSORS

Page 23: Thermal remote sensing BY Hariom Ahlawat

Applications

Page 24: Thermal remote sensing BY Hariom Ahlawat

Application Areas

Surface temperature detectionCamouflage detectionFire detection and fire risk mappingEvapotranspiration and drought monitoringEstimating air temperatureOil spill monitoringWater quality monitoringVolcanic activity monitoringUrban heat island analysis

Page 25: Thermal remote sensing BY Hariom Ahlawat

Mars Hematite detected by TES

Page 26: Thermal remote sensing BY Hariom Ahlawat

24.0°F

43.0°F

25

30

35

40

Furnace Vent

Vent Duct

Typical IR imagery of Heat Loss in Residential Structures

Page 27: Thermal remote sensing BY Hariom Ahlawat

Energy Gain (Floor Leak)

Missing Insulation in Vaulted Ceiling Area

Moisture

Heat Loss Heat Loss

Page 28: Thermal remote sensing BY Hariom Ahlawat

37.3°F

46.6°F

38

40

42

44

46

Typical Institutional Building Heat Loss

37.3°F

46.6°F

38

40

42

44

46

37.7°F

50.9°F

38

40

42

44

46

48

50

28.5°F

54.5°F

30

35

40

45

50Typical Air Leak Patterns

37.7°F

50.9°F

38

40

42

44

46

48

50

Page 29: Thermal remote sensing BY Hariom Ahlawat

*>59.3°F

*<43.9°F

44.0

46.0

48.0

50.0

52.0

54.0

56.0

58.0

*>64.4°F

*<44.2°F

45.0

50.0

55.0

60.0

*>64.4°F

*<37.9°F

40.0

45.0

50.0

55.0

60.0 Air Leakagefrom non-insulated areas and window frames.

Page 30: Thermal remote sensing BY Hariom Ahlawat

Processing thermal images

Major issuesMoisture absorption in atmosphereMixed ground objects

Some visualization techniquesFalse color compositeLevel slicing

Page 31: Thermal remote sensing BY Hariom Ahlawat

Sea-surface temperature, June 22, 2000

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47

Ocean surface temperature from MODIS

Page 33: Thermal remote sensing BY Hariom Ahlawat

QUESTIONS PLEASE !!

Page 34: Thermal remote sensing BY Hariom Ahlawat

Thank You

Page 35: Thermal remote sensing BY Hariom Ahlawat

Thank You


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