Notes adapted from Prof. P. Lewis [email protected]

38
UCL DEPARTMENT OF GEOGRAPHY UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Radiative Transfer Theory at optical wavelengths applied to vegetation canopies: part 1 Notes adapted from Prof. P. Lewis [email protected] Dr. Mathias (Mat) Disney UCL Geography Office: 113, Pearson Building Tel: 7679 0592 Email: [email protected] http://www2.geog.ucl.ac.uk/~mdisney/teaching/GEOGG141/GEOGG141. html http://www2.geog.ucl.ac.uk/~mdisney/teaching/3051/GEOG3051.html

description

GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Radiative Transfer Theory at o ptical wavelengths applied to vegetation canopies: part 1. Notes adapted from Prof. P. Lewis [email protected]. Dr. Mathias (Mat) Disney UCL Geography Office: 113, Pearson Building - PowerPoint PPT Presentation

Transcript of Notes adapted from Prof. P. Lewis [email protected]

Page 1: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHYUCL DEPARTMENT OF GEOGRAPHY

GEOGG141/ GEOG3051Principles & Practice of Remote Sensing (PPRS)Radiative Transfer Theory at optical wavelengths applied to vegetation canopies: part 1

Notes adapted from Prof. P. Lewis [email protected]

Dr. Mathias (Mat) DisneyUCL GeographyOffice: 113, Pearson BuildingTel: 7679 0592Email: [email protected]://www2.geog.ucl.ac.uk/~mdisney/teaching/GEOGG141/GEOGG141.htmlhttp://www2.geog.ucl.ac.uk/~mdisney/teaching/3051/GEOG3051.html

Page 2: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Aim of this section

• Introduce RT approach as basis to understanding optical and microwave vegetation response

• enable use of models• enable access to literature

Page 3: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Scope of this section

• Introduction to background theory– RT theory– Wave propagation and polarisation– Useful tools for developing RT

• Building blocks of a canopy scattering model– canopy architecture– scattering properties of leaves– soil properties

Page 4: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Reading

Full notes for these lectureshttp://www2.geog.ucl.ac.uk/~mdisney/teaching/GEOGG141/rt_theory/rt_notes1.pdf http://www2.geog.ucl.ac.uk/~mdisney/teaching/GEOGG141/rt_theory/rt_notes2.pdf

BooksJensen, J. (2007) Remote Sensing: an Earth Resources Perspective, 2nd ed., Chapter 11 (355-408), 1st ed chapter 10.Liang, S. (2004) Quantitative Remote Sensing of Land Surfaces, Wiley, Chapter 3 (76-142).Monteith, J. L. and Unsworth, M. H. (1990) Principles of Environmental Physics, 2nd ed., ch 5 & 6.

PapersFeret, J-B. et al. (2008) PROSPECT-4 and 5: Advances in the leaf optical properties model separating photosynthetic pigments, RSE, 112, 3030-3043.Jacquemoud. S. and Baret, F. (1990) PROSPECT: A model of leaf optical properties spectra, RSE, 34, 75-91.Nilson, T. and Kuusk, A. (1989) A canopy reflectance model for the homogeneous plant canopy and its inversion, RSE, 27, 157-167.Price, J. (1990), On the information content of soil reflectance spectra RSE, 33, 113-121Walthall, C. L. et al. (1985) Simple equation to approximate the bidirectional reflectance from vegetative canopies and bare soil surfaces, Applied Optics, 24(3), 383-387.

Page 5: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Why build models?

• Assist data interpretation• calculate RS signal as fn. of biophysical variables

• Study sensitivity• to biophysical variables or system parameters

• Interpolation or Extrapolation• fill the gaps / extend observations

• Inversion• estimate biophysical parameters from RS

• aid experimental design• plan experiments

Page 6: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Page 7: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Radiative Transfer Theory

• Applicability– heuristic treatment

• consider energy balance across elemental volume– assume:

• no correlation between fields– addition of power not fields

• no diffraction/interference in RT– can be in scattering

– develop common (simple) case here

Page 8: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Radiative Transfer Theory

• Case considered:– horizontally infinite but vertically finite plane

parallel medium (air) embedded with infinitessimal oriented scattering objects at low density

– canopy lies over soil surface (lower boundary)– assume horizontal homogeneity

• applicable to many cases of vegetation• But…..?

Page 9: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Building blocks for a canopy model

• Require descriptions of:– canopy architecture– leaf scattering– soil scattering

Page 10: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Canopy Architecture• 1-D: Functions of depth from the top of the canopy (z).

Page 11: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Canopy Architecture

• 1-D: Functions of depth from the top of the canopy (z).

1. Vertical leaf area density (m2/m3)2. the leaf normal orientation distribution function

(dimensionless).3. leaf size distribution (m)

Page 12: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Canopy Architecture

• Leaf area / number density– (one-sided) m2 leaf per m3

LAI

Page 13: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Canopy Architecture

• Leaf Angle Distribution

Page 14: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

• Archetype Distributions:· planophile

· erectophile

· spherical

· plagiophile

· extremophile

Leaf Angle Distribution

Page 15: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

• Archetype Distributions:

Leaf Angle Distribution

Page 16: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

• RT theory: infinitesimal scatterers– without modifications (dealt with later)

• In optical, leaf size affects canopy scattering in retroreflection direction– ‘roughness’ term: ratio of leaf linear dimension to canopy

height

also, leaf thickness effects on reflectance /transmittance

Leaf Dimension

Page 17: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Canopy element and soil spectral properties

• Scattering properties of leaves– scattering affected by:

• Leaf surface properties and internal structure; • leaf biochemistry; • leaf size (essentially thickness, for a given LAI).

Excellent review here:http://www.photobiology.info/Jacq_Ustin.html

Page 18: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Scattering properties of leaves

• Leaf surface properties and internal structure

opticalSpecular

from surface

Smooth (waxy) surface- strong peak

hairs, spines- more diffused

Page 19: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Scattering properties of leaves

• Leaf surface properties and internal structure

opticalDiffused

from scattering at internal air-cell wall interfaces

Depends on total areaof cell wall interfaces

Depends on refractive index:varies: 1.5@400 nm

1.3@2500nm

Page 20: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Scattering properties of leaves

• Leaf surface properties and internal structure

optical

More complex structure (or thickness):- more scattering- lower transmittance- more diffuse

Page 21: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Scattering properties of leaves

• Leaf biochemstry

Page 22: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Scattering properties of leaves• Leaf biochemstry

Feret, Jacquemoud et al. (2008) PROSPECT-4 and 5: Advances in the leaf optical properties model separating photosynthetic pigments, RSE, 112, 3030-3043.

Page 23: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Scattering properties of leaves• Leaf biochemstry

Feret, Jacquemoud et al. (2008) PROSPECT-4 and 5: Advances in the leaf optical properties model separating photosynthetic pigments, RSE, 112, 3030-3043.

Page 24: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Scattering properties of leaves• Leaf biochemstry

Feret, Jacquemoud et al. (2008) PROSPECT-4 and 5: Advances in the leaf optical properties model separating photosynthetic pigments, RSE, 112, 3030-3043.

Page 25: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHYScattering properties of leaves

• Leaf water

Feret, Jacquemoud et al. (2008) PROSPECT-4 and 5: Advances in the leaf optical properties model separating photosynthetic pigments, RSE, 112, 3030-3043.

Page 26: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Scattering properties of leaves• Leaf biochemstry

– pigments: chlorophyll a and b, a-carotene, and xanthophyll • absorb in blue (& red for chlorophyll)

– absorbed radiation converted into:• heat energy, flourescence or carbohydrates through

photosynthesis

Page 27: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Scattering properties of leaves• Leaf biochemstry

– Leaf water is major consituent of leaf fresh weight,• around 66% averaged over a large number of leaf types

– other constituents ‘dry matter’• cellulose, lignin, protein, starch and minerals

– Absorptance constituents increases with concentration• reducing leaf reflectance and transmittance at these

wavelengths.

Page 28: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Scattering properties of leaves

• Optical Models– flowering plants: PROSPECT – a generalised

plate model

Figure from: http://teledetection.ipgp.jussieu.fr/opticleaf/models.htm & see for more detail on various approaches to leaf optical properties modelling

Jacquemoud. S. and Baret, F. (1990) PROSPECT: A model of leaf optical properties spectra, RSE, 34, 75-91.

Page 29: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Scattering properties of leaves

• Optical Models– flowering plants: PROSPECT – extension of plate

model to N layers

http://teledetection.ipgp.jussieu.fr/opticleaf/models.htm

Page 30: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Scattering properties of leaves• leaf dimensions

– optical• increase leaf area for constant number of leaves -

increase LAI• increase leaf thickness - decrease transmittance

(increase reflectance)

Page 31: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Scattering properties of soils

• Optical and microwave affected by:– soil moisture content

– Wetter soils are darker (optical); have lower dielectric (microwave)

– soil type/texture– soil surface roughness

– shadowing (optical)– coherent scattering (microwave)

Page 32: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

soil moisture content• Optical

– effect essentially proportional across all wavelengths• enhanced in water absorption bands

Page 33: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY soil texture/type

• Optical– relatively little variation in spectral

properties– Price (1990):

• PCA on large soil database - 99.6% of variation in 4 PCs

– Stoner & Baumgardner (1982) defined 5 main soil types:• organic dominated• minimally altered• iron affected• organic dominated• iron dominated

Price, J. (1990), On the information content of soil reflectance spectra RSE, 33, 113-121.

Page 34: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Soil roughness effects

• Affects directional properties of reflectance (optical particularly)

• Simple models:– as only a boundary condition, can sometimes use simple

models• e.g. Lambertian• e.g. trigonometric (Walthall et al., 1985; Nilson and Kuusk 1990)

where θv,i are the view and illumination (sun) zenith angles; ϕ is relative azimuth angle (ϕi - ϕv).

Page 35: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY Soil roughness effects

• Rough roughness:– optical surface scattering

• clods, rough ploughing– use Geometric Optics model (Cierniewski)– projections/shadowing from protrusions

Page 36: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHYSoil roughness effects

• Rough roughness:– optical surface scattering

• Note backscatter reflectance peak (‘hotspot’)• minimal shadowing• backscatter peak width increases with increasing roughness

Page 37: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHYSoil roughness effects

• Rough roughness:– volumetric scattering

• consider scattering from ‘body’ of soil– particulate medium– use RT theory (Hapke - optical)– modified for surface effects (at different scales of roughness)

Page 38: Notes adapted from Prof. P. Lewis  plewis@geog.ucl.ac.uk

UCL DEPARTMENT OF GEOGRAPHY

Summary

• Introduction– Examined rationale for modelling– discussion of RT theory– Scattering from leaves

• Canopy model building blocks– canopy architecture: area/number, angle, size– leaf scattering: spectral & structural– soil scattering: roughness, type, water