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UCL DEPARTMENT OF GEOGRAPHY UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling 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/GEOGG1 41.html http://www2.geog.ucl.ac.uk/~mdisney/teaching/3051/GEOG3051.h tml

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Page 1: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHYUCL DEPARTMENT OF GEOGRAPHY

GEOGG141/ GEOG3051Principles & Practice of Remote Sensing (PPRS)Angular, temporal, radiometric resolution, sampling

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

Page 2: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Previously introduced– spatial and spectral resolution– narrow v broad band tradeoffs....– signal to noise ratio

• This session– temporal and angular sampling and/or resolution– REMEMBER: sampling NOT same as resolution, but

sometimes used interchangeably– orbits and sensor swath– radiometric resolution

2

Recap

Page 3: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Single or multiple observations• How far apart are observations in time?

– One-off, several or many?

• Depends (as usual) on application– Is it dynamic?– If so, over what timescale?

3

Temporal sampling/resolution

Useful link: http://nasascience.nasa.gov/earth-science

Page 4: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Examples– Vegetation stress monitoring, weather, rainfall

• hours to days– Terrestrial carbon, ocean surface temperature

• days to months to years– Glacier dynamics, ice sheet mass balance, erosion/tectonic

processes• Months to decades

4

Temporal

Useful link: http://nasascience.nasa.gov/earth-science

Page 5: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Sensor orbit– geostationary orbit - over same spot

• BUT distance means entire hemisphere is viewed e.g. METEOSAT

– polar orbit can use Earth rotation to view entire surface

• Sensor swath– Wide swath allows more rapid revisit

• typical of moderate res. instruments for regional/global applications– Narrow swath == longer revisit times

• typical of higher resolution for regional to local applications

5

What determines temporal sampling?

Page 6: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Orbital characteristics – orbital mechanics developed by Johannes Kepler (1571-1630),

German mathematician– Explained observations of Danish nobleman Tyco Brahe (1546-

1601)– Kepler favoured elliptical orbits (from Copernicus’ solar-centric

system)

• Properties of ellipse?

6

Orbits and swaths

Page 7: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Flattened circle – 2 foci and 2 axes: major and minor– Distance r1+r2 = constant = 2a (major axis)

– “Flatness” of ellipse defined by eccentricity, e = 1-b2/a2 = c/a– i.e. e is position of the focus as a fraction of the semimajor axis, a

7

Ellipse

From http://mathworld.wolfram.com/Ellipse.html

Increasing eccentricity

• ecircle = 0

• As e 1, c a and ellipse becomes flatter

r1 r2

f1 f2C

2a

2c

2b

major axis

minor axis

Page 8: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Kepler’s Laws – deduced from Brahe’s data after his death– see nice Java applet

http://www-groups.dcs.st-and.ac.uk/~history/Java/Ellipse.html

• Kepler’s 1st law: – Orbits of planets are elliptical, with sun at one focus

8

Kepler’s laws

From:http://csep10.phys.utk.edu/astr161/lect/history/kepler.html

Page 9: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Kepler’s 2nd law – line joining planet to sun sweeps out equal areas in equal times

9

Kepler’s laws

From:http://csep10.phys.utk.edu/astr161/lect/history/kepler.html

Page 10: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Kepler’s 3rd law – “ratio of the squares of the revolutionary periods for two planets (P1,

P2) is equal to the ratio of the cubes of their semimajor axes (R1, R2)”

– P12/P2

2 = R13/R2

3

• i.e. orbital period increases dramatically with R

• Convenient unit of distance is average separation of Earth from Sun = 1 astronomical unit (A.U.)– 1A.U. = 149,597,870.691 km– in Keplerian form, P(years)2 R(A.U.)3

– or P(years) R(A.U.)3/2

– or R(A.U.) P(years)2/3

10

Kepler’s laws

Page 11: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Orbital period for a given instrument and height? – Gravitational force Fg = GMEms/RsE

2

• G is universal gravitational constant (6.67x10-11 Nm2kg2); ME is Earth mass (5.983x1024kg); ms is satellite mass (?) and RsE is distance from Earth centre to satellite i.e. 6.38x106 + h where h is satellite altitude

– Centripetal (not centrifugal!) force Fc = msvs2/RsE

• where vs is linear speed of satellite (=sRsE where is the satellite angular velocity, rad s-1)

– for stable (constant radius) orbit Fc = Fg

– GMEms/RsE2 = msvs

2/RsE = ms s2RsE

2 /RsE

– so s2 = GME /RsE

3

11

Orbits: examples

Page 12: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Orbital period T of satellite (in s) = 2/– (remember 2 = one full rotation, 360°, in radians)– and RsE = RE + h where RE = 6.38x106 m

– So now T = 2[(RE+h)3/GME]1/2

• Example: polar orbiter period, if h = 705x103m– T = 2[(6.38x106 +705x103)3 / (6.67x10-11*5.983x1024)]1/2

– T = 5930.6s = 98.8mins

• Example: altitude for geostationary orbit? T = ??– Rearranging: h = [(GME /42)T2 ]1/3 - RE

– So h = [(6.67x10-11*5.983x1024 /42)(24*60*60)2 ]1/3 - 6.38x106

– h = 42.2x106 - 6.38x106 = 35.8x106m

12

Orbits: examples

Page 13: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Convenience of using radians– By definition, angle subtended by an arc (in radians) = length of

arc/radius of circle i.e. = l/r– i.e. length of an arc l = r– So if we have unit circle (r=1), l = circumference = 2r = 2– So, 360° = 2 radians

13

Orbits: aside

r

l

Page 14: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Geostationary? – Circular orbit in the equatorial plane, altitude ~36,000km– Orbital period?

• Advantages– See whole Earth disk at once due to large distance– See same spot on the surface all the time i.e. high temporal coverage– Big advantage for weather monitoring satellites - knowing atmos.

dynamics critical to short-term forecasting and numerical weather prediction (NWP)

• GOES (Geostationary Orbiting Environmental Satellites), operated by NOAA (US National Oceanic and Atmospheric Administration)

• http://www.noaa.gov/ and http://www.goes.noaa.gov/

14

Orbital pros and cons

Page 15: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Meteorological satellites - combination of GOES-E, GOES-W, METEOSAT (Eumetsat), GMS (NASDA), IODC (old Meteosat 5)– GOES 1st gen. (GOES-1 - ‘75 GOES-7 ‘95); 2nd gen. (GOES-8++ ‘94)

15

Geostationary

From http://www.sat.dundee.ac.uk/pdusfaq.html

METEOSAT 0° WGOES-W 135° WGOES-E 75° W GMS 140° EIODC 63° E

Page 16: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• METEOSAT - whole earth disk every 15 mins

16

Geostationary

From http://www.goes.noaa.gov/f_meteo.html

Page 17: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Disadvantages– typically low spatial resolution due to high altitude– e.g. METEOSAT 2nd Generation (MSG) 1x1km visible, 3x3km IR

(used to be 3x3 and 6x6 respectively)• MSG has SEVIRI and GERB instruments• http://www.eumetsat.int/Home/Main/What_We_Do/Satellites/

Meteosat_Second_Generation/Space_Segment/SP_1119959405658?l=en– Cannot see poles very well (orbit over equator)

• spatial resolution at 60-70° N several times lower• not much good beyond 60-70°

– NB Geosynchronous orbit same period as Earth, but not equatorial

17

Geostationary orbits

From http://www.esa.int/SPECIALS/MSG/index.html

Page 18: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Advantages– full polar orbit inclined 90 to equator

• typically few degrees off so poles not covered• orbital period typically 90 - 105mins

– near circular orbit between 300km (low Earth orbit) and 1000km– typically higher spatial resolution than geostationary– rotation of Earth under satellite gives (potential) total coverage

• ground track repeat typically 14-16 days

18

Polar & near polar orbits

From http://collections.ic.gc.ca/satellites/english/anatomy/orbit/

Page 19: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

19

(near) Polar orbits: NASA Terra

From http://visibleearth.nasa.gov/cgi-bin/viewrecord?134

Page 20: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

– inclination 98.2, T = 98.8mins– http://www.cscrs.itu.edu.tr/page.en.php?id=51– http://landsat.gsfc.nasa.gov/project/Comparison.html

20

Near-polar orbits: Landsat

From http://www.iitap.iastate.edu/gccourse/satellite/satellite_lecture_new.html & http://eosims.cr.usgs.gov:5725/DATASET_DOCS/landsat7_dataset.html

• ASIDE: repeat time

• Orbital period is 5928s

• So in this time Earth surface moves l = r = r*(2*5928/(24*60*60))

• So if r = 6.38x106 then l = 2750km

Page 21: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Disadvantages– need to launch to precise altitude and orbital inclination– orbital decay

• at LEOs (Low Earth Orbits) < 1000km, drag from atmosphere• causes orbit to become more eccentric• Drag increases with increasing solar activity (sun spots) - during solar

maximum (~11yr cycle) drag height increased by 100km!– Build your own orbit:

http://lectureonline.cl.msu.edu/~mmp/kap7/orbiter/orbit.htm

21

(near) Polar orbits

From http://collections.ic.gc.ca/satellites/english/anatomy/orbit/

Page 22: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Sun-synchronous– Passes over same point on surface at approx. same local solar time

each day (e.g. Landsat)– Characterised by equatorial crossing time (Landsat ~ 10am)– Gives standard time for observation– AND gives approx. same sun angle at each observation

• good for consistent illumination of observations over time series (i.e. Observed change less likely to be due to illumination variations)

• BAD if you need variation of illumination (angular reflectance behaviour)

• Special case is dawn-to-dusk– e.g. Radarsat 98.6° inclination– trails the Earth’s shadow (day/night border)– allows solar panels to be kept in sunlight all the time)

22

Types of near-polar orbit

Page 23: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Inclination much lower– orbits close to equatorial– useful for making observations solely over tropical regions

• Example– TRMM - Tropical Rainfall Measuring Mission– Orbital inclination 35.5°, periapsis (near point: 366km), apoapsis (far point:

3881km)– crosses equator several times daily– Flyby of Hurrican Frances (24/8/04)– iso-surface

23

Near-ish: Equatorial orbit

From http://trmm.gsfc.nasa.gov/

Page 24: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• TLEs (two line elements)– http://www.satobs.org/element.html e.g.

PROBA 1

1 26958U 01049B 04225.33423432 .00000718 00000-0 77853-4 0 2275

2 26958 97.8103 302.9333 0084512 102.5081 258.5604 14.88754129152399

• DORIS, GPS, Galileo etc.– DORIS: Doppler Orbitography and Radiopositioning Integrated by Satellite– Tracking system providing range-rate measurements of signals from a dense

network of ground-based beacons (~cm accuracy)– GPS: Global Positioning System– http://www.vectorsite.net/ttgps.html– http://www.edu-observatory.org/gps/tracking.html

24

Orbital location?

Page 25: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Swath describes ground area imaged by instrument during overpass

25

Instrument swath

one sample

two samples

three samples

satellite ground swath

direction of travel

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UCL DEPARTMENT OF GEOGRAPHY

26

MODIS on-board Terra

From http://visibleearth.nasa.gov/cgi-bin/viewrecord?130

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UCL DEPARTMENT OF GEOGRAPHY

27

Terra instrument swaths compared

From http://visibleearth.nasa.gov/Sensors/Terra/

Page 28: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• MODIS, POLDER, AVHRR etc.– swaths typically several 1000s of km– lower spatial resolution– Wide area coverage– Large overlap obtains many more view and illumination angles

(much better termporal & angular (BRDF) sampling)– Rapid repeat time

28

Broad swath

Page 29: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Note across-track “whiskbroom” type scanning mechanism• swath width of 2330km (250-1000m resolution)• Hence, 1-2 day repeat cycle

29

MODIS: building global view

From http://visibleearth.nasa.gov/Sensors/Terra/

Page 30: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• 2400km swath, 1.1km pixels at nadir, but > 5km at edge of swath• Repeats 1-2 times per day

30

AVHRR: global view

From http://edc.usgs.gov/guides/avhrr.html

Page 31: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

31

POLDER (RIP!): global view

From http://www-loa.univ-lille1.fr/~riedi/BROWSES/200304/16/index.html

• Polarisation and Directionality of Earth’s Reflectance– FOV ±43° along track, ±51° across track, 9 cameras, 2400km swath, 7x6km

resn. at nadir– POLDER I 8 months, POLDER II 7 months....

Each set of points corresponds to given viewing zenith and azimuthal angles for near-simultaneous measurements over a region defined by lat 0°±0.5° and long of 0°±0.5° (Nov 1996)

Each day, region is sampled from different viewing directions so hemisphere is sampled heavily by compositing measurements over time

From Loeb et al. (2000) Top-of-Atmosphere Albedo Estimation from Angular Distribution Models Using Scene Identification from Satellite Cloud Property Retrievals, Journal of Climate, 1269-1285.

Page 32: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Landsat TM/MSS/ETM+, IKONOS, QuickBird etc.– swaths typically few 10s to 100skm– higher spatial resolution– local to regional coverage NOT global– far less overlap (particularly at lower latitudes)– May have to wait weeks/months for revisit

32

Narrow swath

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UCL DEPARTMENT OF GEOGRAPHY

33

Landsat: regional to local view

From http://visibleearth.nasa.gov/Sensors/Terra/

• 185km swath width, hence 16-day repeat cycle (and spatial res. 25m)

• Contiguous swaths overlap (sidelap) by 7.3% at the equator

• Much greater overlap at higher latitudes (80% at 84°)

Page 34: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

34

IKONOS, QuickBird, WorldView: very local view!

• QuickBird: 16.5km swath at nadir, 61cm! panchromatic, 2.44m multispectral

• http://www.digitalglobe.com

• IKONOS: 11km swath at nadir, 1m panchromatic, 4m multispectral

• http://www.spaceimaging.com/

Page 35: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• ERS 1 & 2– ATSR instruments, RADAR altimeter, Imaging SAR (synthetic aperture

RADAR) etc. – ERS 1: various mission phases: repeat times of 3 (ice), 35 and 168

(geodyssey) days– ERS 2: 35 days

35

Variable repeat patterns

From http://earth.esa.int/rootcollection/eeo/ERS1.1.7.html

Page 36: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Wide swath instruments have large overlap– e.g. MODIS 2330km (55), so up to 4 views per day at different

angles! – AVHRR, SPOT-VGT, POLDER I and II, etc.– Why do we want good angular sampling?

• Remember BRDF?• See Barnsley et al (1997) paper

– Information in angular signal we can exploit!– Or remove BRDF effects when combining observations from different

times/angles– More samples of viewing/illum. hemisphere gives more info.

36

So.....angular resolution

Page 37: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Can look like noise over time BUT plotted as a function of angle we see BRDF effect

• So must account for BRDF if we want to look at changes over time

37

Angular (BRDF) effects

Page 38: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• MODIS and SPOT-VGT: polar plots– http://www.soton.ac.uk/~epfs/methods/polarplot.shtml

• Reasonable sampling BUT mostly across principal plane (less angular info.)• Is this “good” sampling of BRDF

38

Angular sampling: broad swath

Solar principal plane

Cross solar principal plane

view zenith

relative azimuth (view - solar)

Page 39: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• POLDER I !• Broad swath (2200km) AND

large 2D CCD array gave huge number of samples– 43 IFOV along-track and

51 IFOV across-track

39

Angular sampling: broad swath

Page 40: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Is wide swath angular sampling REALLY multi-angular?– Different samples on different days e.g. MODIS BRDF product is

composite over 16 days– minimise impact of clouds, maximise number of samples

• “True” multi-angular viewing requires samples at same time– need to use several looks e.g. ATSR, MISR (& POLDER)

40

BUT.......

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UCL DEPARTMENT OF GEOGRAPHY

41

Angular sampling: narrow swath

• ATSR-2 and MISR polar plots• Better sampling in principal plane (more angular info.)• MISR has 9 cameras

Page 42: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

42

Angular sampling: combinations?

• MODIS AND MISR: better sampling than either individually• Combine observations to sample BRDF more effectively

Page 43: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Function of swath and IFOV – e.g. MODIS at nadir ~1km pixel – remember l = r so angle (in rads) = r/l where r this time is 705km

and l ~ 1km so angular res ~ 1.42x10-6 rads at nadir– at edge of swath ~5km pixel so angular res ~ 7x10-6 rads

• SAMPLING more important/meaningful than resolution in angular sense (as for temporal)

43

So, angular resolution

Page 44: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Had spatial, spectral, temporal, angular.....• Precision with which an instrument records EMR

– i.e. Sensitivity of detector to amount of incoming radiation– More sensitivity == higher radiometric resolution

• determines smallest slice of EM spectrum we can assign DN to– BUT higher radiometric resolution means more data

• As is the case for spatial, temporal, angular etc.

• Typically, radiometric resolution refers to digital detectors– i.e. Number of bits per pixel used to encode signal

44

Radiometric resolution

Page 45: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Analogue– continuous measurement levels– film cameras– radiometric sensitivity of film emulsion

• Digital– discrete measurement levels– solid state detectors (e.g. semiconductor CCDs)

45

Radiometric resolution

Page 46: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Bits per pixel– 1 bit (0,1); 2bits (0, 1, 2, 3); 3 bits (0, 1, 2, 3, 4, 5, 6, 7) etc.– 8 bits in a byte so 1 byte can record 28 (256) different DNs (0-255)

46

Radiometric resolution

• 1 to 6 bits (left to right)– black/white (21) up to 64 graylevels (26) (DN values)– human eye cannot distinguish more than 20-30 DN levels in grayscale

i.e. ‘radiometric resolution’ of human eye 4-5 bits

From http://ceos.cnes.fr:8100/cdrom/ceos1/irsd/pages/dre4.htm

Page 47: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Landsat: MSS 7bits, TM 8bits• AVHRR: 10-bit (210 = 1024 DN levels)

– TIR channel scaled (calibrated) so that DN 0 = -273°C and DN 1023 ~50°C

• MODIS: 12-bit (212 = 4096 DN levels)• BUT precision is NOT accuracy

– can be very precise AND very inaccurate– so more bits doesn’t mean more accuracy

• Radiometric accuracy designed with application and data size in mind – more bits == more data to store/transmit/process

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Radiometric resolution: examples

Page 48: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Coverage (hence angular &/or temporal sampling) due to combination of orbit and swath– Mostly swath - many orbits nearly same

• MODIS and Landsat have identical orbital characteristics: inclination 98.2°, h=705km, T = 99mins BUT swaths of 2400km and 185km hence repeat of 1-2 days and 16 days respectively

– Most EO satellites typically near-polar orbits with repeat tracks every 16 or so days

– BUT wide swath instrument can view same spot much more frequently than narrow

• Tradeoffs again, as a function of objectives

48

Summary: angular, temporal resolution

Page 49: UCL DEPARTMENT OF GEOGRAPHY GEOGG141/ GEOG3051 Principles & Practice of Remote Sensing (PPRS) Angular, temporal, radiometric resolution, sampling Dr. Mathias

UCL DEPARTMENT OF GEOGRAPHY

• Number of bits per pixel– more bits, more precision (not accuracy)– but more data to store, transmit, process– most EO data typically 8-12 bits (in raw form)

• Tradeoffs again, as a function of objectives

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Summary: radiometric resolution