CN101718866A - Improved physical method for topographic correction of remote sensing images - Google Patents

Improved physical method for topographic correction of remote sensing images Download PDF

Info

Publication number
CN101718866A
CN101718866A CN200910223585A CN200910223585A CN101718866A CN 101718866 A CN101718866 A CN 101718866A CN 200910223585 A CN200910223585 A CN 200910223585A CN 200910223585 A CN200910223585 A CN 200910223585A CN 101718866 A CN101718866 A CN 101718866A
Authority
CN
China
Prior art keywords
radiation
domatic
cos
solar
pixel
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
CN200910223585A
Other languages
Chinese (zh)
Other versions
CN101718866B (en
Inventor
张兆明
何国金
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
CENTER FOR EARTH OBSERVATION AND DIGITAL EARTH CHINESE ACADEMY OF SCIENCES
Original Assignee
CENTER FOR EARTH OBSERVATION AND DIGITAL EARTH CHINESE ACADEMY OF SCIENCES
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by CENTER FOR EARTH OBSERVATION AND DIGITAL EARTH CHINESE ACADEMY OF SCIENCES filed Critical CENTER FOR EARTH OBSERVATION AND DIGITAL EARTH CHINESE ACADEMY OF SCIENCES
Priority to CN 200910223585 priority Critical patent/CN101718866B/en
Publication of CN101718866A publication Critical patent/CN101718866A/en
Application granted granted Critical
Publication of CN101718866B publication Critical patent/CN101718866B/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Landscapes

  • Image Processing (AREA)

Abstract

The invention relates to an improved physical method for topographic correction of remote sensing images, which considers the influence of the topography on incident irradiance and earth surface reflectivity received by the sloping surface, more accurately computes sky radiation received by the sloping surface pixel, and meanwhile considers the influence of atmosphere during the topographic correction. The method of the invention can obtain the better result of the topographic correction; and the method belongs to the physical method, has universality and can be applied to various optical remote sensing images.

Description

A kind of improved physical method for topographic correction of remote sensing images
Technical field
The invention belongs to the remote sensing technology field, relate to the processing and the application of remotely-sensed data.
Background technology
In rugged mountain region, landform shows two aspects to the influence of satellite sensor received signal: the one, and the incident irradiance that influence of topography terrain object is received; The 2nd, topographic change the geometry that constituted of the sun, the face of land and satellite sensor three, and then have influence on the reflectivity of terrain object on the satellite sensor direction.Corresponding topographic correction also should comprise two parts, at first the built-up radiation that the surface level pixel is received is converted to the built-up radiation that domatic pixel receives, and (built-up radiation that domatic pixel received comprises three parts: the reflected radiation of beam radia, sky radiation and surrounding terrain to be called the correction of incident irradiance; Accordingly, the incident irradiance is proofreaied and correct and should be comprised that also beam radia is proofreaied and correct, sky radiation is proofreaied and correct and the reflected radiation of surrounding terrain is proofreaied and correct).Be the surface level reflectivity with domatic reflectivity conversion then, be called reflectivity correction.The influence of elimination or minimizing mountain area remote sensing image mesorelief factor is the inevitable requirement that improves the spectral reflectivity inversion accuracy.
Since the seventies in 20th century, Chinese scholars is just launched research at the orographic effect problem of remote sensing image, has proposed many topographic correction of remote sensing images methods, proofreaies and correct as cosine, and C proofreaies and correct, SCS bearing calibration etc.Wherein the most frequently used is the C landform correcting method of lane.But the obvious deficiency of C method is it to be supposed based on lambert's body, only considered that topographic relief receives the influence of incident irradiance to pixel, and it is a kind of empirical model, have subjectivity, the calibration model that obtains for different remote sensing images has nothing in common with each other, do not have versatility, this has just caused difficulty to its widespread use.Development along with the quantitative remote sensing technology, requirement to topographic correction is also more and more higher, this paper has proposed a kind of improved topographic correction of remote sensing images method on the basis of traditional landform correcting method of lane, the advantage of this method is that it has considered the influence of landform to incident irradiance and earth surface reflection rate simultaneously, calculated to degree of precision the sky radiation that domatic pixel received, in topographic correction, considered atmospheric effect, and it is a kind of physical model, have universality, be applicable to all optical remote sensing images.
Summary of the invention
The object of the present invention is to provide a kind of improved physical method for topographic correction of remote sensing images, to overcome the deficiency of existing landform correcting method of lane.Utilize this method can obtain better topographic correction effect, thereby promote the development of association area remote sensing application.
For achieving the above object, the improved topographic correction of remote sensing images method of the present invention's proposition is:
The first step, the sky radiation that utilizes beam radia that 6S radiation delivery Model Calculation surface level pixel received and surface level pixel to be received.
Second step, the beam radia that utilizes the domatic pixel of cosine correction calculation to receive.
The 3rd step, the sky radiation that receives by the domatic pixel of Perez (1990) Model Calculation.
The 4th step, the reflected radiation of calculating surrounding terrain.
The 5th the step, utilize 6S radiation delivery model that remote sensing image is carried out atmospheric correction.
Formula is converted to radiance on the star radiance of atmosphere bottom below the 6th step, the utilization.
L = L sat - L p - L env τ
The 7th step, to utilize Dymond (1999) formula be the surface level reflectivity with domatic reflectivity conversion, finishes topographic correction.
Embodiment
1. beam radia calculates
The beam radia that domatic pixel received can be obtained through the cosine calibration shift by the direct solar radiation that its corresponding surface level pixel is received, and concrete conversion formula is as follows:
E d = Θ E d h cos i cos z (formula 1)
In the formula: E dBe the beam radia that domatic pixel received, E d hBeam radia for the surface level pixel is received is obtained by the 6S model.I is domatic solar incident angle (angle of direct sunlight and domatic normal), and z is a solar zenith angle.Θ is the topographic shadowing coefficient, if domatic be shadow region (cosi<0), Θ is 0, otherwise is 1; Domatic solar incident angle i is obtained by formula (2):
(formula 2)
S is the angle of gradient of face of slope,
Figure G2009102235852D0000024
Be solar azimuth, A is the aspect of face of slope.Solar zenith angle and solar azimuth can be obtained by the image header file, and the domatic angle of gradient and aspect can be obtained by dem data.
2. sky radiation calculates
The sky radiation that the quantitative Analysis face of slope is received and the reflected radiation of surrounding terrain are often relatively more difficult, in a lot of topographic correction models, all do not consider the influence of these two factors.Document [high Yongnian, Zhang Wanchang. topographic correction of remote sensing images progress and comparative experiments thereof. Geographical Study, 2008,27 (2): 467-477.] calibration result to the different terrain bearing calibration compares analysis, found that the reflected radiation of considering sky radiation and surrounding terrain, the topographic correction effect is just better; Consider that not effect is then relatively poor.Therefore in order to improve the correction accuracy of topographic correction model, need the influence of the reflected radiation of consideration sky radiation and surrounding terrain.
Noorian [Noorian A M such as (2008), Moradi I, Kamali G A.Evaluation of 12 models to estimatehourly diffuse irradiation on inclined surfaces.Renewable Energy, 2008,33:1406-1412.] 12 kinds of sky radiation computation models have been carried out comparative study, and utilize the field survey data to verify.Found that Perez model [Perez R, Ineichen P, Seals R, et al.Modeling daylight availability and irradiance componentsfrom direct and global irradiance.Solar Energy, 1990,44 (5): 271-289.] conversion effect optimum, the present invention uses for reference the newest research results of Noorian (2008) etc., utilizes the Perez model to calculate the sky radiation that domatic pixel receives.
E f = E f h × { 0.5 × ( 1 - F 1 ) [ 1 + cos ( S ) ] + F 1 × ( a / b ) + F 2 × sin ( S ) } (formula 3)
A=max (0, cosi) (formula 4)
B=max (0.087, cos z) (formula 5)
E fBe the sky radiation that domatic pixel receives, E f hBe the sky radiation that the surface level pixel is received, obtain by the 6S modeling.A and b are intermediate variables.S is the angle of gradient of face of slope, and z and i are respectively solar zenith angle and domatic solar incident angle, F 1And F 2Be the coefficient that characterizes sky anisotropy degree, they are functions of weather condition.
F 1=F 11+ F 12* Δ+F 13* z (formula 6)
F 2=F 21+ F 22* Δ+F 23* z (formula 7)
Δ is a sky brightness, calculates by formula (8),
Δ = E f h × m / E 0 (formula 8)
E 0It is the exosphere solar irradiance, m is relative atm number [Kasten F.A new table and approximate formula forrelative optical air mass.Archives of Meteorology Geophysics and Bioclimatology SeriesB, 1966,14 (2): 206-223.]
M=[cos z+0.15 * (93.885-z) -1.253] -1(formula 9)
F 11, F 12, F 13And F 21, F 22, F 23Table look-up according to sky sharpness (μ) and to obtain, sky sharpness (μ) is pressed following formula and is determined [Perez R, Ineichen P, Seals R, et al.Modeling daylight availability and irradiance components from direct andglobal irradiance.Solar Energy, 1990,44 (5): 271-289.]:
μ = [ ( E f h + E d h / cos z ) / E f h + 1.041 × z 3 ] / ( 1 + 1.041 × z 3 ) (formula 10)
E d hBe the beam radia that is received on the surface level, z is a solar zenith angle.
3. calculate the reflected radiation of surrounding terrain
Reflected radiation (the E of surrounding terrain a) calculate [Sandmeier S according to following formula, Itten K I.A physically-based modelto correct atmospheric and illumination effects in optical satellite data of rugged terrain.IEEETransactions on Geoscience and Remote Sensing, 1997,35 (3): 708-717.]:
E a=E h* ρ Mean* V t(formula 11)
E wherein hBe the solar global irradiance (E that surface level received d hAnd E f hSum), ρ MeanThe average reflectance of expression surrounding terrain, the average reflectance of the image behind the 6S atmospheric correction of learning from else's experience, V tBe the visible factor of landform, obtain by following formula:
V t = 1 - cos ( S ) 2 (formula 12)
S is the angle of gradient of face of slope.
4 topographic corrections
Based on earth surface reflection is anisotropic supposition, and topographic relief can cause the variation of the sun-face of land-sensor geometric relationship, thereby has changed the incident angle and the emergence angle of sunray, makes the reflectivity generation marked change of pixel.And for surface level, the incident angle of different pixels is identical with emergence angle, thereby the surface level reflectivity of similar atural object is identical.Therefore, in order to eliminate the influence of topographic relief, need be the surface level reflectivity with domatic reflectivity conversion to the pixel reflectivity.
Surface radiation brightness calculation formula through topographic correction is as follows:
L = ρ d E d + ρ f ( E f + E d ) π (formula 13)
Wherein, E d, E fAnd E aRepresent the reflected radiation of beam radia, sky radiation and the surrounding terrain of domatic pixel reception respectively.ρ dBe domatic reflectivity, ρ to direct solar radiation fBe domatic reflectivity to scattered radiation, L is the radiance of atmosphere bottom, is obtained by following formula:
L = L sat - L p - L env τ (formula 14)
L SatBe radiance on the star, can obtain L by the sensor radiation calibration pBe journey radiation, L EnvBe environmental radiation, τ is an atmosphere optical thickness, and back three can obtain from the 6S model.
[Dymond J R such as Dymond, Shepherd J D.Correction of the topographic effect in remote sensing.IEEE Transactions on Geoscience and Remote Sensing, 1999,37 (5): 2618-2620.] proposed following formula and considered the influence of landform the beam radia reflectivity:
ρ d h ρ d = cos ( i ) + cos ( e ) cos ( i h ) + cos ( e h ) (formula 15)
ρ dBe domatic reflectivity, ρ to direct solar radiation d hBe the reflectivity of surface level to direct solar radiation, i and e are respectively incident angle and the emergence angle of direct solar radiation on domatic, i hAnd e hBe respectively incident angle and the emergence angle of direct solar radiation on surface level.
Because the information major part that satellite sensor received derives from the reflection of the face of land to beam radia, the reflected radiation of sky radiation and surrounding terrain is relative less, and landform is also less to the influence of their reflectivity.In order to simplify calculating, suppose
Figure G2009102235852D0000045
So:
L = ρ d h E d / δ + ρ d h ( E f + E a ) π (formula 16)
δ = cos ( i ) + cos ( e ) cos ( i h ) + cos ( e h ) (formula 17)
Final computing formula through the earth surface reflection rate behind the topographic correction is:
ρ d h = πL E d / δ + E f + E a (formula 18)
The test of 5 topographic corrections
In the topographic correction test below, the inventive method and the C landform correcting method of lane of using always have been carried out comparative analysis.
Test figure is utilized the Landsat 5TM image of Beijing Mountainous Area of North on July 12nd, 2006, and the resolution of testing used DEM is 30 meters.
To the checking of landform calibration result, the present invention uses for reference two kinds of method for quantitatively evaluating commonly used in the practice, i.e. " correlativity of earth surface reflection rate and corresponding solar incident angle cosine " and " standard deviation ".Before the topographic correction, the earth surface reflection rate of pixel and the correlativity of solar incident angle cosine are obvious, and pixel earth surface reflection rate changes along with the variation of solar incident angle significantly.Through behind the topographic correction, if the influence that the solar incident angle that the earth surface reflection rate of pixel no longer is subjected to cause because of topographic relief changes, correlativity between them should weaken so, and correlativity is weak more, shows that the effect of topographic correction is good more.After passing through topographic correction in addition, the earth surface reflection rate value of similar atural object is more approaching, and atural object becomes more " homogeneous ", so standard deviation should reduce, and standard deviation is more little, shows that the effect of topographic correction is good more
In order to calculate the correlativity of earth surface reflection rate and corresponding solar incident angle cosine, with earth surface reflection rate image and the cosi image overlay before and after the topographic correction, picked at random sampled point then, then the slope of these sampled point equations of linear regression and related coefficient are represented the correlativity of earth surface reflection rate and cosi.Slope is big more, correlativity strong more (referring to that the earth surface reflection rate is subjected to influence that cosi changes greatly); Related coefficient is big more, and correlativity is strong more.
The correlativity (is example with TM the 4th wave band) as shown in table 1 of each face of land reflectivity and solar incident angle cosine cosi before and after the topographic correction:
The correlativity of each face of land reflectivity and cosi before and after table 1 topographic correction
The slope of linear equation Related coefficient
Before the topographic correction ??0.1415 ??0.61
After the inventive method is proofreaied and correct ??-0.0008 ??0.004
After the C bearing calibration is proofreaied and correct ??-0.0511 ??0.232
As can be seen from Table 1, utilize the inventive method to carry out topographic correction after, the correlativity between earth surface reflection rate and the cosi (slope and related coefficient) obviously weakens, and has shown the validity of the inventive method.After utilizing the C bearing calibration to proofread and correct, the correlativity between earth surface reflection rate and the cosi also obviously weakens, but slope and related coefficient show that greater than the inventive method the calibration result of the inventive method is better than the C bearing calibration.
In order further to verify the effect of topographic correction, on the TM image, choose forest sample district, add up the standard deviation (table 2) of topographic correction front and back TM the 4th wave band reflectivity then respectively.
Standard deviation relatively before and after table 2 topographic correction
Standard deviation
Before the topographic correction ??6.99
After the inventive method is proofreaied and correct ??4.38
After the C bearing calibration is proofreaied and correct ??5.01
A good landform correcting method of lane makes that the standard deviation of similar atural object reduces behind the topographic correction, the inventive method gained result has just in time verified this point, through behind the topographic correction, standard deviation obviously reduces, the inside that shows similar atural object diminishes, the actual state that more can reflect the face of land, and the standard deviation of the inventive method correspondence shows that less than the C bearing calibration calibration result of the inventive method is better than the C bearing calibration.

Claims (5)

1. an improved physical method for topographic correction of remote sensing images the steps include:
The first step, the sky radiation that utilizes beam radia that 6S radiation delivery Model Calculation surface level pixel received and surface level pixel to be received;
Second step, the beam radia that utilizes the domatic pixel of cosine correction calculation to receive;
The 3rd step, the sky radiation that receives by the domatic pixel of Perez (1990) Model Calculation;
The 4th step, the reflected radiation of calculating surrounding terrain;
The 5th the step, utilize 6S radiation delivery model that remote sensing image is carried out atmospheric correction;
Formula is converted to radiance on the star radiance of atmosphere bottom below the 6th step, the utilization;
L = L sat - L p - L env τ
The 7th step, to utilize Dymond (1999) formula be the surface level reflectivity with domatic reflectivity conversion, finishes topographic correction.
2. physical method for topographic correction as claimed in claim 1, wherein the concrete conversion formula in second step is as follows:
E d = Θ E d h cos i cos z
In the formula: E dBe the beam radia that domatic pixel received, E d hBeam radia for the surface level pixel is received is obtained by the 6S model; I is domatic solar incident angle, and z is a solar zenith angle, and Θ is the topographic shadowing coefficient, if domatic be the shadow region, Θ is 0, otherwise is 1; Domatic solar incident angle i is obtained by following formula:
S is the angle of gradient of face of slope,
Figure F2009102235852C0000014
Be solar azimuth, A is the aspect of face of slope, and solar zenith angle and solar azimuth can be obtained by the image header file, and the domatic angle of gradient and aspect can be obtained by dem data.
3. physical method for topographic correction as claimed in claim 2, wherein the detailed calculated process in the 3rd step is:
E f = E f h × { 0.5 × ( 1 - F 1 ) [ 1 + cos ( S ) ] + F 1 ( a / b ) + F 2 × sin ( S ) }
a=max(0,cosi)
b=max(0.087,cosz)
E fBe the sky radiation that domatic pixel receives, E f hBe the sky radiation that the surface level pixel is received, obtained by the 6S modeling that a and b are intermediate variables, S is the angle of gradient of face of slope, and z and i are respectively solar zenith angle and domatic solar incident angle, F 1And F 2Be the coefficient that characterizes sky anisotropy degree, they are functions of weather condition;
F 1=F 11+F 12×Δ+F 13×z
F 2=F 21+F 22×Δ+F 23×z
Δ is a sky brightness, calculates by following formula,
Δ = E f h × m / E 0
E 0Be the exosphere solar irradiance, m is relative atm number,
m=[cos?z+0.15×(93.885-z) -1.253] -1
F 11, F 12, F 13And F 21, F 22, F 23Tabling look-up according to sky sharpness (μ) obtains, and sky sharpness (μ) is pressed following formula and determined:
μ = [ ( E f h + E d h / cos z ) / E f h + 1.041 × z 3 ] / ( 1 + 1.041 × z 3 )
E d hBe the beam radia that is received on the surface level, z is a solar zenith angle.
4. physical method for topographic correction as claimed in claim 3, wherein the concrete computing formula in the 4th step is as follows:
E a=E h×ρ mean×V t
E wherein aThe reflected radiation of the surrounding terrain that receives for domatic pixel, E hSolar global irradiance (the E that is received for the surface level pixel d hAnd E f hSum), ρ MeanThe average reflectance of expression surrounding terrain, the average reflectance of the image behind the 6S atmospheric correction of learning from else's experience, V tBe the visible factor of landform, obtain by following formula:
V t = 1 - cos ( S ) 2
S is the angle of gradient of face of slope.
5. physical method for topographic correction as claimed in claim 4, wherein the detailed calculated process in the 7th step is:
L = ρ d E d + ρ f ( E f + E a ) π
Wherein, E d, E fAnd E aRepresent the reflected radiation of beam radia, sky radiation and the surrounding terrain of domatic pixel reception respectively, ρ dBe domatic reflectivity, ρ to direct solar radiation fBe domatic reflectivity to scattered radiation, L is the radiance of atmosphere bottom, is obtained by following formula:
L = L sat - L p - L env τ
L SatBe radiance on the star, can obtain L by the sensor radiation calibration pBe journey radiation, L EnvBe environmental radiation, τ is an atmosphere optical thickness, and back three can obtain from the 6S model;
Consider the influence of landform according to following formula to the beam radia reflectivity:
ρ d h ρ d = cos ( i ) + cos ( e ) cos ( i h ) + cos ( e h )
ρ dBe domatic reflectivity, ρ to direct solar radiation d hBe the reflectivity of surface level to direct solar radiation, i and e are respectively incident angle and the emergence angle of direct solar radiation on domatic, i hAnd e hBe respectively incident angle and the emergence angle of direct solar radiation on surface level.
Suppose So:
L = ρ d h E d / δ + ρ d h ( E f + E a ) π
δ = cos ( i ) + cos ( e ) cos ( i h ) + cos ( e h )
Final computing formula through the earth surface reflection rate behind the topographic correction is:
ρ d h = πL E d / δ + E f + E a
CN 200910223585 2009-11-24 2009-11-24 Improved physical method for topographic correction of remote sensing images Expired - Fee Related CN101718866B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN 200910223585 CN101718866B (en) 2009-11-24 2009-11-24 Improved physical method for topographic correction of remote sensing images

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN 200910223585 CN101718866B (en) 2009-11-24 2009-11-24 Improved physical method for topographic correction of remote sensing images

Publications (2)

Publication Number Publication Date
CN101718866A true CN101718866A (en) 2010-06-02
CN101718866B CN101718866B (en) 2012-09-05

Family

ID=42433468

Family Applications (1)

Application Number Title Priority Date Filing Date
CN 200910223585 Expired - Fee Related CN101718866B (en) 2009-11-24 2009-11-24 Improved physical method for topographic correction of remote sensing images

Country Status (1)

Country Link
CN (1) CN101718866B (en)

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102721644A (en) * 2012-06-21 2012-10-10 中国科学院对地观测与数字地球科学中心 Method and device for processing remote sensing data of water environment
CN103198314A (en) * 2013-02-20 2013-07-10 北京农业信息技术研究中心 Remote sensing image radiation correction method
CN103438900A (en) * 2013-07-25 2013-12-11 航天恒星科技有限公司 Three-line-array camera image collaborative absolute radiometric calibration and compensation method
CN104156567A (en) * 2014-07-23 2014-11-19 中国科学院遥感与数字地球研究所 Technique for acquiring surface reflectance by coupling satellite remote-sensing image atmospheric correction and topographical correction processes
CN104951656A (en) * 2015-06-23 2015-09-30 中国科学院遥感与数字地球研究所 Wide-viewshed satellite image surface reflectance retrieval method
CN105242247A (en) * 2015-09-08 2016-01-13 首都师范大学 Improved topographic radiation correction method

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP4580720B2 (en) * 2004-09-09 2010-11-17 株式会社東芝 Remote sensing device
CN101034477A (en) * 2007-03-29 2007-09-12 上海大学 Method for eliminating shadow on remote sensing digital image and recovering picture element remote sensing value in shadow

Cited By (11)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102721644A (en) * 2012-06-21 2012-10-10 中国科学院对地观测与数字地球科学中心 Method and device for processing remote sensing data of water environment
CN102721644B (en) * 2012-06-21 2014-07-23 中国科学院对地观测与数字地球科学中心 Method and device for processing remote sensing data of water environment
CN103198314A (en) * 2013-02-20 2013-07-10 北京农业信息技术研究中心 Remote sensing image radiation correction method
CN103198314B (en) * 2013-02-20 2015-11-25 北京农业信息技术研究中心 Remote sensing images radiation correction method
CN103438900A (en) * 2013-07-25 2013-12-11 航天恒星科技有限公司 Three-line-array camera image collaborative absolute radiometric calibration and compensation method
CN103438900B (en) * 2013-07-25 2016-06-01 航天恒星科技有限公司 The collaborative absolute radiation calibration of three line scanner camera image and correction method
CN104156567A (en) * 2014-07-23 2014-11-19 中国科学院遥感与数字地球研究所 Technique for acquiring surface reflectance by coupling satellite remote-sensing image atmospheric correction and topographical correction processes
CN104156567B (en) * 2014-07-23 2017-05-03 中国科学院遥感与数字地球研究所 Technique for acquiring surface reflectance by coupling satellite remote-sensing image atmospheric correction and topographical correction processes
CN104951656A (en) * 2015-06-23 2015-09-30 中国科学院遥感与数字地球研究所 Wide-viewshed satellite image surface reflectance retrieval method
CN104951656B (en) * 2015-06-23 2018-01-12 中国科学院遥感与数字地球研究所 Wide ken satellite image Reflectivity for Growing Season inversion method
CN105242247A (en) * 2015-09-08 2016-01-13 首都师范大学 Improved topographic radiation correction method

Also Published As

Publication number Publication date
CN101718866B (en) 2012-09-05

Similar Documents

Publication Publication Date Title
CN101718866B (en) Improved physical method for topographic correction of remote sensing images
CN102628940B (en) Remote sensing image atmospheric correction method
CN102636143B (en) Aerosol optical depth remote sensing retrieval method
CN101598543B (en) Practical atmospheric correction method for remote sensing images
CN101598797B (en) Method for realizing rugged topography remote sensing scene simulation
CN107367716A (en) A kind of high-precision satellite-borne SAR geometric calibration method
CN102778675B (en) Atmospheric correction method and atmospheric correction module for satellite remote-sensing image
CN102338869B (en) Inversion method and system of downlink shortwave radiation and photosynthetically active radiation data
CN101598798B (en) System for rebuilding spectrum of high spectrum intervention data and method thereof
CN107389029A (en) A kind of surface subsidence integrated monitor method based on the fusion of multi-source monitoring technology
CN102288956B (en) Atmospheric correction method for multispectral data of remote sensing satellite
CN106407656A (en) Retrieval method for aerosol optical thickness based on high resolution satellite image data
CN102628942B (en) Method for compensating radar image dual-aspect information
CN104535979A (en) Remote sensing inversion method and system for land cloud optical thickness
CN106526590A (en) Method for monitoring and resolving three-dimensional ground surface deformation of industrial and mining area by means of multi-source SAR image
Berg et al. Improved geolocation and Earth incidence angle information for a fundamental climate data record of the SSM/I sensors
CN104156567B (en) Technique for acquiring surface reflectance by coupling satellite remote-sensing image atmospheric correction and topographical correction processes
CN103926589A (en) Satellite-borne laser altimeter system solid surface target plane and height accuracy test method
CN104181515A (en) Shallow sea water depth inversion method based on high-spectrum data of blue-yellow wave band
CN105242247A (en) Improved topographic radiation correction method
CN101526620A (en) Landform correcting method of lane-carried or satellite-carried laser scanning imaging
CN104101297A (en) Space object dimension acquisition method based on photoelectric observation
CN110532662A (en) A kind of sea surface salinity inversion method of the main passive microwave salinometer based on machine learning
Shamim et al. An improved technique for global daily sunshine duration estimation using satellite imagery
CN109781593A (en) A kind of aerosol quadratic inversion method based on PARASOL multi-angle polarization data

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
C10 Entry into substantive examination
SE01 Entry into force of request for substantive examination
C14 Grant of patent or utility model
GR01 Patent grant
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20120905

Termination date: 20171124

CF01 Termination of patent right due to non-payment of annual fee