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Microwave Remote Sensing of Atmospheric Trace Gases Remote Sensing I Lecture 6 Summer 2006

Microwave Remote Sensing of Atmospheric Trace Gases

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Microwave Remote Sensing of Atmospheric Trace Gases. Remote Sensing I Lecture 6 Summer 2006. J. F(J). Rotational Energy Levels. Rotational Transitions. allowed transitions:. Rotational Transitions. Microwave Spectrum of HCl. Microwave Spectrum of ClO. posible orientations. - PowerPoint PPT Presentation

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Page 1: Microwave Remote Sensing of Atmospheric Trace Gases

Microwave Remote Sensing of Atmospheric Trace Gases

Remote Sensing I

Lecture 6

Summer 2006

Page 2: Microwave Remote Sensing of Atmospheric Trace Gases

Rotational Energy Levels

J F(J)

)0()1(~10 JFJFJJ

)0()1(~01 FF

]cm[202~ 101

BB

]cm[426~ 112

BBB

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Rotational Transitions

121~1 JBJJJBJJ

JJJJB 22 23

12 JB

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Rotational Transitions

12~1 JBJJ

allowed transitions:

1J

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Microwave Spectrum of HCl

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Microwave Spectrum of ClO

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Degeneracies of Rotations

posibleorientations

12 J

J=1

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Degeneracies of Rotations

J=2 J=3

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Intensities of Rotational Lines

•Probability for transition between level l and level udepends on the number of molecules in level l•In thermal equilibrium given by Boltzmann distribution:

TkEN

NBJ

l

u exp

TkJBhcJ B1exp

(tends to decrease with increasing J)

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Intensities of Rotational Lines

•Depends also on degenaracies of the levels:

12 Jg J(tends to increase with increasing J)

Overall proportional to:

TkJBhcJJ B1exp12

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Intensities of Rotational Lines

May be used to derivetemperature from observedspectrum

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Microwave Spectrum of N2O

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The N2O Molecule

NN O

N2O is a linear molecule

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Microwave Spectrum of H2O

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The Water Molecule

O

H H

0.09578 nm

104.48°

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Microwave Spectrum of Ozone

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Microwave Limb Sounding:

MLS / UARS

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(Source: MLS Website)

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Part 1: Airborne Microwave Remote Sensing of Atmospheric Trace Gases.

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Airborne Submillimeter Radiometer (ASUR)

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ASUR frequency range and primary species

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ASUR onboard the NASA DC-8

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Part 2: Ground-based Microwave Remote Sensing of Atmospheric Trace Gases.

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Observations in Spitsbergen (79°N)

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Observations in Spitsbergen (79°N)

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Radiometer for Atmospheric Measurements (RAM)

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Schematic Overview of the RAM

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Measured Microwave Spectrum by the RAM

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Pressure Broadening of Spectral Lines

50km / 0.5 hPa

20km / 50 hPa

10km / 200 hPa

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Weighting Functions for Ozone Retrieval

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Retrieval techniques / Inverse Modelling

xy F

xKy

Assume that the measured spectrum y is a known function of the atmospheric profile x plus some noise ε.

Linearize F (also known as the forward model):

Page 43: Microwave Remote Sensing of Atmospheric Trace Gases

However,

can not be directly inverted (ill-posed problem)

Optimal Estimation

xKy

aTa

Taa KxySKKSKSxx

A-priori profile

A-priori profile covariance matrix

Measurement error covariance matrix

Best guess profile

Best estimate given by Optimal Estimation solution:

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Example Ozone Profile: RAM vs. Ozonesonde

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Optimal Estimation: Averaging Kernels

aTa

Taa KxySKKSKSxx

1 SKKSKSD T

aT

a

aa xxKDxx̂

DxxAxx aaˆ

DxAIAx a

Optimal estimation solution:

Define:

Then:

Define Averaging Kernel Matrix A = DK:

Page 46: Microwave Remote Sensing of Atmospheric Trace Gases

Averaging Kernel Functions