Correcting Negatively-biased Radio Occultation (RO ......jpl.nasa.gov Parametrization (Updated)...
Transcript of Correcting Negatively-biased Radio Occultation (RO ......jpl.nasa.gov Parametrization (Updated)...
Correcting Negatively-biased Radio Occultation (RO)
Refractivity below Ducts using an Optimal Estimation Approach
Kuo-Nung Wang1 (Eric), Chi O Ao1, Manuel de La Torre Juarez1 and Feiqin Xie2
(1)NASA Jet Propulsion Laboratory, Pasadena, CA, United States
(2)Texas A&M University - Corpus Christi, Corpus Christi, TX, United States
© 2017 California Institute of Technology. Government sponsorship acknowledged.
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Ducting
Motivation
• Negative N-bias (2007~2008)
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[Xie et al, Geophysical Research Letters, Vol. 37, 2010]
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Ducting
Introduction
• Ducting occurs when dN / dh < -157
(N-units/km) at the top of PBL
• The curvature of the signal path will
equal or larger than the curvature of
the Earth
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Earth Ducting layer
[A. T. Young, http://aty.sdsu.edu/explain/simulations/ducting/duct_intro.html]
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Ducting
N-bias
• No tangent point lies within the ducting layer
• x=rn(r) becomes a multi-value function w.r.t. height (r)
• Bending angle w.r.t. x will remain seamless
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h
x
hb
ht
h
α
h
N
True Abel
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Parametrization
Reconstruction
• The h(x) below ducting can be derived analytically based
on bi-linear assumption
• Using other assumptions a h(x) profile can be defined by
a pair of parameter [xb, xm]
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ℎ1 𝑥 = ෨ℎ 𝑥 +2
𝜋ℎ𝑡 − ℎ𝑏 𝑧 − 1 + 𝑧2 𝑡𝑎𝑛−1 Τ1 𝑧
where 𝑧 = ൗ𝑥𝑏−𝑥
𝑥𝑚−𝑥𝑏
xmxb
ht
hb
hm
h1(x)
h2(x)
h3(x)
h4(x)
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Ill-posed problem
Reconstruction
• Infinite number of refractivity solutions corresponds to
the same bending angle profile (Xie et al. 2006)
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Which [xb, xm] pair is correct?
Reconstruction
• Precipitable water (PW): different profiles (different [xb,
xm]) contains different PW
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[Wang et al, AMT discussion, 2017]
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Which [xb, xm] pair is correct?
Reconstruction
• Optimal Estimation
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xb
xm
Apriori
Measurement
Apriori
Apriori
𝐶0
Estimated [xb, xm]
𝐶𝑦
PW
Optimal
Estimation
Ƹ𝑠𝑛+1 = 𝑠0 + (𝐶0−1 + 𝐾𝑛
𝑇𝐶𝑦−1𝐾𝑛)
−1𝐾𝑛𝑇𝐶𝑦
−1 𝑦 − 𝑦𝑛 − 𝐾𝑛 𝑠0 − Ƹ𝑠𝑛
y
𝑠 Ƹ𝑠
𝐾𝑛 = ቤ𝜕𝑦
𝜕𝑠𝑠=𝑠𝑛
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Refractivity Reconstruction (Simulation)
Results
• End-to-end validation
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PW
Radiosonde
Refractivity
A-priori:
[xb, xm]
Reconstructed
Refractivity
Forward
Abel
Optimal
Estimation
Bending
Angle
Inverse
Abel
Abel
Refractivity
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Refractivity Reconstruction (Simulation)
Results
• VOCALS (VAMOS Ocean-Cloud-Atmosphere-Land
Study) campaign collocated with AMSR-E
• Location: Southeast pacific ocean
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Refractivity Reconstruction (Simulation)
Results
• X-h curves and N-h curves
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Refractivity Reconstruction (Simulation)
Results
• 19 cases (reconst. - RAOB)
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Refractivity Reconstruction (Simulation)
Results
• 6 cases (reconst. - RAOB)
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Refractivity Reconstruction (Actual RO signals)
Results
• 8 cases
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Refractivity Reconstruction (Actual RO signals)
Results
• 8 cases (Reconst. - RAOB)
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Summary
• Optimal estimation constrained by PW measurements reduces the
RO N-bias to < 1% in simulation and < 5% in actual data compared
to 15% using inverse Abel
• Critical layer height, thickness and refractivity increment can also be
better estimated with PW-constrained optimization than with Abel
integrals
• In addition to PW constraint, the flexibility of the optimal estimation
framework allows to use other physical constraints to correct the N-
bias in the presence of ducting
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Planetary Boundary Layer (PBL)
Introduction
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Earth’s surface
~1km PBL
~10km Free Troposphere
• Temperature inversion:
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GPS Radio Occultation (RO)
Introduction
• Forward Model:
𝛼 𝑟𝑜 = −2𝑛 𝑟𝑜 𝑟𝑜න𝑟0
∞ 1
𝑛 𝑟
𝑑𝑛 𝑟
𝑑𝑟
1
𝑛 𝑟 𝑟 2 − 𝑛 𝑟𝑜 𝑟𝑜2𝑑𝑟
• Changing variable: x = rn(r)
• Assume the value of x has 1-to-1 relationship with r.
• Forward Abel Transform:
𝛼 𝑥𝑜 = −2𝑥𝑜න𝑥0
∞ 1
𝑛 𝑥
𝑑𝑛 𝑥
𝑑𝑥
1
𝑥2 − 𝑥02
𝑑𝑥
where 𝑥 = 𝑟𝑛 𝑟
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Refractive index
Bending Angle
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GPS Radio Occultation (RO)
Introduction
• Inverse Abel Transform:
𝑛 𝑥𝑜 = 𝑒𝑥𝑝1
𝜋න𝑥0
∞ 𝛼 𝑥
𝑥2 − 𝑥𝑜2𝑑𝑥
• The retrieved refractivity profile has 1-to-1 relationship
with the bending angle observation.
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Bending Angle
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Parametrization (Updated)
Progress
• Steps: (for each [x1, x2])
– h3 can be calculated based on x1
– ෨ℎ 𝑥 is a square root function of x at x1: linear regression is used
to fit ෨ℎ 𝑥 and calculate C (to get h1)
• ෨ℎ 𝑥 − ℎ3 = − 𝐶 𝑥1 − 𝑥
• 𝐶 = −16
𝜋2ℎ3−ℎ1
2
𝑥2−𝑥1
– Get the profile below h1:
– The slope of h-x close to x1 should remain the same (get h2)
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ℎ𝐴 𝑥 = ෨ℎ 𝑥 +2
𝜋ℎ3 − ℎ1 𝑧 − 1 + 𝑧2 𝑡𝑎𝑛−1 ൗ1 𝑧
x2x1
h3
h1
h2
a
b
c
d
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Which [xb, xm] pair is correct?
Reconstruction
• Apriori for xb:
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Which [xb, xm] pair is correct?
Reconstruction
• PW calculation for certain [xb, xm] :
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𝑃𝑊 = න𝑞(𝑁, 𝑇)𝑑𝑝
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Refractivity Reconstruction (Simulation)
Results
• 6 cases
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Refractivity Reconstruction (Actual RO signals)
Results
• 8 cases
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Refractivity Reconstruction (Actual RO signals)
Results
• 8 cases
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Refractivity Reconstruction (Actual RO signals)
Results
• Reconstruction on RO signals
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PW
GPS-RO
Refractivity
A-priori:
[xb, xm]
Reconstructed
Refractivity
Optimal
Estimation
Radiosonde
Refractivity