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The Homogeneity of Midlatitude Cirrus Cloud Structural Properties Analyzed from the Extended FARS Dataset

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Title: The Homogeneity of Midlatitude Cirrus Cloud Structural Properties Analyzed from the Extended FARS Dataset


1
The Homogeneity of Midlatitude Cirrus Cloud
Structural Properties Analyzed from the Extended
FARS Dataset
  • Likun Wang
  • Ph.D. Candidate

2
Content
  1. Motivation
  2. FARS high cloud dataset
  3. Proposed Method
  4. Proposed future research

3
Why are cirrus clouds important?
  • Influence on the radiation balance of the climate
    system (Liou, 1986)
  • Macrophysical properties
  • Cloud top, base, thickness, cover, overlap
  • Microphysical properties
  • Ice water content (IWC) and ice crystal size
    distribution
  • Ice crystal habit

4
Why are cirrus clouds important? (cont)
  • Important in the chemistry of the upper
    troposphere
  • Contribute to upper troposphere ozone depletion
    (Borrman et al. 1996 Kley et al. 1996)
  • Perturb chlorine chemistry (Solomon et al. 1997
    )

5
Reality v.s. GCM
  • Using Plane Parallel Homogeneous (PPH)
    approximation

6
Reality v.s. GCM (cont)
  • No horizontal inhomogeneities
  • e.g. the distribution characteristics of cloudy
    and clear sky regions
  • e.g. the horizontal variability of microphysical
    properties within a layer

7
Reality v.s. GCM (cont)
  • Limited vertical inhomogeneities
  • e.g. How clouds overlap?
  • maximum overlap for adjacent levels random
    overlap for non adjacent levels is assumed
  • e.g. the vertical variability of microphysical
    properties within a layer

8
Why PPH cant represent reality ?
PPH without homogeneities
ICA With homogeneities
9
PPH v.s. ICA
  • Independent column approximation (ICA)
  • Sliced grid box into different column
  • Radiative transfer calculations of a cloud field
    are done in for every column
  • then an average value is determined

10
PPH v.s. ICA ------Albedo Bias
aPPHgt aICA Overestimate
aPPH
Bias
aICA
Albedo
t2
tm
Optical Thickness
t1
  • Carlin et al. personal communication Cahalan et
    al. 1994 Barker,1996

11
PPH v.s. ICA ------ OLR Bias
  • OLR(ICA)-OLR(PPA) 14 W/m- 2 (Fu et al. 2000)

12
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13
Inhomogeneous structure observed from cases study
14
How about cirrus?
  • the complexity of internal structure exists
  • scale 10-2 105 m
  • Include
  • Turbulence
  • Kelvin-Helmholtz waves
  • Small scale cellular structure, convective cell
  • Gravity waves
  • Mesoscale Unicinus Complexes (MUC)

15
How about cirrus? (cont)
  • Starr and Cox (1985)
  • embedded cellular structures develop in the
    simulation of cirrostratus cloud layer
  • horizontal scales 1 km or less
  • Dobbie and Jonas (2001)
  • radiation could have an important effect on
    cirrus clouds inhomogeneity

16
Big difficulties
  • Case analysis is not enough to disclose the
    characteristics of cirrus clouds inhomogeneities
  • Need a high resolution and long-term datasets
  • Different scale processes often happen together
    and coexist in the same cloud system and not easy
    to locate
  • Need an efficient analysis tool

17
Content
  1. Motivation
  2. FARS high cloud dataset
  3. Proposed Method
  4. Proposed future research

18
FARS Site
  • Located 40? 4900N, 111? 4938W
  • Instruments
  • Passive Remote Sensors
  • Active Remote Sensors
  • Polarization Cloud Lidar (PCL) ---Ruby lidar
  • Two-color Polarization Diversity Lidar (PDL)
  • 95 GHz Polarimetric Doppler Radar

19
Ruby lidar
  • Two channels
  • Vertical polarization transmitted
  • Manually "tiltable" 5 from zenith
  • 0 .1 Hz PRF, 7.5 m maximum range resolution
  • Maximum 2K per channel data record length
  • 1-3 mrad receiver beamwidths
  • 25 cm diameter telescope
  • 0.694 µm wavelength, 1.5J maximum output

20
FARS high cloud dataset
  • October,1987 --- Now
  • Typical 3-hour data (10 sec resolution)
  • Using the average wind speed 25 m/s
  • Spatial scale 250 m 270 km
  • Mainly focus on higher, colder and thinner
    cirrus cloud independent with low clouds (lidar
    limit)

21
FARS Data (Oct. 1987 - Dec. 2001)
  • Total 3216 hours

22
FARS Data per month
Max 404 hours(OCT) Min 177 hours (JUN)
23
Content
  • Motivation
  • FRAS high cloud dataset
  • Proposed Method
  • Proposed future research

24
Signal from lidar
  • P0 is the power output (J) ,
  • c speed of the light (m s-1),
  • t the pulse length (m),
  • Ar the receiver collecting area (m2),
  • ? the volume backscatter coefficient (m sr)-1,
  • ? the volume extinction coefficient area (m-1),
  • ? the multiple forward-scattering correction
    factor.
  • m and c denote contributions from molecules and
    cloud.

25
Signal from lidar
  • Calibrate the scattering and extinction due to
    air molecules under the pure molecular scattering
    assumption (Sassen 1994)
  • Assume a relationship (Klett 1984)
  • It is possible to gather the information on
    inhomogeneous properties by analyzing P(R)R2

26
From Time series to spatial series data
  • Assume that the internal cloud properties vary
    much more with space than with typical
    observation periods
  • Also assume cirrus moves faster horizontally than
    vertically
  • Using radiosonde data, we can transfer time
    series data to spatial series data

27
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28
Why wavelet?
29
Spectrum of two process (Fourier transform)
30
But using wavelet
31
Continuous Wavelet Transform (CWT)
  • the element transform wavelet function can be
    defined
  • Where
  • t is translation parameters
  • s is scale parameters

32
? can be many forms including morlet, Mexican hat

33
Continuous Wavelet Transform (CWT)
  • CWT is defined as follows
  • Where
  • x(t) is the signal
  • ?(t) is the wavelet function
  • t and s , the translation and scale parameters,
    respectively

34
Content
  • Motivation
  • FRAS high cloud dataset
  • Proposed Method
  • Proposed future research

35
Proposed future work
  • Examining structural inhomogeneity of broken
    cirrus cloud cases
  • Determining the statistics of broken cirrus
    fractional cloud amounts
  • Determining cloud layer overlap for multiple
    layer cirrus clouds without low water clouds
  • Creating the relationship between the cloud top
    temperature and the length scales of cloud
    distribution

36
Proposed future work
  • Examining inhomogeneous properties in
    homogeneous cirrus
  • Check all the cirrostratus cases
  • Locate inner inhomogeneous dynamics process such
    as gravity waves, Kelvin-Helmholtz waves and
    convective cell
  • Evaluate statistics characteristics of these
    process

37
Proposed future work
  • Furthering the knowledge of cirrus cloud
    structures and the dynamics to the major cloud
    generating mechanisms
  • Classified into four kinds type
  • Check every types inner structures
  • Try to find the relationship between inner
    structures and dynamics

38
Proposed future work
  • Calculating the bias of radiative quantities due
    to the neglect of cirrus cloud inhomogeneities
  • Use Fu and Liaos radiation transfer model
  • Structural characteristics
  • Quantify the bias of albedo and OLR between ICA
    and PPH

39
Purpose of research
FARS lidar data
radiosonde data
Final Purpose is Characterize the vertical and
horiziontal inhomogeneities of midlatitude cirrus
cloud
spatial series data
wavelet method
cloud detection method
cloud fraction
cloud overlap
length scale of cloud distribution
40
Purpose of research (cont)
Final Purpose is Quantify the radiative bias
due to the neglect of midlatitude cirrus cloud
inhomogeneities using radiation transfer models
Characteristics from data analysis
Radiation Transfer Model
LW Radiation Bias
Albedo Bias
41
Thank you! Need hard work!
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