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Title: The Madden-Julian Oscillation simulated by the Beijing Climate Center


1
The Madden-Julian Oscillation simulated by the
Beijing Climate Centers AGCM
  • Dong Min Wu Tongwen
  • Wang Zaizhi Zhang Fang
  • Beijing Climate Center, China Meteorological
    Administration
  • Beijing, 100081 PRC

2
Contents
  • Introduction
  • Model and data
  • Results
  • spectral structure
  • MJO variance distribution
  • Annual cycle of the MJO (Wavelet
  • analysis)
  • Propagating speed
  • Discussion

3
Model and Data
  • The Beijing Climate Center Model (BCC_AGCM2.0.1)
  • It is developed based on NCAR CAM3.0
    (released on 2004 09)
  • A refference Atmosphere is introduced to
    the model, The prognostic variable T and Ps
    become T and Ps
  • A new Zhang_Mcfarlane convection scheme
    (2005) replaced the original one (1995)
  • Latent heating calculation modified over
    ocean
  • Snow cover representation slightly changed
  • NCAR CAM3 (Collins et al. 2004)

4
Model run and validation data
  • Model run
  • Monthly SST from 1949,9-2001,10 (52 years)
  • Validation data
  • NCEP(1948-2002),ECMWF(1957-2002)
  • CMAP (1979-200)
  • VariablesU 850 hPa Precipitation

5
The spectral structure
  • The U850 and PP for each year (365 days) at each
    latitude are used to do time-space spectral
    analysis by FFT
  • Averaged over 10S-10N
  • Averaged over 51 year (1950-2000)

6
Comparison of time-space spectrum of U850
7
Comparison of time-space spectrum of precipitation
8
Comparison of time-space spectrum of
precipitation (pentad data)
9
Variance of MJO
  • After the spectral Analysis
  • Take the Waves of wave number 1 5 and period
    20 -90 days to reconstruct a MJO time series
  • Plot the variance of the MJO series in the
    tropics (20S-20N) for each season

10
Comparison variance of U850 MJOECMWF
11
Variance of U850 MJONCEP
12
variance of U850 MJOBCC2
13
Comparisonvariance of U850 MJOCAM3
14
Annual cycle of MJO for U850 ECMWF
15
Annual cycle of MJO for U850 NCEP
16
Annual cycle of MJO for U850 BCC2
17
Annual cycle of MJO for U850 CAM3
18
The propagating speed of MJO for U850ECMWF
NCEP
19
The propagating speed of MJO for U850models
20
Discussions
  • The BCC AGCM can simulate the MJO prety well. The
    ability of BCC model in simulating the
  • MJO is much improved than CAM3.0
  • It can reproduce the time-space structure of the
    U850 and precipitation In the tropics
  • It can reproduce the MJO variance space
    distribution
  • The simulated annual cycle of MJO is close to the
    observation.
  • The convection scheme is a key issue in the
    simulating the MJO

21
The problems need to be solved
  • The simulated MJO is not concentrate on the 30-60
    days. It slightly moved to high frequency
  • The simulated MJO space distribution has some
    difference with the observation.
  • The annual cycle of the simulated MJO also has
    some difference from the observation, especially,
    the simulated MJO is too strong in summer.
  • The simulated MJO has more fast propagating
    speed than the observation

22
Future Work
  • Analysis the mechanism of how can the convection
    scheme influence the MJO
  • The impact of the surface heating flux on the MJO
    simulation.

23
Thanks!
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