Shen Xinyong, Huang Wenyan, Wang Weiguo, et al. Contrastive study on two boundary layer parameterization schemes using TWP-ICE experiment data. J Appl Meteor Sci, 2014, 25(4): 385-396.
Citation: Shen Xinyong, Huang Wenyan, Wang Weiguo, et al. Contrastive study on two boundary layer parameterization schemes using TWP-ICE experiment data. J Appl Meteor Sci, 2014, 25(4): 385-396.

Contrastive Study on Two Boundary Layer Parameterization Schemes Using TWP-ICE Experiment Data

  • Received Date: 2014-02-07
  • Rev Recd Date: 2014-05-16
  • Publish Date: 2014-07-31
  • TWP-ICE (Tropical Warm Pool International Cloud Experiment) is carried out at Darwin Station in northern Australia by Europe and the United States, observations can be used for numerical simulation study. High resolution WRF single column model is used to simulate a case during TWP-ICE with two boundary layer parameterization schemes (YSU and MYJ schemes). Simulation results of boundary layer structure, cloud and precipitation with these two boundary layer parameterization schemes are compared.The whole simulation process can be divided into two phases, which are monsoon active period and monsoon suppressed period. During monsoon active period, the boundary layer structure simulated by MYJ scheme is better than YSU scheme. Small turbulent exchange coefficient is simulated by YSU scheme leading to weak turbulent mixing and small heat flux in boundary layer during monsoon active period, which prevents the heat and moisture of surface from upward transporting. Therefore, the simulated potential temperature and vapor mixing ratio are significantly higher than observations at the bottom boundary layer, and the simulated vapor mixing ratio is lower than observation at the top of boundary layer. During monsoon suppressed period, great turbulent exchange coefficient is simulated by MYJ scheme at night, leading to strong turbulent mixing and large heat flux, and the simulated potential temperature and vapor mixing ratio variation with height are smaller than observations, so MYJ scheme cannot simulate the structure of nocturnal boundary layer well.Also, the simulation of cloud and precipitation is affected by the boundary layer parameterization schemes. During monsoon active period, weak turbulent mixing is simulated by YSU scheme, leading to the wet bias near the surface and dry bias above. As a result, YSU scheme simulates smaller cloud liquid water content and frozen water content, less cloud fraction and lower precipitation rate. During the same period, MYJ scheme simulates the boundary layer structure well, and can better simulate cloud and precipitation. During monsoon suppressed period, the cloud fraction and precipitation simulated with both schemes show no significant difference, both exceeding observations.

  • Fig. 1  Sea level pressure (shaded) and 850 hPa wind (arrow) from FNL data (triangle mark indicates the location of Darwin Station)

    Fig. 2  Time-height cross sections of simulated turbulent exchange coefficient by YSU scheme and MYJ scheme

    Fig. 3  Time-height cross sections of simulated heat flux by two schemes

    (a) sensible heat flux simulated by YSU scheme, (b) sensible heat flux simulated by MYJ scheme, (c) latent heat flux simulated by YSU scheme, (d) latent heat flux simulated by MYJ scheme

    Fig. 4  Mean vertical profiles of observed and simulated meteorological elements during active monsoon (21 January 2006-25 January 2006)

    (a) potential temperature at 0300 UTC, (b) vapour mixing ratio at 0300 UTC, (c) wind speed at 0300 UTC, (d) potential temperature at 1500 UTC, (e) vapour mixing ratio at 1500 UTC, (f) wind speed at 1500 UTC

    Fig. 5  The same as in Fig. 4, but for during suppressed monsoon (26 January 2006-2 February 2006)

    Fig. 6  Time-height cross sections of observed and simulated liquid water content

    (a) observed by radar, (b) simulated by cloud-resolving model, (c) simulated by YSU scheme, (d) simulated by MYJ scheme

    Fig. 7  Time-height cross sections of observed and simulated relative humidity

    (a) observed, (b) simulated by YSU scheme, (c) simulated by MYJ scheme

    Fig. 8  Time-height cross sections of observed and simulated frozen water content

    (a) observed by satellite, (b) sumulated by cloud-resolving model, (c) simulated by YSU scheme, (d) simulated by MYJ scheme

    Fig. 9  Time-height cross sections of observed and simulated cloud fraction

    (a) observed, (b) simulated by cloud-resolving model, (c) simulated by YSU scheme, (d) simulated by MYJ scheme

    Fig. 10  Time series of observed and simulated rain rate

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    • Received : 2014-02-07
    • Accepted : 2014-05-16
    • Published : 2014-07-31

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