To access these data files, click on the above hyperlinked filenames.
This figure shows an inventory of sounding data during the SCSMEX IOPs. A completely filled circle indicates that soundings were available 152 times out of a possible 152 (4 soundings per day for 38 days). The red circles indicate the nominal positions of the research vessels located within the enhanced sounding arrays. The grid over the NESA shows the analysis domain for our gridded data product.
Data in the above files represent an average of gridded data fields
over the SCSMEX Northern Enhanced Sounding Array (NESA),
that is, the northern polygon in the above figure.
Fields of height (z), zonal wind
(u), meridional wind (v), temperature (T) and specific
humidity (q) were objectively analyzed using multiquadric interpolation
(Nuss and Titley 1994) over a rectangular grid slightly larger than
the NESA at 25 mb resolution from 1000 to 25 mb and at 1 degree resolution
in both the latitude and longitude directions (see grid in above figure).
Surface pressure was also analyzed over this grid. These analyses were done
for 244 periods (61 days at 00, 06, 12, and 18 UTC) during May and June of
1998.
Data used in this analyses included quality-controlled sounding data from
53 sounding sites around and over the South China Sea and
the JMA reanalysis in data sparse regions
(i.e., at every 5 degree grid intersection no observations within a
3 degree radius).
During SCSMEX the ships were on site during the following periods:
Notes:
advect.nesa
O'Brien J.J., 1970: Alternative solutions to the classical vertical velocity
problem. J. Appl. Meteor., 9, 197-203.
Yanai, M.S., S. Esbensen and J.H. Chu, 1973: Determination of bulk properties
of tropical cloud clusters form large-scale heat and moisture budgets.
J. Atmos. Sci., 30, 611-627.
IOP 1: 05/06/1998 to 05/25/1998 (20 days)
However the sounding sites over the Northern South China Sea (the NESA pologon)
took observations 4x/day for the period from 05/05/98 thru 06/20/98. We refer
to this 47-day period as the SCSMEX IOP during which time the results
should be of higher quality due to the enhanced nature of the observations.
IOP 2: 06/05/1998 to 06/22/1998 (18 days)
fields.nesa
File "fields.nesa" contains 244 periods of six-hourly data. For each six hour
period there are 42 lines of data.
Line 1 contains: [year, month, day, hour]
written with format (4i3)
Lines 2-42 contain: [p(mb), z(m), u(m/s), v(m/s), omega(mb/hr), T(C),
theta(K), specific humidity(gr/kg) and
divergence(1/s)*10e6] written with format (9f.2)
Omega is computed using O'Brien's (1970) method with an isovalue divergence
adjustment. Omega is set to zero at the surface and at 100 mb.
File "advect.nesa" contains 244 periods of six-hourly data. For each six hour
period there are 42 lines of data.
Line 1 contains: [year, month, day, hour]
written with format (4i3)
Lines 2-42 contain: [p(mb), hu(m/s**2), vu(m/s**2), hv(m/s**2), vv(m/s**2),
hT(C/s), vT(C/s), hq(gr/(gr*s)), vq(gr/(gr*s))]
written with format (f8.2,1p,8e11.3)
where hu - horizontal advection of u
where vu - vertical advection of u
where hv - horizontal advection of v
where vv - vertical advection of v
where hT - horizontal advection of T
where vT - vertical advection of T
where hq - horizontal advection of q
where vq - vertical advection of q
These horizontal and vertical advection terms were computed using centered
differences as follows:
horizontal advection of "f": h(f) = u*df/dx + v*df/dy
where: dx = a cos(phi)*d(lambda)
dy = a d(phi)
phi - latitiude
lambda - longitude
vertical advection of "f": v(f) = omega*df/dp
q1q2.nesa
File "q1q2.nesa" contains 244 periods of six hourly data. The computation of Q1
and Q2 were not done for the first and last periods of the IOP because time
center differences were used in computing these fields and no grids were
analyzed before and after the IOP. For each six hour period there are 42 lines
of data.
Line 1 contains: [year, month, day, hour]
written with format (4i3)
Lines 2-42 contain: [p(mb), Q1(C/day), Q2(C/day)]
written with format (3f.2)
The apparent heat source, Q1, and moisture sink, Q2 (Yanai et al. 1973)
were computed as:
Q1/cp = [dT/dt + h(T) + (p/po)**kappa * omega * d(theta)/dp]
Q2/cp = -Lv/cp * [dq/dt + h(q) + v(q)]
where dt = 12 hours
po = 1000 mb
cp = 1004
Lv = 2.5e6
g = 9.8
eopo.nesa
File "eopo.nesa" contains values of surface evaporation (e_0) and precipitation
rates (p_0) for 244 six-hourly periods. The surface evaporation values
represent the average from the JMA reanalyses. Once surface
evaporation is known, rainfall rates can be computed from the moisture budget by
integrating the equation for Q2 (shown above) from 1000 mb to 100 mb as follows:
p_0 = e_0 + 1./(g*Lv) * [integral(Q2*dp) from 1000mb to 100mb]
Line 1-244 contains: [year, month, day, hour, e_0(mm/day), p_0(mm/day)]
written with format (4i3,2f8.2)
References
Nuss W.A. and D.W. Titley, 1994: Use of multiquadric interpolation for
meteorological objective analysis. Mon. Wea. Rev., 22, 1611-1631.
Please send any questions or comments to Paul Ciesielski,
paulc@atmos.colostate.edu