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2. Observation and data analysis
     We used sounding data observed by Vaisala Digicora2 MW 15
		rawinsonde in Pohang( 
		 E,
E, 
		 N ), Korea during a year of 1998. The ascending rate of the balloon
		is approximately 50 - 60
N ), Korea during a year of 1998. The ascending rate of the balloon
		is approximately 50 - 60  , and all the observation variables are recorded every 10 second.
		As a result, the vertical resolution of data is roughly 50 - 60
		m. However, because the rawinsonde automatically smooth horizontal
		wind data using low-pass filter in order to reduce observational
		errors, the vertical resolution of horizontal wind data becomes
		approximately 500 m. For the convenience, all observed variables
		used in this study are interpolated into 50 m grids using cubic-splint
		method.
, and all the observation variables are recorded every 10 second.
		As a result, the vertical resolution of data is roughly 50 - 60
		m. However, because the rawinsonde automatically smooth horizontal
		wind data using low-pass filter in order to reduce observational
		errors, the vertical resolution of horizontal wind data becomes
		approximately 500 m. For the convenience, all observed variables
		used in this study are interpolated into 50 m grids using cubic-splint
		method. 
		     Figure 1 shows time-height cross sections of monthly mean
		temperature and zonal wind observed at Pohang. In this figure
		we used sounding data that reached the higher altitude than 30
		km. Temperature in the troposphere decreases rapidly with height,
		while temperature in the stratosphere increases slowly with height.
		The vertical lapse rate remains nearly constant in the stratosphere
		regardless of the change of season. This suggests that the static
		stability in the stratosphere is nearly constant during a year
		of 1998.  The jet stream in winter(January and December) are much
		stronger than that in summer(July, August). Figure 1b also shows
		the clear seasonal variation of zonal wind that the zonal wind
		in the winter stratosphere is generally westerly, while that in
		the summer stratosphere is easterly. However, it should be taken
		note that easterly wind regions are also observed near z = 33
		km in January and November. 
| ![\includegraphics[scale=0.60]{fig01}](img15a.jpg)  | 
     For the analysis of gravity wave characteristics in the stratosphere
		and the troposphere, the temperature and wind profiles within
		17 - 30 km and 2 - 9 km altitude ranges are used, respectively.
		The rapid changes of temperature and wind at the tropopause can
		be excluded in the data analysis using the two separated analysis
		regions. The sounding data observed at 00UTC and 12UTC are used
		except for July in which there were only 7 soundings that reached
		the higher altitude than 30 km at 00UTC and 12UTC. Accordingly,
		in July, the sounding data observed at 06UTC and 18UTC are also
		used in addition to 00UTC and 12UTC. 
		     To obtain gravity wave perturbation from temperature and
		wind profiles in the stratosphere and the troposphere, basic state
		profiles are estimated by fitting second order polynomial into
		sounding profile for individual variables, and perturbation profiles
		are calculated by removing the basic state profile from the each
		sounding profile.