Tools and Materials LITERATURE REVIEW

Z = Geopotential height m  = Lapse rate 6.5 K km -1 R = Gas constant for dry air 287 Jkg -1 ·K g = Acceleration of gravity 9.8 ms -2 TS = Surface Temperature K o p = Initial air pressure Assumption: 1013.25 hPa p = Pressure at given point hPa b Geopotential The use of pressure field as a vertical coordinate gives some advantages to visualize both the quasi-horizontal pressure surfaces and the structures of the atmosphere. Geopotential are used in synoptic scale to analyze the movement of air masses in isobaric coordinate. The values of geopotential are obtained as the potential of gravity per unit mass at a certain geometric height above mean sea level. 34 .. .......... gdz d    = Geopotential m 2 s -2 g = Acceleration of gravity 9.8 ms -2 z = Geometric height m

3.3.4 Horizontal Wind Profile

The approaching methods to analyze and approximate wind movement from satellite imagery are commonly based on the momentum equations. The orientation of a pressure gradient is used to simulate wind movement and to evaluate wind field on each pressure level. In isobaric coordinate, the pressure gradient is replaced by the gradient of geopotential in assumption that neither frictions nor turbulence occurs. 35 .. .......... ˆ h v k f p Dt h v D          Dt h v D  = Horizontal acceleration   p  = Gradient of geopotential k f ˆ = The Coriolis parameter h V  = Horizontal wind components Due to the fact that the Coriolis force is very weak near the equator, the component of Coriolis can be neglected so that the east-west wind component u and north-south wind component v is expressed as: The advective components were negligible since the satellite data used is in the form of snapshot dt=1 second. As the result obtained is in the acceleration form ms -2 and dt=1 second; the acceleration can be thought as the speed of wind exactly at the time when the image was acquired. The magnitude of horizontal wind can be found by using simple vector expression Stull 1995. 36 .. .......... 2 2 v u V    . As for the wind trajectory:  = 37 .......... arctan 360 90 o u v C o o          o o 180   if o U 180  C = Angular rotation in full circle  2 360   o C IV RESULTS AND DISCUSSION 4.1 Study Area The area analyzed by MODIS sensor on board the Terra satellite for this study is focusing around the mountain ranges located roughly in between 106 o E and 107 o E, 6.25 o S and 6.85 o S in the southern part of West Java, Indonesia. The main reason of choosing a particular area surrounded by mountains is simply due to the noticeable differences of surface temperature between the mountain ’s peak and the area with lesser height as it provide some aids to analyze the wind development. As the temperature at the surface heats the air above it by conduction, the heated air expands and become less dense than the surrounding environment and so it rises. Later on, the differences of air density cause a pressure gradient between one point and another, forcing the air to flow.

4.2 Preprocessing data

The image acquired by MODIS sensor on board the Terra satellite is geometrically distorted due to the wide-angle swath and the Earth’s curvature which lead to overlapping data errors. The distortion is so visible that it may affect image interpretation; hence, overlapping parts need to be removed so that x t u        y t v       