are key to understanding atmospheric temperature changes. As air parcels move vertically, they expand or compress without exchanging heat, leading to cooling or warming. This affects cloud formation, precipitation, and overall atmospheric stability.
Dry and moist adiabatic processes differ based on air saturation. Dry processes follow a steeper lapse rate, while moist processes involve . Understanding these differences is crucial for predicting weather patterns and atmospheric behavior.
Adiabatic Processes
Adiabatic processes in thermodynamics
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LABORATORY 6: CLIMATE CHANGE – PART 1 – Physical Geography Lab Manual: The Atmosphere and Biosphere View original
Involve no heat exchange between a system (air parcel) and its surroundings
Occur when air parcels move vertically in the atmosphere with minimal heat exchange due to air's low thermal conductivity (insulating properties)
and warming significantly influence atmospheric temperature changes
Rising air parcels expand and cool adiabatically as pressure decreases (adiabatic cooling in updrafts)
Sinking air parcels compress and warm adiabatically as pressure increases ( in downdrafts)
Crucial for understanding atmospheric stability, cloud formation (cumulus), and precipitation processes (rain, snow)
Potential temperature conservation
(θ) is the temperature an air parcel would have if brought adiabatically to a reference pressure level (usually 1000 hPa)
Defined as: θ=T(pp0)cpR
T is the actual temperature (K)
p0 is the reference pressure (1000 hPa)
p is the actual pressure (hPa)
R is the gas constant for dry air (287 J/kg/K)
cp is the specific heat capacity at constant pressure (1004 J/kg/K)
Conserved during adiabatic processes, remaining constant as an air parcel moves vertically without heat exchange
Useful for comparing temperatures of air parcels at different heights and identifying atmospheric stability (stable vs unstable layers)
Dry and Moist Adiabatic Processes
Dry vs moist adiabatic processes
Dry adiabatic processes occur in unsaturated air (relative humidity < 100%)
Temperature changes follow the (DALR) of approximately -9.8℃/km
Rising unsaturated air cools at the DALR, sinking unsaturated air warms at the DALR
Moist adiabatic processes occur in saturated air (relative humidity = 100%)
Temperature changes follow the (MALR), which varies with temperature and pressure
MALR is less than the DALR due to latent heat release during condensation (cloud formation)
Rising saturated air cools at the MALR, sinking saturated air warms at the MALR
Transition between dry and moist adiabatic processes occurs at the
LCL is the height at which a rising air parcel becomes saturated and condensation begins (cloud base)
Atmospheric stability analysis
Atmospheric stability depends on the compared to adiabatic lapse rates
Stable: Environmental lapse rate < MALR (vertical motion suppressed)
Conditionally unstable: MALR < Environmental lapse rate < DALR (instability depends on saturation)
Unstable: Environmental lapse rate > DALR (vertical motion enhanced)
Potential temperature assesses atmospheric stability
Increasing θ with height indicates a stable atmosphere (inversion)
Decreasing θ with height indicates an unstable atmosphere (allows convection)
Constant θ with height indicates a neutrally stable atmosphere (allows vertical mixing)
Analyzing atmospheric stability using adiabatic processes and potential temperature is essential for predicting convection (thunderstorms), turbulence (clear air), and other weather phenomena (fog, haze)