Buoyancy and vertical motion in a fluid•In the atmosphere, local density variation is usually a result of differential heating•Hot= less dense and more buoyant•The key is to compare an object’s density to that of its surrounding environment•If buoyancy is stronger than weight, the object will float. If weight is greater, the object will sinkWhat is a parcelHow is buoyancy defined?• A “parcel” of air is like a bubble of air that rises upward from near the surface through the atmosphere. Much of atmospheric convection can be understood by analyzing the behavior of a rising parcel• Buoyancy is the vertical force caused by density difference between “parcel” and surrounding environment that causes it to rise• F=m a (Newton’s 2ndlaw)eeptenvironmenparceltenvironmenbuoyancyTTTa3 different lapse rates to keep track of:Environmental Lapse Rate: 6.5 C/km•Caused by radiation balances between surface and •troposphere and atmospheric conditions•Dramatic variance from day to day results in much of our weather •“The reason we launch weather balloons”Dry Adiabatic Lapse Rate: 9.8 C/km•Combination of 1stlaw of Thermodynamics, ideal gas law and pressure change with height•As air expands, molecules are spread apart and slow down (conservation of energy)•“Rising Air Cools”Moist Adiabatic Lapse Rate: ~6 C/km •Condensation of cloud drops releases latent heat, reducing cooling•Value changes slightly w/height and T because of variable condensation rate•Positive feedback for instability•“Rising clouds cool, but not as much”3 different types of stability to rememberAbsolutely Stable: Γenv<6 °C/km•When lapse rate of the environment is low, causing air to cool with height more slowly than any kind of parcel•As a parcel rises it will become colder faster than the environment and quickly become more dense than surroundings, causing it to sink.•Cumulus clouds can’t form spontaneously when absolutely stable conditions existAbsolutely Unstable: Γenv>9.8 °C/km•When lapse rate of the environment is high, rising air cools, but not as quickly as the surroundings.•The rising parcel experiences a greater and greater density deficit, causing rapid upward acceleration•If absolute instability occurs over a large depth of the atmosphere, look out!Conditional Stability: 6 °C/km < Γenv< 9.8 °C/km•When the atmosphere has an intermediate lapse rate (typical) it will allow cool slower than condensing air but faster than dry air.•Once a cloud has formed, it can continue to rise and develop on its own because of the density deficit.•Dry air won’t rise on its own, but if it can be forced upward some other way to generate clouds, then convection can take off. This occurs frequently.Environment and Parcel Lines:•When parcel line is to the right (warmer), buoyancy is positive•Slope of line shows lapse rates•Area between lines shows magnitude of accumulated buoyancy•Cloud forms at “Lifting Condensation Level” – Cloud base, determined only be dewpoint depression; rule of thumb: LCL (1000’s of ft) = (T-Td)/4.4Environment and Parcel Lines:•When parcel line is to the left (colder), buoyancy is negative•Air won’t rise unless it is forced to rise in another way (i.e convergence)Environment and Parcel Lines:•Conditional Instability can result in convection if low-level forcing can initial condensation•“Level of Free Convection”Stable or Unstable?Generally, what can a skew-T diagram tell us?•Upper-level temperature, moisture, pressure and wind •Stability of the atmosphere, and therefore probability of Tstorms•Lower atmosphere temps, and therefore frozen precip. Type•Wind speed with height, and therefore tornadic possibility or aviation turbulence•Likelihood and altitude of cloudiness in the absence of convection•Where in the atmosphere clouds are likely to transition to mixed and solid phaseSpecifically, what markers are we looking for?•T and Td at any level•Wind speed and dir at any level•Lapse rates at various levels•LCL: Lifting Condensation Level•CCL: Convective Condensation Level•LFC: Level of Free Convection•CAPE: Convective Available Potential Energy•CIN: Convective Inhibition•EL: Equilibrium Level•MPL: Max. Parcel Height•FZL: Freezing Level•WBZ: Wet Bulb Zero Level•PW: Precipitable Water•CONVT: Convective TemperatureLifting Condensation Level?•Follow the surface mixing ratio upwards until it intersects with the dry adiabatic lapse rate of the lifted (and cooling) surface parcel•This intersection indicates that the parcel has been lifted to its saturation mixing ratio and condensation will occur•This estimates the cloud base from surface convection or surface-lifting•Try it on your skew-T – what do you getConvective Condensation Level?•Follow the surface mixing ratio upwards until it intersects with the temperature sounding itself.•This intersection indicates that the saturation is reached in a parcel rising from the surface on its own later in the day – this parcel would have to be warmer than the surface at the time of the sounding, which results in a higher cloud base•This estimates the cloud base from afternoon surface convection better than the LCL•Try it on your skew-T – what do you getLevel of Free Convection:•From the LCL, the parcel will now cool along a moist adiabat•Follow the moist adiabat until the parcel’s Temperature crosses that of the environment•At this point the parcel is buoyant and an updraft will result•This won’t occur on soundings that are stable•Find the LFC on your skew-TConvective Available Potential Energy?•Find the area between the parcel and environment above the LFC until the temperatures intersect again.•Because temperature is proportional to density, this equation integrates buoyancy force X distance which is an energy•This “potential energy” gets converted to kinetic energy in the updraft•Greater CAPE = stronger updrafts and storms•Difference between “tall and skinny and tall and fat CAPE”•This is the best measurement of instability for storm formation•Shade the CAPE on your skew TConvective Inhibition?•CIN is pretty much the opposite of CAPE– this is negative buoyancy area that acts to prevent convection•This is the area between the environmental and parcel temperature that is below the LFC, where the parcel is colder•Greater values of CIN require