The change in
density of a hypothetical
parcel of air as it rises relative to the density of the surrounding air determines where in the atmosphere it can continue rising by
buoyancy. The density of an air parcel is based on its
temperature,
pressure, and
water vapor content, provided that its
chemical makeup is otherwise constant. CAPE is a measure of the maximum
kinetic energy per unit mass that an air parcel can acquire by remaining less dense than its surroundings. This requires an approximation of the change in the parcel's density as it rises. For calculations of CAPE, the hypothetical air parcel is assumed to initially rise and cool at the
dry adiabatic lapse rate: the rate at which air cools as it expands without any release of
latent heat. Once the parcel cools to the point of
saturation, it is then assumed to cool at the
moist adiabatic lapse rate: the rate at which air cools adjusted for the release of latent heat from water vapor
condensing within the saturated air parcel. For typical daytime atmospheric conditions, accounting for moisture produces larger and more accurate estimates of CAPE. The parcel begins with temperature and moisture characteristics of its surroundings but then deviates from those conditions as it rises. MUCAPE may be a more appropriate measure of the buoyant energy available to a thunderstorm with
inflow originating well above the surface. While CAPE quantifies instability in the context of air moving directly upward,
slantwise CAPE (SCAPE) can be computed in situations where
buoyant ascent can be realized if parcels move in some combination of both the horizontal and vertical. thermodynamically representing a reversible moist adiabatic process. This calculation is better suited for humid tropical environments such as within
tropical cyclones. The numerical methodology underlying CAPE can also be performed for portions of the atmosphere where an air parcel would be denser and cooler than its surroundings. These areas have negative buoyancy, resulting in the force of buoyancy acting downwards. Integrating within these areas, typically between the surface and the LFC, results in a negative value also known as
convective inhibition (CIN). Additional upward forces are required for an air parcel to rise against negative buoyancy, with CIN providing a measure of the work required to overcome negative buoyancy and reach a freely buoyant height. A similar quantity is
downdraft CAPE (DCAPE), which integrates the negative buoyancy potentially imparted on an initially saturated parcel as it descends from some arbitrary height to the ground. This measure is used to quantify the potential for
downbursts. == Applications and limitations ==