Adiabatic Cloud Parcel

A **toy lifted parcel** keeps its water-vapor pressure **e** fixed (no entrainment/detrainment). Saturation vapor pressure **e_s(T)** follows a **Magnus-type** formula. **Dew point** **T_d** solves **e_s(T_d) = e**. While rising, the parcel cools at a constant **dry adiabatic lapse** **Γ_d ≈ 9.8 K km⁻¹** until **T = T_d**; that height is the **lifting condensation level (LCL)**, sketched as **cloud base**. Above the LCL a constant **moist lapse** **Γ_m ≈ 6.5 K km⁻¹** stands in for a pseudoadiabat — adequate for **qualitative** meteorology, not for skew-T analysis or precipitation forecasting.

Who it's for: High-school or intro atmospheric-science students linking humidity, lapse rates, and cloud base; pairs with climate toy models.

Key terms

  • lifting condensation level
  • dew point
  • dry adiabatic lapse rate
  • moist adiabatic
  • relative humidity
  • parcel model

How it works

Moist air lifted adiabatically cools at roughly the dry lapse rate until it becomes saturated at the **lifting condensation level (LCL)** — then condensation is drawn as cloud. The profile above LCL uses a simplified moist lapse for illustration.

Frequently asked questions

Why does RH increase even before the cloud?
The parcel keeps the same vapor pressure e while temperature drops; saturation pressure e_s(T) falls with T, so RH = e/e_s(T) climbs until it reaches 100% at the dew point.
Is Γ_m = 6.5 K km⁻¹ exact?
No. Real moist-adiabatic lapse rates depend on pressure, temperature, and latent heating; they are curved on a thermodynamic diagram. The constant Γ_m here is a simple continuation for visualization.
Does the cloud draw water conservation?
The cartoon cloud marks where the model switches to a moist lapse. It does not track condensed water, precipitation, or entrainment of dry air.