Prerequisites
Differential equations, ideal gases, dimensional analysis, and hydrostatic balance.
For an isothermal ideal-gas atmosphere, dp/dz = -rho g and p = rho Rs T. With constant g, T and specific gas constant Rs, define H = Rs T/g. Then p(z) = p0 exp(-z/H), and density has the same exponential shape.
Worked example
At z = H, p/p0 = exp(-1), about 0.368. At z = 2H it is exp(-2), about 0.135. With Rs = 287 J/(kg K), T = 280 K and g = 10 m/s^2, H = 8036 m. Real temperature profiles need not be isothermal.
Further inquiry
Derive the exponential profile by separating variables, then integrate density to obtain the column mass per area. Replace constant T with a specified positive T(z) and write the integral solution for pressure. Explain why this mathematical atmosphere is not a full weather model.
Review criteria
- Declare the pressure boundary condition and constant-g assumption.
- Keep absolute temperature and specific-gas-constant units consistent.
- Distinguish the isothermal model from an observed atmospheric profile.