The wintertime polar vortex is a belt of westerly stratospheric winds circling the pole near 10 hPa (~30 km). It is disturbed by planetary-scale Rossby waves (wavenumber m = 1 or 2) that propagate up from the troposphere. Where these waves break, they deposit westward momentum and decelerate the vortex — the Eliassen–Palm flux convergence mechanism:
dS/dt = -k·A(t)·S + γ·(S0 - S)
U(60°N,10hPa) = Umax·S
Here S is vortex strength (1 = full climatological strength), A(t) the wave-forcing amplitude you set below, k the deceleration rate, and γ a radiative-relaxation term that rebuilds the vortex once forcing eases. A Sudden Stratospheric Warming is formally defined as U reversing from westerly (+) to easterly (−) at 60°N/10 hPa.
As the vortex weakens, angular momentum balance forces mass to converge and sink over the pole. That descent compresses and adiabatically warms the polar stratosphere, often by 30–50 K in a matter of days — modeled here as a lagged response to the vortex's deceleration:
dT/dt = β·max(0, -dS/dt) - α·(T - T0)
- Wave amplitude — stronger forcing (larger A) drives faster deceleration; sustained strong forcing pushes U through zero, triggering the SSW criterion.
- m = 1 vs m = 2 — a wavenumber-1 disturbance displaces the vortex off the pole (e.g. January 2004, 2019); wavenumber-2 forcing splits it into two daughter vortices (e.g. January 2009) — both are real, observed SSW morphologies.
- Radiative relaxation — with the wave amplitude returned to zero, γ slowly rebuilds the vortex over weeks, matching the post-SSW recovery seen in reanalysis data.
Real-world relevance: SSWs are the strongest documented tropospheric–stratospheric coupling event — the weakened vortex signal propagates down and shifts the surface jet stream and polar-front storm track for 4–8 weeks, a key source of sub-seasonal cold-air-outbreak predictability for forecasters.