The extension of a concentrated swirling core to the surface—in other words, the actual formation of a tornado—can occur once the mesocyclone is established. Most mesocyclones do not generate tornadoes. In the ones that do, a small region of increased convergence and stretching that is typically no more than one kilometre in diameter develops in the mesocyclone for reasons that have so far eluded storm researchers. This usually occurs at the interface between the thunderstorm’s updraft and downdraft. Enhanced spin begins several kilometres above the ground, then quickly builds downward. Around such a small volume, rotation is strong enough for a smaller dynamic pipe to form and extend to within several tens of metres of the surface. This dynamic pipe is called the tornado core. Once it forms, the parent mesocyclone is reclassified as a tornado cyclone.

As the core approaches the ground, surface friction slows the rotational motion and prevents the establishment of cyclostrophic balance. Surface friction also limits the rate of airflow into the base of the core. This restriction prevents inflow from filling the tornado’s low-pressure core from below. At the same time, the parent storm’s strong updraft prevents sufficient air from filling the core from above.

With air pressure in the vortex core thus reduced in comparison to the pressure outside the core at the same elevation, a condensation funnel forms. This occurs because, at lower atmospheric pressure, air flowing upward in the core cools more quickly with increasing height than air rising at higher pressure just outside the core. Assuming that inflowing air has the same amount of moisture throughout, air rising in the core reaches its dew point at a lower height than air rising just outside the core; any further rise leads to condensation and a visible cloud. Because pressure is lowest at the axis of the vortex, air rising along this centre line reaches its dew point nearer the ground than air spiraling up just a short distance outward. This process gives rise to the characteristic conical or funnel shape of the condensation cloud.

Location in the parent storm

Many weak tornadoes form between the surface and the lowest portion of the parent cloud. These tornadoes exist for only a short time (a few minutes). Such tornadoes most commonly form beneath the flanking line of cumulus congestus clouds that frequently develop above a strong thunderstorm’s gust front (the leading edge of the storm’s downdraft). Often called gustnadoes, these vortices are true tornadoes when they are attached to the updraft of a rapidly growing congestus cloud. Gustnadoes draw their spin from the wind shear across the gust front. Their transient nature, relatively small diameters, and lack of a rotating region within the generating cloud cause them to be difficult to observe with radar. As a result, small tornadoes are not well documented, and in many respects they are less understood than stronger events.

In contrast to gustnadoes, almost all strong and violent tornadoes (and some weak ones as well) are closely connected with a rotating updraft that extends through much of the height of the parent storm. Such tornadoes tend to form near the interface between a storm’s updraft and downdraft. To an observer on the ground, they are generally perceived as being beneath the right-rear quadrant of the main body of the storm in the Northern Hemisphere as viewed along the storm path. Because of the connection of these tornadoes to large-diameter circulations within the thunderstorm, many of the events leading to their formation have been fairly well documented both visually and by radar.