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A difference in temperature causes different pressures, air travel from high to low pressure, and that is wind.

We can even produce wind in an experiment like in this video. In this video, what is the way it can produce gusts?

To increase wind speed, you must increase the pressure gradient at this local place, but it is impossible to change the temperature at these places so fast, every time a gust hits.

It isn't clear to me what causes gusts. Is it a sudden increase in wind speed that lasts a few seconds at flat surfaces, like sea, lake, desert, and ice?

This video is an example when gusts come.

22flower
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3 Answers3

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In this Wikipedia article,

Turbulence is caused by excessive kinetic energy in parts of a fluid flow, which overcomes the damping effect of the fluid's viscosity. For this reason turbulence is commonly realized in low viscosity fluids

You ask:

It isn't clear to me what cause gusts, sudden increase in wind speed that lasts a few seconds at flat surfaces like sea, lake, desert, ice?

Qualitatively, it is turbulence at small scales, both in area and in the energy in the flow. I am sure that, if you look at a large area of "sea, lake, desert, ice", at the time you see the local gust, there will be more of these sudden gusts.

anna v
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Some points need to be clarified here. Despite the very details of turbulence are not fully understood yet, anyway we can say something about the qualitative or the average motion of fluids even when turbulence occurs.

  1. The video linked in your answer can be explained by buoyancy. It can be related to the mechanisms of (in)stability in fluids and macroscopic motion of the flow, more than turbulence.

    Let's start with a toy problem, with a fluid confined between two horizontal planes at different temperatures, with warmer temperature on the bottom wall:

    • when the temperature jump is lower than a critical value, a temperature gradient is established in the fluid, without any motion; this situation corresponds to a stable equilibrium of the system;
    • when the temperature jump exceeds that critical value, first instability occurs; the equilibrium loses its stability and convective cells appears in the fluid: in some regions of the flow close to the bottom wall, the fluid is warmer and less dense that the surrounding fluid, and it tends to move upwards by buoyancy; as the fluid approaches the top low-T wall, the temperature of the fluid particle decreases; now, denser than before and the surrounding regions, the fluid particle tends to move downwards towards the high-T bottom wall; passing close to the bottom wall, the fluid particles absorbs heat again, its temperature increases and its density decreases and it's ready to move upwards again by buoyancy.

    enter image description here

    The very same mechanism occurs here: upwards motion over the hot vessel, sucking air from the surrounding regions. I suspect also that the vessel with ice is quite irrelevant to the problem, or at least it has a "higher order effect".

enter image description here

  1. Pressure gradient, viscous stresses and volume forces are not directly related to the velocity of the fluid, but are related to the acceleration of the material particles. You can easily realize it, writing the momentum equation in differential convective form

    $\rho D_t \mathbf{v} = + \rho \mathbf{g} -\nabla P + \mathbf{s_n}$,

    being $D_t \mathbf{v} = \mathbf{a}$ the acceleration of the material particles, $\rho$ the density of the fluid, $\mathbf{g}$ the force per unit mass, $P$ the pressure, $\mathbf{s_n}$ the viscous stress vector.

    Thus, when you move in a large region of space, you can encounter fluid in motion at quite fast velocity (strong jet gust, or), even if there is no strong local pressure gradient. The fluid gets accelerated in quite a long range, to get that velocity. You can get these thermal (updraft) over hot surfaces like parking areas, when flying at quite low altitudes.

  2. You experience sudden gust because you're flying usually quite at a high velocity, so that you encounter that regions of the fluid for a very small time-interval.

basics
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Please first note that the flow, while indeed driven by the temperature differences between the tropics and the higher latitude on the global scale, is actually mostly along the isobars in mid-latitudes, not across them. That means that the flow is not from a place of higher pressure to a place of lower pressure, but mostly around the pressure lows and highs. This is because on the large scales the relevant forces are the pressure force and the Coriolis force. That leads to the geostrophic equilibrium. In the planetary boundary layer (lowest ~2 km), the flow is turned in a certain direction towards the low pressure, because the turbulent friction force plays an important role as well. But not above the boundary layer.

Wind gusts are caused by turbulence, chaotic unpredictable movement of fluid that causes strong mixing and friction. In a comment you asked "Why is turbulence related to gust, gust is not chaotic, it has same direction as wind, just speed is increased?" The gust is very local, when looking from a distance, it can be large turbulent structure, but a turbulent structure nonetheless. The largest turbulent vortexes in the turbulent atmospheric flows are sized ~km. They contain the most of the energy. Due to the chaotic nature of turbulence, they give birth to sudden increases in wind speed in various parts of the flow region.

Turbulence develops due to instabilities in the flow typically caused by differences of the wind vector from place to place (wind shear) or differences of density/temperature - often the warm surface of the Earth vs. colder (but it is more complicated due to compressibility).

So even when there are no temperature/density effects (neutral stratification), there will be turbulence due to the wind shear. If there is wind, there is always wind shear, because the wind speed at the surface is zero. If the Reynolds number is high enough, and in the atmosphere it always is, there will be turbulence caused by differences of the flow speed from place to place. When we also account for the stabilizing effect of a stable temperature stratification, the instability is the Kelvin-Helmholtz (K-H) instability that causes turbulence if the wind shear is large enough when compared to the stratification (the ratio is the Richardson number).

See this laboratory demonstration of the K-H instability The same instability creates all ordinary turbulence when any object moves in the air. The turbulence around us, around cars, around aeroplanes.

Turbulence can also be caused by thermal convection even if there is no mean horizontal wind at all. Thermal convection develops when thermal stratification becomes unstable due to positive heat flux from the warm surface. Unfortunately, in a compressible fluid (like the air) the situation is complicated by the compressibility and one must look at the profiles of the potential temperature and not temperature. In a well-mixed atmosphere the potential temperature is constant, but the temperature decreases by one degree of Celsius by every 100 m of height. The result of convection are rising thermals and plumes of warm air in which birds and glider aircraft like to soar. Wind gusts may be well caused by the thermally-produced turbulence.

enter image description here This shows my simulation of thermal convection in the atmosphere with shallow clouds. No mean wind, just thermal turbulence. Potential temperature, moisture, liquid water, vertical velocity.

When thermal convection becomes very strong due to very unstable stratification, storms may develop. Those have their own complicated wind flow, which is very turbulent, and can cause strong gusts. The origin is from the thermal convection, just complicated by the complicated thermodynamics of water in the clouds.

Also, the large scale flow, mentioned at the start of the answer, often creates fronts between warmer and colder air. On these fronts, weather patterns develop on larger scales and especially cold fronts cause locally unstable stratification and hence convection and storms and hence wind gusts.