Biometeorology, ESPM 129 1Lecture 16, Wind and Turbulence, Part 1, Surface Boundary Layer: Theory and Principles Instructor: Dennis Baldocchi Professor of Biometeorology Ecosystem Science Division Department of Environmental Science, Policy and Management 345 Hilgard Hall University of California, Berkeley Berkeley, CA 94720 October 3, 2012 Topics to be Covered: A. Processes A. Wind and Turbulence 1. Concepts a. Definition of Turbulence b. Reynold’s Number c. Conservation equation for wind d. TKE budget, conceptual Away out here they got a name For rain and wind and fire The rain is Tess, the fire Joe, And they call the wind Mariah Lerner and Lowe, ‘Paint your Wagon’ L16.1 Processes We experience wind and turbulence in every day life. It affects how airplanes fly, the efficiency of automobile travel and our ability to the predict weather and climate. Wind is moving air. Wind has speed and direction. Thereby, wind velocity is a vector quantity. It is distinct from its relative wind speed, which only has magnitude. Using the Cartesian coordinate system we define three wind velocities. The longitudinal wind velocity is u. This is the vector along the horizontal mean wind (x). The lateral wind velocity is v. This is the cross-wind component (y). The vertical (z) wind velocity is w. The instantaneous wind velocity is comprised of 3 components, the mean wind velocity, a periodic wave velocity and random fluctuating velocities. The mean wind advectsBiometeorology, ESPM 129 2material. Waves tend to occur at night under stable thermal stratification. If they are regular they transport very little heat and mass. Fluctuating component of wind is associated with turbulence. This component is very important for it is a mechanism for transporting heat, energy and mass between the biosphere and atmosphere. The study of fluid flow is complex. It contains motions that are highly organized (like a whirlwind, tornado or hurricane) and chaotic (as in turbulent flow). The study of fluid flow and turbulence is considered by many to remain one of the unsolved problems of modern physics. The famous fluid mechanic, Theodore von Karman, is credited with stating: ‘There are two great unexplained mysteries in our understanding of the universe. One is the nature of a unified generalized theory to explain both gravity and electromagnetism. The other is an understanding of the nature of turbulence. After I die, I expect God to clarify the general field theory to me. I have no such hope for turbulence’. With regards to biometeorology, turbulence is responsible for: 1) transferring heat, momentum and mass (water vapor, carbon dioxide, biogenic gases, pollutants) between the biosphere and the atmosphere and diffuses pollutants in the atmosphere. 2) imposing drag forces on plants, causing them to wave, bend and break 3) mixing the air and diffusing air parcels with different properties, thereby forming spatial gradients 4) gusts associated with turbulence place loads on the surface, which can erode soils and eject dust, spores and insect eggs into the atmosphere. L16.1.1 Laminar and Turbulent Flows Fluid flow can either be laminar or turbulent. A visualization of the transition of fluid flow between laminar and turbulent states is shown below.Biometeorology, ESPM 129 3 Figure 1 Visualization of turbulence http://www.thtlab.t.u-tokyo.ac.jp/index.html Copyright(C)1980 Y. Iritani, N. Kasagi and M. Hirata, All rights reserved Concepts distilled from the photograph include a gradual evolution between laminar and turbulent boundary layers as a fluid in a laminar state flows over a surface. First shear occurs at the interface, but the flow is still laminar. Soon, turbulence forms near the surface as the shear becomes unstable, while the overlaying flow is still laminar. If the fluid flow occurs over a surface for a long enough distance, the entire profile can become turbulent. Hence over small boundary, like leaves, fluid flow can have a mix of transition states. Figure 2 Evolution of boundary layers as wind blows over a surface LaminarBoundary LayerTurbulentBoundary LayerBiometeorology, ESPM 129 4 Turbulence is the chaotic and seemingly random motion of fluid parcels. Turbulence has mechanical and convective origins. Shear forces cause mechanical turbulence while buoyant instabilities (due to the intermingling of fluid parcels with different densities) causes convective turbulence. A distinct property of turbulence in the natural environment is a wide spectrum of scales (eddies) that are associated with the fluid flow. The largest scales of turbulence are produced by forces driving the mean fluid flow. Dynamically unstable, these large eddies break down into progressively smaller eddies via an inertial cascade. This cascading breakdown of eddy size continues until the eddies are so small that energy is consumed by work against viscous forces that convert kinetic energy into heat. A qualitative understanding of the multiple scales of turbulence can be attained through poetry. The famous fluid mechanic, L.F. (Lewis Fry) Richardson is attributed with writing a poem on turbulence, a parody of Jonathan Swift’s poem the flea1: Great whirls have little whirls That feed on their velocity And little whirls have lesser whirls And so on to viscosity Another poetic illustration of a property of turbulence can be acquired with a rhyme used by air pollution engineers: dilution is the solution to pollution As biological beings we probably could not exist as we do without the efficient transfer of mass and energy via turbulence, as needed to sustain our rates of metabolism. Just think as a kid when you stuck your head under the sheets, didn’t get hard to breathe after a while?? Atmospheric turbulence differs from turbulence generated in a laboratory or in pipe flow. In the atmosphere, convective turbulence coexists with mechanical turbulence. On the global scale, the rotation of the earth affects how we view geophysical fluid dynamic problems. Solar energy is the original source of winds on Earth. Temperature and pressure gradients, due to differential heating of land and sea cause air to move. The kinetic energy due to wind movement, however, is rather small compared to the solar energy budget. Oort (1964) computes that 3.1 W m-2 of solar energy (345 W m-2) produces kinetic energy to generate winds. 1 So, naturalists