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MET 61 1 MET 61 Introduction to Meteorology MET 61 Introduction to Meteorology - Lecture 10 Atmospheric Dynamics Dr. Eugene Cordero Ahrens: Chapter 9 W&H: Chapter 7, pg 271-296 Class Outline: Principle forces in the atmosphere Pressure gradient Coriolis Geostrophic wind
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MET 61 2 MET 61 Introduction to Meteorology Atmospheric forces Fundamental Forces in the atmosphere – – – –
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MET 61 3 MET 61 Introduction to Meteorology Atmospheric forces Fundamental Forces in the atmosphere –Pressure Gradient Force –Gravity –Rotation of the Earth –Friction
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MET 61 4 MET 61 Introduction to Meteorology Pressure Ultimately responsible for our weather
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MET 61 6 MET 61 Introduction to Meteorology Horizontal Pressure Changes Determines the direction and speed of winds: –Predominate force in atmospheric flows Can help explain general circulation of atmosphere.
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MET 61 7 MET 61 Introduction to Meteorology
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MET 61 9 MET 61 Introduction to Meteorology
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MET 61 10 MET 61 Introduction to Meteorology
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MET 61 11 MET 61 Introduction to Meteorology Pressure Gradient Force Pressure gradient: –Dependent on spacing between isobars – –
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MET 61 12 MET 61 Introduction to Meteorology Pressure Gradient Force Pressure gradient: –Dependent on spacing between isobars –Dense or tight clustering of isobars - strong or large pressure gradient –Weak clustering of isobars - weak pressure gradient Pressure gradient directed from high to low pressure
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MET 61 13 MET 61 Introduction to Meteorology
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MET 61 14 MET 61 Introduction to Meteorology Reading a weather map Orient yourself (location, date and time) Identify what you are looking at Determine the interval of the field
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MET 61 15 MET 61 Introduction to Meteorology
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MET 61 16 MET 61 Introduction to Meteorology
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1.At what local time is this map valid? 2.What fields are we looking at? 3.Indicate the direction of the pressure gradient force at points A-C. A A C C B B
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MET 61 18 MET 61 Introduction to Meteorology 1.At what local time is this map valid? 2.What fields are we looking at? 3.Indicate the direction of the pressure gradient force at points A-C. A A C C B B
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MET 61 19 MET 61 Introduction to Meteorology
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MET 61 20 MET 61 Introduction to Meteorology Atmospheric Thickness
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MET 61 21 MET 61 Introduction to Meteorology
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MET 61 22 MET 61 Introduction to Meteorology Hypsometric Equation Combination of ideal gas law with hydrostatic balance. Relates atmospheric thickness with average temperature. Thickness of atmosphere relates to difference between two atmospheric layers; z t (m) = thickness between two pressure levels
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MET 61 23 MET 61 Introduction to Meteorology
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MET 61 24 MET 61 Introduction to Meteorology
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MET 61 26 MET 61 Introduction to Meteorology knots
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MET 61 27 MET 61 Introduction to Meteorology The rotation of the Earth Rockets, migrating birds, and large scale weather systems are all deflected due to the rotation of the Earth. The Earth’s rotation causes both – – The Coriolis Force is the name of this rotational force that deflects motion.
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MET 61 28 MET 61 Introduction to Meteorology The rotation of the Earth Rockets, migrating birds, and large scale weather systems are all deflected due to the rotation of the Earth. The Earth’s rotation causes both –Translational movement –Rotational movement The Coriolis Force is the name of this rotational force that deflects motion.
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MET 61 29 MET 61 Introduction to Meteorology
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MET 61 30 MET 61 Introduction to Meteorology
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MET 61 31 MET 61 Introduction to Meteorology
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MET 61 32 MET 61 Introduction to Meteorology Coriolis Force Affects direction, not speed of object Maximum at the poles Zero at the equator (only translational movement) - omega - Earth’s rotational rate =360 degrees/24 hours or v - wind speed - latitude
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MET 61 33 MET 61 Introduction to Meteorology Coriolis Force Affects direction, not speed of object Maximum at the poles Zero at the equator (only translational movement) F c =2 v sin - omega - Earth’s rotational rate =360 degrees/24 hours or v - wind speed - latitude 2 radians/86400 seconds=7.27x10 -5 s -1 Calculate Coriolis force for wind moving at 10m/s 2(7.27x10 -5 s -1 )(10m/s)(sin37)=8.8e-4 m/s 2
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MET 61 34 MET 61 Introduction to Meteorology Coriolis Force Take home message: –N. Hem - deflects air to the right –S. Hem - deflects air to the left –Relatively small acceleration, thus requires long periods of time to influence motion.
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MET 61 35 MET 61 Introduction to Meteorology Geostrophic balance Geostrophic balance is balance between: and Result: flow of air is parallel to isobars
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MET 61 36 MET 61 Introduction to Meteorology Geostrophic balance Geostrophic balance is balance between: Pressure gradient force and Coriolis force Result: flow of air is parallel to isobars friction is assumed to be zero
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MET 61 37 MET 61 Introduction to Meteorology Geostrophic Wind example 1000 mb 1004 mb 1008 mb Northern Hemisphere
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MET 61 38 MET 61 Introduction to Meteorology Geostrophic Wind example L H 1000 mb 1004 mb 1008 mb Pressure Gradient Force Geostrophic Wind Coriolis Force Northern Hemisphere
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MET 61 39 MET 61 Introduction to Meteorology
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MET 61 40 MET 61 Introduction to Meteorology
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MET 61 41 MET 61 Introduction to Meteorology
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MET 61 42 MET 61 Introduction to Meteorology
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A A C C B B 1.Indicate with arrows the pressure gradient and Coriolis force at A, B and C. 2.Indicate the direction of the wind at each point. 3.Which point do you think the wind will be stronger?
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MET 61 44 MET 61 Introduction to Meteorology Geostrophic Wind Assume friction is zero Flow is parallel to isobars Balance between pressure gradient and Coriolis force - density, f - Coriolis parameter (2 sin v - wind speed d – distance between isobars p - pressure
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MET 61 45 MET 61 Introduction to Meteorology Geostrophic Wind Assume friction is zero Flow is parallel to isobars Balance between pressure gradient and Coriolis force - density, f - Coriolis parameter (=2 sin V g - geostrophic wind speed d – distance between isobars p – pressure difference
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MET 61 46 MET 61 Introduction to Meteorology http://www.met.sjsu.edu/weather/avn.html
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MET 61 47 MET 61 Introduction to Meteorology Estimate the geostrophic wind speed for this situation
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MET 61 48 MET 61 Introduction to Meteorology Assume (500mb) = 0.71 kg/m 3 d=200km=2x10 5 m p=4mb=400N/m 2 F=2 sin =9.34x10 -5 V g ~ 30 m/s
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MET 61 49 MET 61 Introduction to Meteorology http://www.met.sjsu.edu/weather/avn.html
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MET 61 50 MET 61 Introduction to Meteorology Geostrophic Wind with Friction 1000 mb 1004 mb 1008 mb Northern Hemisphere
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MET 61 51 MET 61 Introduction to Meteorology Geostrophic Wind with Friction L H 1000 mb 1004 mb 1008 mb Pressure Gradient Force Geostrophic Wind Coriolis Force Northern Hemisphere Friction Friction decreases speed of wind, thus Coriolis force is weaker.
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MET 61 52 MET 61 Introduction to Meteorology
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MET 61 53 MET 61 Introduction to Meteorology
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MET 61 54 MET 61 Introduction to Meteorology
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MET 61 55 MET 61 Introduction to Meteorology A B
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MET 61 56 MET 61 Introduction to Meteorology A B
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MET 61 57 MET 61 Introduction to Meteorology
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MET 61 58 MET 61 Introduction to Meteorology Jet Stream Result of North-South temperature gradient Stronger the pressure gradient, stronger the zonal wind. Kinks in jet stream due to wave instability: Result is exchange of heat from tropics to poles
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MET 61 59 MET 61 Introduction to Meteorology
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MET 61 60 MET 61 Introduction to Meteorology
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MET 61 61 MET 61 Introduction to Meteorology
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MET 61 62 MET 61 Introduction to Meteorology
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MET 61 63 MET 61 Introduction to Meteorology Terminology Cyclone: Anticyclone: At the surface, pressure cells are often closed. However, at higher altitudes, pressure cells are often elongated, forming ridges and troughs. –Low pressure systems - –High pressure systems -
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MET 61 64 MET 61 Introduction to Meteorology Terminology Cyclone: Anticyclone: At the surface, pressure cells are often closed. However, at higher altitudes, pressure cells are often elongated, forming ridges and troughs. –Low pressure systems - –High pressure systems - refers to closed low pressure system refers to a closed high pressure system Troughs Ridges
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MET 61 65 MET 61 Introduction to Meteorology Upper atmosphere pressure gradients Meteorologist often examine the upper level pressure gradients to determine the prevailing weather conditions. However, it is not convenient to simply calculate the pressure gradient because of it’s dependence on density. Rather, meteorologist calculate the height of a particular pressure surface. The slope of these heights determines the pressure gradient force.
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MET 61 66 MET 61 Introduction to Meteorology
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MET 61 67 MET 61 Introduction to Meteorology Soccer example x 12m F c =2 v sin , where, 2 = 1.45x10 -4 s -1 Say, v=12m/s, thus t=1s F c =2 v sin =(1.45x10 -4 s -1 )(12m/s)(sin 37)=1.05 x 10 -3 m/s 2 Note, that F c is really the acceleration, a. So, from x=v 0 t + ½at 2, then if v0 = 0 we have x= ½at 2 = (0.5)(1.05 x 10 -3 m/s 2 )(1s) 2 =5.2 x 10 -3 m = 0.52 mm
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MET 61 68 MET 61 Introduction to Meteorology Quiz 3: Part A 1.Write down the component form of the Geostrophic wind. 2.Explain the difference between the total derivative and the local derivative, and show how these are different mathematically.
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MET 61 69 MET 61 Introduction to Meteorology Quiz 3: Part B 1.Write down the component form of the momentum equations. Be sure to show all your work (how you got each term). 2.For each term in your above equations, provide a physical description (explanation) for what it means.
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MET 61 70 MET 61 Introduction to Meteorology 3.Indicate the temperature advection at points A and B. Justify your answer. B A
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MET 61 71 MET 61 Introduction to Meteorology Quiz 2: Part A Explain in words why the jet stream is westerly in both the northern and southern hemispheres. Describe the three basic conservations laws?
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MET 61 72 MET 61 Introduction to Meteorology Activity 9: Due April 11 th 1.Use links found on the department web page to explore wind speed and direction from maps of model output such as shown in class. From these maps, calculate geostrophic wind using either pressure or height information (if you use height, then use equations given on pg 188-189 of Stull). Compare your answer with model wind information (isotachs). Show calculations and maps from at least two locations. 2. Compute by how much a soccer ball will be deflected during a 12m penalty kick due to the coriolis force.
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