Thermodynamic Diagrams (Based on Ch.5 of Hess) [For the Classical Equation Editor: ( Dq 0 )]
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Meteorology – Lecture 19
Meteorology – Lecture 19 Robert Fovell [email protected] 1 Important notes • These slides show some figures and videos prepared by Robert G. Fovell (RGF) for his “Meteorology” course, published by The Great Courses (TGC). Unless otherwise identified, they were created by RGF. • In some cases, the figures employed in the course video are different from what I present here, but these were the figures I provided to TGC at the time the course was taped. • These figures are intended to supplement the videos, in order to facilitate understanding of the concepts discussed in the course. These slide shows cannot, and are not intended to, replace the course itself and are not expected to be understandable in isolation. • Accordingly, these presentations do not represent a summary of each lecture, and neither do they contain each lecture’s full content. 2 Animations linked in the PowerPoint version of these slides may also be found here: http://people.atmos.ucla.edu/fovell/meteo/ 3 Mesoscale convective systems (MCSs) and drylines 4 This map shows a dryline that formed in Texas during April 2000. The dryline is indicated by unfilled half-circles in orange, pointing at the more moist air. We see little T contrast but very large TD change. Dew points drop from 68F to 29F -- huge decrease in humidity 5 Animation 6 Supercell thunderstorms 7 The secret ingredient for supercells is large amounts of vertical wind shear. CAPE is necessary but sufficient shear is essential. It is shear that makes the difference between an ordinary multicellular thunderstorm and the rotating supercell. The shear implies rotation. -
Thermodynamics
Copyright© 2004, School of Meteorology, University of Oklahoma. Rev 04/04 Knowledge Expectations for METR 3213 Physical Meteorology I: Thermodynamics Purpose: This document describes the principal concepts, technical skills, and fundamental understanding that all students are expected to possess upon completing METR 3213, Physical Meteorology I: Thermodynamics. Individual instructors may deviate somewhat from the specific topics and order listed here. Pre-requisites: Grade of C or better in MATH 2443, PHYS 2524, METR 2024 (or 2413). Students should have a basic understanding of functions of several variables, partial derivatives, differentials of multivariate functions, line and surface integrals, the basics of state variables such as temperature, pressure, density, and volume, and basic energy concepts prior to starting this course. Goal of the Course: This course introduces the physical processes associated with atmospheric composition, basic radiation and energy concepts, the equation of state, the zeroth, first, and second law of thermodynamics, the thermodynamics of dry and moist atmospheres, thermodynamic diagrams, statics, and atmospheric stability. Topical Knowledge Expectations I. Basic Radiation Principles. • Understand the basic physical concepts of radiative transfer of energy, including radiation characteristics, quantities and units. • Understand the concepts of emission, absorption, and scattering of radiation. • For solar (short-wave) radiation, understand the definition of the albedo and know typical values for different surfaces. Understand the dominant causes of absorption and scattering of solar radiation in the atmosphere. • For long-wave radiation in the atmosphere, understand the important constituents (greenhouse gases) and processes affecting emission and absorption. • Be familiar and work problems using Wien’s Law, Stefan Boltzmann’s Law, and the Inverse Square Law. -
Chapter 5 Frictional Boundary Layers
Chapter 5 Frictional boundary layers 5.1 The Ekman layer problem over a solid surface In this chapter we will take up the important question of the role of friction, especially in the case when the friction is relatively small (and we will have to find an objective measure of what we mean by small). As we noted in the last chapter, the no-slip boundary condition has to be satisfied no matter how small friction is but ignoring friction lowers the spatial order of the Navier Stokes equations and makes the satisfaction of the boundary condition impossible. What is the resolution of this fundamental perplexity? At the same time, the examination of this basic fluid mechanical question allows us to investigate a physical phenomenon of great importance to both meteorology and oceanography, the frictional boundary layer in a rotating fluid, called the Ekman Layer. The historical background of this development is very interesting, partly because of the fascinating people involved. Ekman (1874-1954) was a student of the great Norwegian meteorologist, Vilhelm Bjerknes, (himself the father of Jacques Bjerknes who did so much to understand the nature of the Southern Oscillation). Vilhelm Bjerknes, who was the first to seriously attempt to formulate meteorology as a problem in fluid mechanics, was a student of his own father Christian Bjerknes, the physicist who in turn worked with Hertz who was the first to demonstrate the correctness of Maxwell’s formulation of electrodynamics. So, we are part of a joined sequence of scientists going back to the great days of classical physics. -
Vertical Structure of the Atmosphere
Chapter 5: Vertical structure of the atmosphere 5.1 Sounding of the atmosphere Fig.2.1 indicates that globally temperature decreases with altitude in the troposphere. However, already Fig.4.2 showed that locally the temperature can also stay constant with height (isothermal layer), or even increase (inversion layer). The actual stratification of the atmosphere is highly variable in space and time and is, thus, routinely probed by all national weather services. Generally, this probing consists of launching a radiosonde every 3 to 6 hours. Fig. 5.1: Photo sequence of the launching of a radiosonde on a ship and (on the right) the schematic structure of a radiosonde; La METEO de A à Z; Météo France ISBN/2.234.022096 The balloon is filled with hydrogen. Attached is a parachute to assure a soft landing, an aluminium foil to assure a high radar reflectivity and the actual sonde containing instruments for measuring pressure, temperature and humidity. For a description of the humidity sensor see chapter 3.4.1. Temperature, humidity and pressure are radiotransmitted to the station at the ground, while wind speed and wind direction are derived from telemetric data following the balloon by radar. The vertical profile of the atmosphere is then transferred on thermodynamic diagram papers. An eXample of such a representation can be found in Fig. 5.3. The diagram paper used here is a skew T –log p diagram paper which has a logarithmic aXis of pressure in the vertical and the isotherms are straight lines tilted 45° with respect to the horizontal. Other diagram papers are known also. -
HODOGRAPHS and SEVERE WEATHE B E. W. Mccaul. Jr.. Steve
HODOGRAPHS AND SEVERE WEATHE B E. W. McCaul. Jr.. Steve Lazarus. Fred Carr One ingredient which is believed to be important in governing the morphology of thunderstorms is the profile of vertical shear in the environment which supports the storms. Numerous observational and theoretical studies have shown that storms which form in weakly-sheared environments tend to have non-steady circulations (multicells), while those that form in strongly-sheared environments can develop steady, persistent circulations (supereells). Although intuition suggests that strong shear can only inhibit the formation of organized updrafts, this tendency is partly offset by the ability of shear flows to generate a variety of hydrodynamical instabilities which allow for the possibility of updraft growth. Forecasters who work in areas of the country prone to outbreaks of severe weather should be prepared to recognize not only the thermodynamic conditions but also the vertical shear conditions favorable for various types of severe storms. Inspection of temperature and moisture soundings can reveal the presence of the necessary thermodynamic instability, while inspection of wind profiles (hodographs) can help diagnose whether conditions are right for the development of tornadoes. Hodographs can be drawn either as plots of u (z) vs. v (z) in Cartesian coordinates or V (z) vs. 8 (z) in cylindrical coordinates. In either case, the actual shape of the hodograph will be the same for any given wind profile. On the OU Meteorology weather computer, hodographs from any raob station may be plotted using "mchodo" in GEMPAK. Each plotted hodograph represents nothing more than the curve which connects, in order of ascending altitude, the tips of all the observed wind vectors from a sounding, with the bases of the vectors attached to a common origin. -
ESCI 241 – Meteorology Lesson 8 - Thermodynamic Diagrams Dr
ESCI 241 – Meteorology Lesson 8 - Thermodynamic Diagrams Dr. DeCaria References: The Use of the Skew T, Log P Diagram in Analysis And Forecasting, AWS/TR-79/006, U.S. Air Force, Revised 1979 An Introduction to Theoretical Meteorology, Hess GENERAL Thermodynamic diagrams are used to display lines representing the major processes that air can undergo (adiabatic, isobaric, isothermal, pseudo- adiabatic). The simplest thermodynamic diagram would be to use pressure as the y-axis and temperature as the x-axis. The ideal thermodynamic diagram has three important properties The area enclosed by a cyclic process on the diagram is proportional to the work done in that process As many of the process lines as possible be straight (or nearly straight) A large angle (90 ideally) between adiabats and isotherms There are several different types of thermodynamic diagrams, all meeting the above criteria to a greater or lesser extent. They are the Stuve diagram, the emagram, the tephigram, and the skew-T/log p diagram The most commonly used diagram in the U.S. is the Skew-T/log p diagram. The Skew-T diagram is the diagram of choice among the National Weather Service and the military. The Stuve diagram is also sometimes used, though area on a Stuve diagram is not proportional to work. SKEW-T/LOG P DIAGRAM Uses natural log of pressure as the vertical coordinate Since pressure decreases exponentially with height, this means that the vertical coordinate roughly represents altitude. Isotherms, instead of being vertical, are slanted upward to the right. Adiabats are lines that are semi-straight, and slope upward to the left. -
Thickness and Thermal Wind
ESCI 241 – Meteorology Lesson 12 – Geopotential, Thickness, and Thermal Wind Dr. DeCaria GEOPOTENTIAL l The acceleration due to gravity is not constant. It varies from place to place, with the largest variation due to latitude. o What we call gravity is actually the combination of the gravitational acceleration and the centrifugal acceleration due to the rotation of the Earth. o Gravity at the North Pole is approximately 9.83 m/s2, while at the Equator it is about 9.78 m/s2. l Though small, the variation in gravity must be accounted for. We do this via the concept of geopotential. l A surface of constant geopotential represents a surface along which all objects of the same mass have the same potential energy (the potential energy is just mF). l If gravity were constant, a geopotential surface would also have the same altitude everywhere. Since gravity is not constant, a geopotential surface will have varying altitude. l Geopotential is defined as z F º ò gdz, (1) 0 or in differential form as dF = gdz. (2) l Geopotential height is defined as F 1 z Z º = ò gdz (3) g0 g0 0 2 where g0 is a constant called standard gravity, and has a value of 9.80665 m/s . l If the change in gravity with height is ignored, geopotential height and geometric height are related via g Z = z. (4) g 0 o If the local gravity is stronger than standard gravity, then Z > z. o If the local gravity is weaker than standard gravity, then Z < z. -
IMS4 Weather Studio
IMS4 Weather Studio IMS4 Weather Studio is a unique tool for processing, analyzing and graphic presentation of the surface and upper air meteorological, radiation and climatological data. Processing, analyzing and presentation of data of various kinds Meteorological and Standalone application or integrated Supports standard Archive of various settings Pilot Briefing with IMS4 Message switching meteorological saved by individual users and data processing server formats The easy-to-use tool provides convenient way for objective • Topography analysis and displaying of complex data - real-time data • Actual or historical weather data from SYNOP and METAR distribution systems (GTS), SADIS, as well as data outputs from bulletins Numeric Weather Prediction models (NWPs). • NWP model output in GRIB format • Satellite and radar information IMS4 Weather Studio has an inestimable wide use in • SIGWX charts in BUFR format meteorological institutions, forecasting services, and crisis • Lightning locations centers, airports, at climatological research and dispersion • Flight Information Region (FIR) modeling and for many other users. Each layer allows customization by providing a wide choice of Layered maps setting options and the stored customized layer configurations The IMS4 Weather Studio allows easy creating, viewing and can be applicated easily over the maps. printing of the layered maps. The layers include among others: 1 IMS4 Weather Studio Visualization of thermodynamic diagram from local temp IMS4 Weather Studio - GRIB Model (station Prostějov, 1.5.2014 – 00.00, 12.00) Weather data Thermodynamic diagram Weather data can be displayed as numeric values at selected The IMS4 Weather Studio offers a tool to draw thermodynamic locations or grid points, or interpolated in the forms of color diagram. -
5 Atmospheric Stability
Copyright © 2015 by Roland Stull. Practical Meteorology: An Algebra-based Survey of Atmospheric Science. 5 ATMOSPHERIC STABILITY Contents A sounding is the vertical profile of tempera- ture and other variables in the atmosphere over one Building a Thermo-diagram 119 geographic location. Stability refers to the ability Components 119 of the atmosphere to be turbulent, which you can Pseudoadiabatic Assumption 121 determine from soundings of temperature, humid- Complete Thermo Diagrams 121 ity, and wind. Turbulence and stability vary with Types Of Thermo Diagrams 122 time and place because of the corresponding varia- Emagram 122 tion of the soundings. Stüve & Pseudoadiabatic Diagrams 122 We notice the effects of stability by the wind Skew-T Log-P Diagram 122 gustiness, dispersion of smoke, refraction of light Tephigram 122 Theta-Height (θ-z) Diagrams 122 and sound, strength of thermal updrafts, size of clouds, and intensity of thunderstorms. More on the Skew-T 124 Thermodynamic diagrams have been devised Guide for Quick Identification of Thermo Diagrams 126 to help us plot soundings and determine stability. Thermo-diagram Applications 127 As you gain experience with these diagrams, you Thermodynamic State 128 will find that they become easier to use, and faster Processes 129 than solving the thermodynamic equations. In this An Air Parcel & Its Environment 134 chapter, we first discuss the different types of ther- Soundings 134 modynamic diagrams, and then use them to deter- Buoyant Force 135 mine stability and turbulence. Brunt-Väisälä Frequency 136 Flow Stability 138 Static Stability 138 Dynamic Stability 141 Existence of Turbulence 142 Building a Thermo-diagram Finding Tropopause Height and Mixed-layer Depth 143 Tropopause 143 Components Mixed-Layer 144 In the Water Vapor chapter you learned how to Review 145 compute isohumes and moist adiabats, and in Homework Exercises 145 the Thermodynamics chapter you learned to plot Broaden Knowledge & Comprehension 145 dry adiabats. -
Thermodynamic Diagrams
ESCI 341 – Atmospheric Thermodynamics Lesson 17 – Thermodynamic Diagrams References: Introduction to Theoretical Meteorology, S.L. Hess, 1959 Glossary of Meteorology, AMS, 2000 GENERAL Thermodynamic diagrams are used to graphically display the relation between two of the thermodynamic variables T, V, and p. Process lines represent specific thermodynamic processes on the diagram. Important process lines are Isotherms Isobars Adiabats Pseudoadiabats Isohumes A useful thermodynamic diagram should have the following general properties The area enclosed by a cyclic process should be proportional to the work done during the process. As many of the process lines as possible should be straight. The angle between the isotherms and adiabats should be as close to 90 as possible. CREATING A DIAGRAM WITH AREA PROPORTIONAL TO WORK We’ve previously used the p- diagram. Since work per unit mass is defined as dw pd the area on a p- diagram is proportional to work. The p- diagram is not very useful for meteorologists because The angle between isotherms and adiabats is very small Process lines aren’t very straight Volume is not a convenient thermodynamic variable for meteorology For meteorology it would be useful to have a diagram that uses T and p as the thermodynamic variables. However, we can’t just arbitrarily use T and p and hope that area will be proportional to work. We have to find a way of setting up the axes of our diagram so that area will be proportional to work. Let the variables for the axes be X and Y, and let X and Y be functions of the thermodynamic variables. -
MSE3 Ch05 Stability
chapter 5 Copyright © 2011, 2015 by Roland Stull. Meteorology for Scientists and Engineers, 3rd Ed. Stability contentS A sounding is the vertical profile of tem- perature and other variables in the atmo- Building a Thermo-diagram 119 sphere over one geographic location. Sta- Components 119 5 bility refers to the ability of the atmosphere to be Pseudoadiabatic Assumption 121 turbulent. Stability is determined by temperature, Complete Thermo Diagrams 121 humidity, and wind profiles. Turbulence and stabil- Types Of Thermo Diagrams 122 ity vary with time and place because of the corre- Emagram 122 sponding variation of the soundings. Stüve & Pseudoadiabatic Diagrams 122 We notice the effects of stability by the: wind Skew-T Log-P Diagram 122 gustiness, dispersion of smoke, refraction of light Tephigram 122 Theta-Height (θ-z) Diagrams 122 and sound, strength of thermal updrafts, size of clouds, and intensity of thunderstorms. More on the Skew-T 124 Thermodynamic diagrams have been de- Guide for Quick Identification of Thermo Diagrams 126 vised to help us plot soundings and determine sta- Thermo-diagram Applications 127 bility. They look complicated at first, but with a bit Thermodynamic State 128 of practice they can make thermodynamic analysis Processes 129 much easier than solving sets of coupled equations. Parcels vs. Environment 134 In this chapter, we first discuss the different types Soundings 134 of thermodynamic diagrams, and then use them to Buoyancy 135 determine stability and turbulence. Brunt-Väisälä Frequency 136 Flow Stability 138 Static Stability 138 Dynamic Stability 141 Turbulence Determination 142 building a thermo-diagram Finding Tropopause Height & Mixed-layer Depth 143 Tropopause 143 components Mixed-Layer 144 In previous chapters, we learned how to compute Summary 145 isohumes (the Moisture chapter), dry adiabats Threads 145 (the Heat chapter), and moist adiabats (the Mois- Exercises 145 ture chapter). -
Student Study Guide Chapter 8
Adiabatic Lapse Rates 8 and Atmospheric Stability Learning Goals After studying this chapter, students should be able to: 1. describe adiabatic processes as they apply to the atmosphere (p. 174); 2. apply thermodynamic diagrams to follow the change of state in rising or sinking air parcels, and to assess atmospheric stability (pp. 179–189); and 3. distinguish between the various atmospheric stability types, and describe their causes and conse- quences (pp. 189–203). Summary 1. An adiabatic process is a thermodynamic process in which temperature changes occur without the addition or removal of heat. Adiabatic processes are very common in the atmosphere; rising Weather and Climate, Second Edition © Oxford University Press Canada, 2017 air cools because it expands, and sinking air warms because it is compressed. The rate of change of temperature in unsaturated rising or sinking air parcels is known as the dry adiabatic lapse rate (DALR). This rate is equal to 10°C/km. When rising air parcels are saturated, they cool at a slower rate because of the release of latent heat. Unlike the DALR, the saturated adiabatic lapse rate (SALR) is not constant, but we often use 6°C/km as an average value. 2. Potential temperature is the temperature an air parcel would have if it were brought to a pressure of 100 kPa. Potential temperature remains constant for vertical motions. 3. The lifting condensation level (LCL) is the height at which an air parcel wising from the surface will begin to condense. The LCL depends on the surface temperature and dew-point temperature. 4.