MET 61 Introduction to Meteorology - Lecture 5

Slides:



Advertisements
Similar presentations
4. 2 Moist air thermodynamics (Reading Text
Advertisements

Chapter 5 Atmospheric Moisture. The process whereby molecules break free of liquid water is known as evaporation. The opposite process is condensation,
Lecture 8 Saturated Adiabatic Processes Phase Changes Liquid Gas (Vapor) Energy absorbed Energy released Solid (Ice) melting evaporation deposition freezing.
Atmospheric Humidity. Global water cycle: precipitation = evaporation.
Section 04 Thermodynamics Adiabatic Processes Lesson 10/11.
38 Atmospheric Stability Stable vs. Unstable Dry and Moist Adiabatic Processes Skew-T diagrams.
L14 Physics of dry air and moist air
Outline Further Reading: Chapter 06 of the text book - adiabatic processes - dry and wet adiabatic lapse rates - ascent versus descent Natural Environments:
Weather Water in the Atmosphere May 14, Precipitation Precipitation is any form of water that falls from a cloud. Water vapor is the source of all.
Moist Processes ENVI1400: Lecture 7. ENVI 1400 : Meteorology and Forecasting2 Water in the Atmosphere Almost all the water in the atmosphere is contained.
Lecture 7 Water Vapor.
Tephigrams ENVI1400 : Lecture 8.
Stability & Skew-T Diagrams
Class 4a: Atmospheric moisture. Introduction to water Earth’s temperature  special properties of water.
Textbook chapter 2, p chapter 3, p chapter 4, p Stability and Cloud Development.
Outline Further Reading: Chapter 06 of the text book - stability and vertical motions - five examples - orographic precipitation Natural Environments:
MET 61 1 MET 61 Introduction to Meteorology MET 61 Introduction to Meteorology - Lecture 4 “Heat in the atmosphere” Dr. Eugene Cordero San Jose State University.
Copyright © 2011 R. R. Dickerson & Z.Q. Li 1 Continuing to build a cloud model: Consider a wet air parcel Parcel boundary As the parcel moves assume no.
Humidity, Saturation, and Stability
MET 61 1 MET 61 Introduction to Meteorology MET 61 Introduction to Meteorology - Lecture 3 Thermodynamics I Dr. Eugene Cordero San Jose State University.
HUMIDITY Chapter 17 Test 4 material. ASSIGNMENT – 10 POINTS WRITE A 1 TO 2 PAGE REPORT ON “THE IMPACT OF THE TRI-STATE TORNADO IN ILLINOIS” DUE IN ONE.
* Reading Assignments: All sections of Chapter 5.
Moisture and Atmospheric Stability
Warm Up 3/14 Which gas is most important for understanding atmospheric processes? a. water vapor c. carbon dioxide b. oxygen d. ozone What is true.
Chapter 4 Moisture and Atmospheric Stability. Steam Fog over a Lake.
The Atmosphere: An Introduction to Meteorology, 12th
Moisture and Clouds Weather Unit When you see this megaphone, Click it for audio information Weather Unit When you see this megaphone, Click it for audio.
Lesson 15 Adiabatic Processes
Chapter 11 Section 2 State of Atmosphere. Temperature vs. Heat Temperature: measures the movement of molecules  Faster = Warmer  Slower = Colder  Measured.
Moisture Variables on Skew T Log P Diagram AOS 330 LAB 8.
Prof. Fred Remer University of North Dakota Phase Changes and Latent Heat Where’s the heat? Solid Liquid Gas.
1 The Thermodynamic Diagram Adapted by K. Droegemeier for METR 1004 from Lectures Developed by Dr. Frank Gallagher III OU School of Meteorology.
Atmospheric Moisture Vapor pressure (e, Pa) The partial pressure exerted by the molecules of vapor in the air. Saturation vapor pressure (e s, Pa ) The.
A&OS C110/C227: Review of thermodynamics and dynamics II Robert Fovell UCLA Atmospheric and Oceanic Sciences 1.
Objectives Review Vocabulary
ThermodynamicsM. D. Eastin Water Vapor in the Air How do we compute the dewpoint temperature, the relative humidity, or the temperature of a rising air.
Water in the Atmosphere Evaporation Condensation and Cloud Formation.
Lab 6: Saturation & Atmospheric Stability
Office Hours Tue: 12:30 PM to 2:30 PM Wed: 9:00 AM to 10:30 AM & 12:00 PM to 2:00 PM Thr: 9:00 AM to 10:30 AM Course Syllabus can be found at:
Copyright © 2013 R. R. Dickerson11 Professor Russell Dickerson Room 2413, Computer & Space Sciences Building Phone(301) web.
Copyright © 2013 R. R. Dickerson11 Professor Russell Dickerson Room 2413, Computer & Space Sciences Building Phone(301) web.
EARTH SCIENCE Prentice Hall EARTH SCIENCE Tarbuck Lutgens 
Exam 2 Review AOS 121 November Geostrophic Balance and Geostrophic Winds Balance between the pressure gradient force and Coriolis force Will.
Water in the Atmosphere Lab 5 October 5, Water Is Important!!!
Unit 7: Severe Weather Lecture 1 Objectives: E4.3f - Describe how mountains, frontal edging (including dry lines) convection, and convergence form clouds.
Lecture 4 Precipitation (1)
Atmospheric Moisture. Water in the Atmosphere Water vapor is the source of all condensation and precipitation Essentially all water on Earth is conserved.
Moist adiabatic process Moist adiabaticDry adiabatic.
Water in the Atmosphere Chapter 18, Section 1. Water in the Atmosphere  Precipitation – any form of water that falls from a cloud  When it comes to.
+ Moisture and Stability Chapter 4. + The Hydrologic Cycle Hydrologic Cycle: the circulation of Earth’s water supply The cycle illustrates the continuous.
Thermodynamics Lee, Jinuk Park, sang ah Yuk, kyeong min Group 6.
CH 18 Review Water in the Atmosphere. If the specific humidity is 5 g/kg and the water vapor capacity is 10 g/kg, the relative humidity is… –A. 25% –B.
Moisture  There are several methods of expressing the moisture content (water in vapor form) of a volume of air.  Vapor Pressure: The partial pressure.
 ADIABATIC HEATING/COOLING A. Adiabatic temperature changes occur when 1. Air is compressed as pressure increases a. Motion of air molecules increases.
Water Cycle, Cloud Formation, and Severe Weather.
Chapter 18 Moisture, Clouds, & Precipitation Water in the Atmosphere When it comes to understanding atmospheric processes, water vapor is the most.
STATE OF THE ATMOSPHERE Advanced Earth Science. Temperature vs. Heat  NOT THE SAME THING!!  Temperature measures how fast or slow molecules move around.
A Major Component of Earth’s Weather. The Hydrologic Cycle Water can exist as a solid, liquid, or gas on Earth. The movement of water from different reservoirs.
I. Water’s Changes of State 18.1 Water in the Atmosphere  A) Precipitation is any form of water that falls from a cloud.  1) When studying the ATM, H20.
STATE OF THE ATMOSPHERE Earth Science. Temperature vs. Heat  NOT THE SAME THING!!  Temperature measures how fast or slow molecules move around (their.
Chapter 18 Moisture, Clouds, and Precipitation When it comes to understanding atmospheric processes, water vapor is the most important gas in the atmosphere!
Cloud Formation: Lifting Processes Atmospheric Lifting In order for air to form clouds, the air must be lifted and rise in altitude There are 4 types.
Atmospheric Moisture (Text Pg 84-92)
Monday’s lesson (At the end the lesson you will be able to…) Describe the changes in temperature with height through the lower layers of the atmosphere.
Stability and Introduction to the Thermodynamic Diagram
Lesson 1 Task 1 Can you draw a fully labelled diagram to show the ‘day model’ of radiation balance in the earth’s energy budget in 5 minutes on these.
Topic 3B: Moist Thermodynamics
Copyright © 2013 R. R. Dickerson
Fall 2000 Author: Dr. Ken Crawford University of Oklahoma
1. Transformations of Moist Air
Presentation transcript:

MET 61 Introduction to Meteorology - Lecture 5 Moisture (II) Dr. Eugene Cordero San Jose State University Stull: Pg 43-48, pg 95-102, 104, 109-112 W&H: Chap 3, Pg 85-93 Class Outline: LCL Moist Lapse Rate Normand’s rule MET 61 Introduction to Meteorology

Eulerian vs. Lagrangian Refer to different perspectives or frames of reference: Eulerian refers to: Lagrangian means that Examples: MET 61 Introduction to Meteorology

Eulerian vs. Lagrangian Refer to different perspectives or frames of reference: Eulerian refers to: examining a fixed volume in space. Lagrangian means that we following an air parcel as it moves in the atmosphere. Examples: MET 61 Introduction to Meteorology

Adiabatic/pseudoadiabatic A parcel of air rises in the atmosphere at the dry adiabatic lapse rate until air is saturated. If all condensation products (rain,snow) remain in the parcel – MET 61 Introduction to Meteorology

Adiabatic/pseudoadiabatic A parcel of air rises in the atmosphere at the dry adiabatic lapse rate until air is saturated. Further lifting results in condensation releasing latent heat. If all condensation products (rain,snow) remain in the parcel – adiabatic process MET 61 Introduction to Meteorology

Adiabatic/pseudoadiabatic If condensation products fall out (rain out), then not an adiabatic (or reversible) process, rather a - However, the amount of heat lost is relatively small, thus the saturated adiabatic lapse rate is similar to pseudoadiabatic lapse rate. MET 61 Introduction to Meteorology

Adiabatic/pseudoadiabatic If condensation products fall out (rain out), then not an adiabatic (or reversible) process, rather a - -pseudoadiabatic MET 61 Introduction to Meteorology

Saturated adiabatic lapse rate The dry adiabatic lapse rate applies to moist air provided it’s unsaturated. The saturated-adiabatic lapse rate is less than the dry rate because of: - MET 61 Introduction to Meteorology

Saturated adiabatic lapse rate The dry adiabatic lapse rate applies to moist air provided it’s unsaturated. Saturated air: e.g. clouds and fog The saturated-adiabatic lapse rate is less than the dry rate because of: -release of latent heat during condensation Dry adiabats: constant potential temperature Moist or saturated adiabats: constant equivalent potential temperature MET 61 Introduction to Meteorology

Thermodynamic Diagram Green Dry Adiabats Red Moist Adiabats Yellow Saturation Mixing Ratio MET 61 Introduction to Meteorology

MET 61 Introduction to Meteorology Skew-T Log-p Diagram MET 61 Introduction to Meteorology

Equivalent potential temperature The equilivant potential temperature, e, refers to the case where a parcel is expanded pseudoadiabatically until all the vapor has condensed, released its latent heat and fallen out. Then the parcel is compressed dry adiabatically to the 1000mb. The final temperature at 1000mb is the equivalent potential temperature. MET 61 Introduction to Meteorology

MET 61 Introduction to Meteorology Wet bulb temperature Is defined as Tw. Example: MET 61 Introduction to Meteorology

MET 61 Introduction to Meteorology Wet bulb temperature Is defined as Tw. By definition it is the lowest temperature a volume of air can be cooled through evaporation. Example: MET 61 Introduction to Meteorology

Wet bulb potential temperature Is defined by w. If the moist adiabat is followed through the wet-bulb temperature of the parcel back to 1000mb, the temperature is called the wet-bulb potential temperature, w MET 61 Introduction to Meteorology

MET 61 Introduction to Meteorology Normand’s rule This rule states that on a pseudoadiabatic chart, the lifting condensation level of an air parcel is at the intersection of three other lines: the potential temperature line which passes through the The equivalent potential temperature line which passes through the Saturation mixing ratio line which passes through MET 61 Introduction to Meteorology

MET 61 Introduction to Meteorology Normand’s rule This rule states that on a pseudoadiabatic chart, the lifting condensation level of an air parcel is at the intersection of three other lines: the potential temperature line which passes through the Temperature and pressure of parcel The equivalent potential temperature line which passes through the Web bulb temperature and pressure of parcel Saturation mixing ratio line which passes through Dew point and pressure of the parcel MET 61 Introduction to Meteorology

MET 61 Introduction to Meteorology Skew-T MET 61 Introduction to Meteorology

MET 61 Introduction to Meteorology Normand’s rule LCL pressure Constant  Constant rs P Td Tw T Constant e 1000mb w temperature MET 61 Introduction to Meteorology

MET 61 Introduction to Meteorology Skew-T MET 61 Introduction to Meteorology

MET 61 Introduction to Meteorology

Irreversible condensation processes Consider a parcel lifted above its LCL so that condensation occurs. If precipitation falls out and the parcel returns to original pressure (adiabatically), then how does the following change? Increase, decrease of stay the same? a) T b)  r (mixing ratio) RH Td Tw MET 61 Introduction to Meteorology

Irreversible condensation processes Net increase in temperature and  Decrease in moisture (i.e. dew point, wet bulb temp etc.) No change in equivalent potential temperature or wet-bulb potential temp MET 61 Introduction to Meteorology

MET 61 Introduction to Meteorology

MET 61 Introduction to Meteorology In the figure below, explain why the temperature and dew point on the windward side of the mountain are different from the leeward side. MET 61 Introduction to Meteorology

MET 61 Introduction to Meteorology Question 1a A parcel of air with initial temperature of 40°C and dew point of 20°C is lifted adiabatically from the 1000 hPa level. Determine it’s thermodynamic state (Temp, RH) @ 800 hPa If the parcel raises further, determine the lifting condensation level and temperature at that level. If the parcel is lifted further up to 500 hPa, what is the final temperature and how much water is condensed during the rise? If 2g/kg of precipitation falls out during the rise, then if the parcel descends, what is the new LCL and what is the thermo state (Temp, RH) at 800 hPa? At 800 hPa, determine the wet bulb temperature and the wet bulb potential temperature. MET 61 Introduction to Meteorology

MET 61 Introduction to Meteorology Activity 4 (Due Feb 21st) An air parcel at 800mb has a temperature of 20°C and a dew point temperature of –2.5°C. Determine the LCL of the parcel Determine the state of the parcel if lifted to 400mb. How much water is condensed out? If 1 g/kg of water is rained out, what is the new LCL and thermodynamic state of the parcel at 800mb? I think that it would be worthwhile at this introductory lecture to provide some definitions that you may have never thought of before Go through..... Climatology also has a distinctly Geographical component to it - we often consider what gives one region or locality a different climate from another. However, although this course is put on by Geography and Environmental Science, there are clear components of meteorology and climatology in it. In the course we will not be taking a particularly mathematical approach to atmospheric science, but everything we will talk about will be based on sound physical principles. MET 61 Introduction to Meteorology

MET 61 Introduction to Meteorology Question 2 An air parcel at 800mb has a temperature of 20°C and a dew point temperature of –2.5°C. Determine the LCL of the parcel Determine the state of the parcel if lifted to 400mb. How much water is condensed out? If 1 g/kg of water is rained out, what is the new LCL and thermodynamic state of the parcel at 800mb? MET 61 Introduction to Meteorology

MET 61 Introduction to Meteorology Quiz #2: Part B The saturation mixing ratio can be described as: For typical values of the Earth’s temperature, show that MET 61 Introduction to Meteorology

MET 61 Introduction to Meteorology Activity: An air parcel at 950 mb has a temperature of 14°C and a saturation mixing ratio of 4.5g/kg. A) What is the wet bulb potential temperature of the air? The air parcel is lifted a further 200mb by passing over a mountain, and 70% of the water vapor that is condensed out by the ascent is removed by precipitation. B) Determine the temperature, potential temperature, mixing ratio and web-bulb potential temperature of the air after it has returned to the 1000 mb level on the other side of the mountain. MET 61 Introduction to Meteorology

MET 61 Introduction to Meteorology Question 1 A parcel of air with initial temperature of 15°C and dew point of 2°C is lifted adiabatically from the 1000mb level. Determine its lifting condensation level and temperature at that level. If the parcel is lifted a further 200 mb above it’s lifting condensation level, what is its final temperature and how much water is condensed during the rise? MET 61 Introduction to Meteorology