Simulating Adiabatic Parcel Rise Presentation by Anna Merrifield, Sarah Shackleton and Jeff Sussman.

Slides:



Advertisements
Similar presentations
LAB 6 10/16. Stability – Lapse Rate The rate at which a parcel cools as it rises. A dry* parcel cools at 10 degrees Celsius per kilometer***. A moist**
Advertisements

Atmospheric Stability
38 Atmospheric Stability Stable vs. Unstable Dry and Moist Adiabatic Processes Skew-T diagrams.
Stability & Movement Figure 7.1 A rock, like a parcel of air, that is in stable equilibrium will return to its original position when pushed. If the rock.
Atmospheric Stability
Atmospheric Stability and Cloud Formation. RECAP Mechanical equilibrium: stable, unstable, neutral. Adiabatic expansion/compression: no heat exchange.
Chapter 27 - Clouds Use of Power Point design and animations with permission from Dr. Joby Hilliker ( West Chester University, West Chester, PA.
Outline Further Reading: Chapter 06 of the text book - adiabatic processes - dry and wet adiabatic lapse rates - ascent versus descent Natural Environments:
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.
Lecture 5.2: Stability Are you stable or unstable? Does it depend on the situation?
AOSS 321, Winter 2009 Earth System Dynamics Lecture 11 2/12/2009 Christiane Jablonowski Eric Hetland
Outline Further Reading: Chapter 06 of the text book - stability and vertical motions - five examples - orographic precipitation Natural Environments:
AOS 100: Weather and Climate Instructor: Nick Bassill Class TA: Courtney Obergfell.
* Reading Assignments: All sections of Chapter 5.
Moisture and Atmospheric Stability
METEO 003 LAB 6 Due Friday Oct. 17 th. Chapter 8 Question 1 a,b,c Radiosonde: instrument carried by a weather balloon to measure atmospheric variables.
Air Pressure. State Variables Describe the “state” of the gas “Variable” means they can change Physicists use P, V, T, N and constant k Chemists use P,
Lapse Rates and Stability of the Atmosphere
Thermodynamics, Buoyancy, and Vertical Motion
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.
Thermodynamics, Buoyancy, and Vertical Motion Temperature, Pressure, and Density Buoyancy and Static Stability Adiabatic “Lapse Rates” Convective Motions.
Chapter 4 Moisture and Atmospheric Stability. Steam Fog over a Lake.
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
MET 102 Pacific Climates and Cultures Lecture 5: Water and Rising Air.
Chapter 11 Section 2 State of Atmosphere. Temperature vs. Heat Temperature: measures the movement of molecules  Faster = Warmer  Slower = Colder  Measured.
1 The Thermodynamic Diagram Adapted by K. Droegemeier for METR 1004 from Lectures Developed by Dr. Frank Gallagher III OU School of Meteorology.
CHAPTER 5 CLOUDS AND STABILITY CHAPTER 5 CLOUDS AND STABILITY.
Atmospheric Properties II Martin Visbeck DEES, Lamont-Doherty Earth Observatory
Clouds & Weather iClick Review Quiz. Warm air has the ability to hold ______________ water than cold air? A) more B) less C) same amount D) saltier.
Precipitation Hydrology (Spring 2013) Illinois State University Instructor: Eric Peterson.
Properties of the Atmosphere
The Atmosphere: Part 3: Unsaturated convection Composition / Structure Radiative transfer Vertical and latitudinal heat transport Atmospheric circulation.
Lab 6: Saturation & Atmospheric Stability
ATOC 4720: class Enthalpy 1. Enthalpy 2. Latent heat 2. Latent heat 3.Adiabatic processes 3.Adiabatic processes.
AOSS 401, Fall 2007 Lecture 6 September 19, 2007 Richard B. Rood (Room 2525, SRB) Derek Posselt (Room 2517D, SRB)
Water in the Atmosphere
Moisture in the Atmosphere
What causes Clouds? What are their Names? Cumulus Stratus Cumulonimbus Cirrus.
Equation of State (a.k.a. the “Ideal Gas Law”) Direct relationship between density and pressure Inverse relationship between density and temperature Direct.
Humidity Under what conditions do you see the above?
Key Terms and Concepts ELR--Environmental Lapse Rate 5°C-6.5°C/1000 m – temperature of the STILL air as you ascend through the troposphere. ALR--Adiabatic.
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!!!
Vertical Motion in the Atmosphere Jon, Ashley, Paige.
Chapter 6. Importance of Clouds  Release heat to atmosphere  Help regulate energy balance  Indicate physical processes.
Atmospheric Stability Terminology I Hydrostatic Equilibrium –Balance, in the vertical, between PGF and gravity –The general state of the atmosphere –Net.
Thermal Properties of Troposphere September 10, 2007.
Cirrus anvil cumulonimbus T (skewed) LCL (Lifting Condensation Level) LFC (Level of Free Convection) EL (Equilibrium level) p overshooting CAPE Sounding.
Atmospheric Stability The resistance of the atmosphere to vertical motion. Stable air resists vertical motion Unstable air encourages vertical motion.
Skew T Log P Diagram AOS 330 LAB 10 Outline Static (local) Stability Review Critical Levels on Thermodynamic Diagram Severe Weather and Thermodynamic.
Vertical Motion and Temperature Rising air expands, using energy to push outward against its environment, adiabatically cooling the air A parcel of air.
Atmospheric Stability and Air Masses
Full calculation of radiative equilibrium. Problems with radiative equilibrium solution Too hot at and near surface Too cold at and near tropopause Lapse.
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.
Cloud Formation. Bell-work 1.Two ways to saturate air: 1.__________________ 2.__________________ 2. As air rises, it cools rate of _____°C / km 3. As.
Meteo 3: Chapter 8 Stability and Cloud Types Read Chapter 8.
Chapter 6 Stability and Cloud Development. Stability & Cloud Development This chapter discusses: 1.Definitions and causes of stable and unstable atmospheric.
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.
Moisture in the Atmosphere Chapter Layers of the Atmosphere.
Topic 3B: Moist Thermodynamics
Atmospheric Stability
AOSS 321, Winter 2009 Earth System Dynamics Lecture 11 2/12/2009
Bellwork 4/10 Please, turn in your Sling Psychrometer Lab
Stability and Cloud Development
1. Transformations of Moist Air
Presentation transcript:

Simulating Adiabatic Parcel Rise Presentation by Anna Merrifield, Sarah Shackleton and Jeff Sussman

Buoyancy Force Relationship of parcel density to atmospheric density At a given pressure, density is determined by Temperature

Buoyancy Force If the parcel is less dense (warmer) than the atmosphere it will rise adiabatically and cool T’ > T env If parcel is more dense (cooler) than the environment it will sink adiabatically and warm T’ < T env

Real World Examples of Parcel Rise Cloud formation If the environment is stable, clouds that form will be shallow (stratus clouds) In an unstable environment, vertical motion occurs, cumulus and cumulonimbus form Thunderstorms/Tornadoes With enough parcel rise, thunderstorms can form

CAPE Convective available potential energy Amount of potential energy available for parcel rise Important for thunderstorm growth/formation

Parcel Method 1.The parcel does not mix with the surrounding environment 2.The parcel does not disturb its environment 3.The pressure of the parcel adjusts instantaneously to its environment 4.The parcel moves isentropically

The Model 1.Obtain the data from Figure 7.2 using DataThief 2.Determine Z(P,T) 3.Model Parcel Temperature assuming: 1.Dry adiabatic rise to LCL 2.Saturated adiabatic rise to LNB 3.“Moist” adiabatic rise above the LNB 4.Model Parcel Temperature assuming: 1.Dry adiabatic rise to LCL 2.Saturated adiabatic rise while entraining dry air to LNB 3.“Moist” adiabatic rise above the LNB 5.Sensitivity analysis: find lapse rates that reproduce the model

1. Obtaining the Data The plot lines were redrawn in color to allow for effective tracing. Markers indicate the axes and the beginning, color, and end of the line we want to trace. After the line is traced, the program picks points on the line and the data can be output and read into Matlab.

1. Problems with DataThief Solution: Rather than throwing out points (they aren’t “bad”, we determined Z using a linear least-squares fit to 3 regions of constant lapse rate

2. Determining Z(P,T) Regions of ~Constant Lapse Rate Γ = 6.5 K/Km Γ =.64 K/Km Γ = 3.6 K/Km

2. Determining Z(P,T)

Dry & Saturated Adiabatic Lapse Rates Dry lapse rate: assumptions – ideal gas, atmosphere is in hydrostatic equilibrium, no water vapor Saturated lapse rate: assumptions – no loss of water through precipitation, only liquid and vapor phases, system at chemical equilibrium, and heat capacities of liquid and water vapor are negligible, parcel has reached 100% relative humidity

Modeling Saturated Adiabatic Rise 1. Initialize e sat (1), T parcel (1) 3. Calculate Γs(1) which depends on ws(1),T parcel (1) 4. Calculate Tparcel(2) 5. Calculate esat(2) 6. Return to start of loop, calculate ws(2) etc. 2. Calculate ws (1)

3. Model Parcel Temperature (No Entrainment) Γ to LCL 9.8 K/Km Γ at LCL5 K/Km Γ at LNB7.5 K/Km Γ above LNB3 K/Km LCL LNB

The Second Model Entrainment: The mixing of the rising air parcel with the surrounding environment Entrainment rate: 1/m dm/dz Assumptions: entrainment of dry air, constant entrainment rate, isotropic entrainment

4. Model Parcel Temperature (Entrainment) λ (1/m) Γ m at LCL (K/Km) Γ m at LNB (K/Km) 5* * * *

Discussion Lack of CAPE in all models Limitations of the simplified model Parcel movement adiabatic and reversible (no precipitation) Entrainment of dry air Sounding given as lnP versus T, not given with altitude which then needed to be derived using assumption of constant lapse rate atmosphere in three regions DataThief does not give monotonically increasing data points

5. Reproduction of Figure 7.2 Γ to LCL 9.8 K/Km Γ at LCL2 K/Km Γ at LNB6.5 K/Km Γ above LNB3 K/Km LCL LNB

Summary of Lapse Rates Environment No Entrainment λ = 5*10^-10 1/m λ = 5*10^-5 1/m λ = 1*10^-4 1/m λ = 5*10^-4 1/m Best Reproduction Approximate Parcel Γ to LCL Γ at LCL Γ at LNB Γ above LNB

Example sounding

CAPE example with entrainment Image from NWS from Amarillo, TX, July 22,2013

Conclusions and Further Work Failure to reproduce plot using simplified governing assumptions of adiabatic parcel rise Further work using soundings from a database