MADISON’S CURRENT WEATHER Madison Weather at 1000 AM CDT 8 JUL 2002 Updated twice an hour at :05 and :25 Sky/Weather: MOSUNNY Temperature: 83 F (28 C) Dew Point: 71 F (21 C) Relative Humidity: 67% Wind: SW9 MPH Barometer: 30.09F (1018.9 mb) CURRENT VISIBLE ATM OCN 100 Summer 2002 13 Current Surface Weather Map with Isobars (“iso” = equal & “bar” = weight), Fronts and Radar ATM OCN 100 Summer 2002 14 Current Temperatures (°F) & Isotherms (“iso” = equal +”therm” = temperature) ATM OCN 100 Summer 2002 17 CURRENT IR ATM OCN 100 Summer 2002 19 Current Dewpoints (oF) ATM OCN 100 Summer 2002 20 Tomorrow AM Forecast Map ATM OCN 100 Summer 2002 21 Last 24 hrs in Madison Local Noon ATM OCN 100 Summer 2002 Sunset Sunrise 22 ATM OCN 100 – Summer 2002 LECTURE 9 THERMODYNAMICS: BEHAVIOR OF GASES IN THE ATMOSPHERE A. INTRODUCTION – – How are pressure & temperature related? Why are lows cloudy and highs fair? ATM OCN 100 Summer 2002 24 B. KINETIC THEORY OF MATTER • • Definitions Historical ATM OCN 100 Summer 2002 25 B. KINETIC THEORY OF MATTER • • • Definitions Historical Assumptions for gases: – Tiny molecules with large space; – No attraction between molecules; – Random molecular motion; – Elastic molecular collisions. ATM OCN 100 Summer 2002 26 B. KINETIC THEORY OF MATTER (con’t.) Variables – – – describing molecular state of a gas Density = molecular mass per volume Temperature ~ average molecular speed Pressure ~ molecular momentum change (~ molecular speed & mass) ATM OCN 100 Summer 2002 28 C. THE GAS LAWS Classical approach to Ideal Gas Law (or Equation of State) Pressure = Density Constant Temperature P = R T (equivalent to PV = nRT) ATM OCN 100 Summer 2002 29 Pressure = Density Constant Temperature P = R T (equivalent to PV = nRT) Atmospheric application of Ideal Gas Law If P = constant, then increases as T decreases; – If = constant, then P increases when T increases; – If T = constant, then increases as P increases. – ATM OCN 100 Summer 2002 30 C. THE GAS LAWS (con’t.) Dalton's Laws of Partial Pressures – Involves mixture of ideal gases; –Each gas species has own partial pressure, p(i). –Then: Total Pressure = Sum of partial pressures ATM OCN 100 Summer 2002 31 C. THE GAS LAWS (con’t.) Atmospheric Applications of Dalton's Laws of Partial Pressures – PTotal = p(N2) + p(O2) + p(Ar) + e + ... – Where p(N2), p(O2), p(Ar) are partial pressures of major atmospheric gases & e = (partial water) vapor pressure. – So for air with some moisture: PTotal = 1020 mb (780 + 210 + 9) mb + e (20 to 40 mb) ATM OCN 100 Summer 2002 32 D. THE THERMODYNAMIC LAWS • • Introduction First Law of Thermodynamics Input = Output + Storage ATM OCN 100 Summer 2002 33 D. THE THERMODYNAMIC LAWS (con’t.) • Atmospheric application of First Law of Thermodynamics Heat exchange = Work + Internal energy Change – Heat exchange by radiation, etc.; – Work by volume change; – Internal energy change by temperature change. ATM OCN 100 Summer 2002 34 D. THE THERMODYNAMIC LAWS (con’t.) • Adiabatic Processes – No heat exchanged with environment; Work = internal energy change – Involves volume change only: Volume change = Temperature change Volume decrease (or Pressure increase) causes heating; Volume increase (or Pressure decrease) causes cooling. ATM OCN 100 Summer 2002 35 E. THE VERTICAL MOTION PROBLEM • Response of an air parcel • Rising motion: Encounters lower pressure Expansion & cooling • • Sinking motion: Encounters higher pressure Compression & warming Specification of the response ATM OCN 100 Summer 2002 36 Recall AIR PRESSURE CLIMATOLOGY See Fig. 5.4 Moran & Morgan (1997) ALTITUDE [km] VERTICAL PRESSURE PROFILE US STANDARD ATMOSPHERE, 1976 5 4 3 1 mb drop for 10 meter height rise 2 1 0 500 600 700 800 900 1000 AIR PRESSURE [millibars] ATM OCN 100 Summer 2002 37 Response of Ascent/Descent of Air Parcel: Dry Adiabatic Lapse Rate (10C°/1000m) See Fig. 6.8 Moran & Morgan (1997) P 600 mb, V= 1.44 m3 P 700 mb, V= 1.28 m3 P 800 mb, V= 1.16 m3 P 900 mb, V= 1.07 m3 ATM OCN 100 Summer 2002 T = 20C, P 1000 mb, V= 1.00 m3 38 E. VERTICAL MOTION (con’t.) • • Specification of parcel response • describes cooling/heating by adiabatic expansion/compression process; • assume dry air parcel. The dry adiabatic lapse rate (DALR) • Recall that lapse rate is how temperature decreases with height; • DALR 10 Co per 1000 meters or 5.5 Fo per 1000 feet. ATM OCN 100 Summer 2002 40 E. VERTICAL MOTION (con’t.) • Response of an air parcel • An example ATM OCN 100 Summer 2002 41 U.S. STANDARD ATMOSPHERE See Fig. 1.9 Moran & Morgan (1997) Altitude [km] 140. 120. 100. 80. Thermosphere Mesopause 60. Stratopause Stratosphere Tropopause Troposphere 40. 20. 0. -100. Mesosphere -50. 0. 50. 100. Temperature [deg C] ATM OCN 100 Summer 2002 42 GREEN BAY RADIOSONDE SOUNDING Sunday PM ATM OCN 100 Summer 2002 43 Why does the Hot Air Balloon Rise? ATM OCN 100 Summer 2002 44 When Convection? ATM OCN 100 Summer 2002 45 F. STATIC STABILITY • • • Importance Stability-Instability Concept • Stable: Return to initial state • Unstable: Continuation away from initial state Criteria for Static Stability (Instability) Determination ATM OCN 100 Summer 2002 46 STABLE CONDITIONS Compare Environment with DALR Colder parcel sinks & returns to start ALTITUDE (m) 2500 Parcel is colder & more dense 2000 Environment is warmer & less dense 1500 1000 500 0 0 5 10 15 20 25 30 TEMPERATURE (C) ATM OCN 100 Summer 2002 47 UNSTABLE CONDITIONS Compare Environment with DALR Warmer parcel continues upward Parcel is warmer & less dense ALTITUDE (m) 2500 2000 1500 1000 500 0 Environment is colder & more dense 0 5 ATM OCN 100 Summer 2002 10 15 20 TEMPERATURE (C) 25 30 48 F. STATIC STABILITY (con’t.) • Processes which change static stability (instability) • Cool below, but warm above (stabilize) • Warm below, but cool above (destabilize) • Visual stability indicators ATM OCN 100 Summer 2002 51 Example of Stabilization– An Inversion ATM OCN 100 Summer 2002 52 Example of Destabilization-Cumulonimbus ATM OCN 100 Summer 2002 53 F. STATIC STABILITY (con’t.) • • • Processes which change static stability (instability) Visual stability indicators Graphical Analysis: The Thermodynamic Diagram ATM OCN 100 Summer 2002 54 GREEN BAY RADIOSONDE SOUNDING Sunday PM ATM OCN 100 Summer 2002 57 MADISON’S CURRENT WEATHER Madison Weather at 1000 AM CDT THU JUL 5 2001 Updated twice an hour at :05 and :25 Sky/Weather: SUNNY Temperature: 63 F (17 C) Dew Point: 42 F (5 C) Relative Humidity: 46% Wind: N7 MPH Barometer: 30.10S Surface Weather Map from Today with Isobars & Fronts ATM OCN 100 Summer 2002 60 Current Temperatures (oF) & Isotherms ATM OCN 100 Summer 2002 61 Current Dewpoints (oF) ATM OCN 100 Summer 2002 62 ATM OCN 100 Summer 2002 63 ATM OCN 100 Summer 2002 64 Tomorrow’s 7AM Forecast ATM OCN 100 Summer 2002 65 Current UVI Forecast ATM OCN 100 Summer 2002 66 Last 24 hrs in Madison ATM OCN 100 Summer 2002 67 ATM OCN 100 Summer 2002 68 At Southern Lake Michigan Buoy ATM OCN 100 Summer 2002 69 U.S. STANDARD ATMOSPHERE See Fig. 1.9 Moran & Morgan (1997) Altitude [km] 140. 120. 100. 80. Thermosphere Mesopause 60. Stratopause Stratosphere Tropopause Troposphere 40. 20. 0. -100. Mesosphere -50. 0. 50. 100. Temperature [deg C] ATM OCN 100 Summer 2002 71 GREEN BAY RADIOSONDE SOUNDING Sunday PM ATM OCN 100 Summer 2002 72 GREEN BAY RADIOSONDE SOUNDING Sunday PM ATM OCN 100 Summer 2002 78 GREEN BAY RADIOSONDE SOUNDING Wednesday PM ATM OCN 100 Summer 2002 79 GREEN BAY RADIOSONDE SOUNDING FRIDAY AM ATM OCN 100 Summer 2002 81 Current Temperatures (oF) – 24 Hrs Ago ATM OCN 100 Summer 2002 90