Presentation is loading. Please wait.

Presentation is loading. Please wait.

Chapter 6 – Cloud Development and Forms. Cloud Formation Condensation (i.e. clouds,fog) results from:

Similar presentations


Presentation on theme: "Chapter 6 – Cloud Development and Forms. Cloud Formation Condensation (i.e. clouds,fog) results from:"— Presentation transcript:

1 Chapter 6 – Cloud Development and Forms

2 Cloud Formation Condensation (i.e. clouds,fog) results from:

3 Cloud Formation Condensation (i.e. clouds,fog) results from: Diabatic cooling (important for fog)

4 Cloud Formation Condensation (i.e. clouds,fog) results from: Diabatic cooling (important for fog) Adiabatic cooling (important for clouds)

5 Cloud Formation Condensation (i.e. clouds,fog) results from: Diabatic cooling (important for fog) Adiabatic cooling (important for clouds) Clouds form due to adiabatic cooling in rising air Γ d = 9.8 o C/km (unsaturated lapse rate) Γ m ~ 5 o C/km (saturated lapse rate)

6 How Does Air Rise? 4 mechanisms cause air to rise: 1) Orographic lift – air that rises because it is going over a mountain

7 How Does Air Rise? 4 mechanisms cause air to rise: 1) Orographic lift – air that rises because it is going over a mountain 2) Frontal lift – air that rises at a front

8 How Does Air Rise? 4 mechanisms cause air to rise: 1) Orographic lift – air that rises because it is going over a mountain 2) Frontal lift – air that rises at a front 3) Horizontal convergence – air that is forced to rise because it is converging

9 How Does Air Rise? 4 mechanisms cause air to rise: 1) Orographic lift – air that rises because it is going over a mountain 2) Frontal lift – air that rises at a front 3) Horizontal convergence – air that is forced to rise because it is converging 4) Convection – air that rises because it is less dense that its surroundings

10 Orographic Lift Air rises as it approaches a mountain peak

11 Orographic Lift Air rises as it approaches a mountain peak

12 Orographic Lift Air descends after it goes over a mountain peak Clear air

13 Rain Shadow A rain shadow is an area of less precipitation and clouds on the downwind side of a mountain (the anti-cloud!)

14 Rain Shadow A rain shadow is an area of less precipitation and clouds on the downwind side of a mountain (the anti-cloud!) Air descends downwind of a mountain peak

15 Rain Shadow A rain shadow is an area of less precipitation and clouds on the downwind side of a mountain (the anti-cloud!) Air descends downwind of a mountain peak Air warms adiabatically due to compression

16 Rain Shadow A rain shadow is an area of less precipitation and clouds on the downwind side of a mountain (the anti-cloud!) Air descends downwind of a mountain peak Air warms adiabatically due to compression Precipitation and clouds evaporate to form rain shadow

17 Rain Shadow

18 Frontal Lifting Front – a zone of rapidly changing temperature (strong temperature gradient)

19 Frontal Lifting Front – a zone of rapidly changing temperature (strong temperature gradient) Types of Fronts 1) Cold Front – cold air is advancing

20 Frontal Lifting Front – a zone of rapidly changing temperature (strong temperature gradient) Types of Fronts 1) Cold Front – cold air is advancing 2)Warm Front – warm air is advancing

21 Frontal Lifting Front – a zone of rapidly changing temperature (strong temperature gradient) Types of Fronts 1) Cold Front – cold air is advancing 2)Warm Front – warm air is advancing 3) Stationary Front – front isn’t moving

22 Frontal Lifting Front – a zone of rapidly changing temperature (strong temperature gradient) Types of Fronts 1) Cold Front – cold air is advancing 2)Warm Front – warm air is advancing 3) Stationary Front – front isn’t moving 4) Occluded Front – you’ll find out later

23 Frontal Lifting Example of a cold front

24 Frontal Lifting Cold Front (cold air pushes warm air up) Warm Front (Warm air overruns cold air)

25 Convergence Air must rise when it converges

26 Convergence Air must rise when it converges

27 Convection Air “bubbles” or “parcels” rise when they are warmed and become less dense than their surroundings (exactly the same way a helium balloon does) 2km T = 11 o C T = -8.6 o C T = 1.2 o C 1km

28 Convection Air “bubbles” or “parcels” rise when they are warmed and become less dense than their surroundings (exactly the same way a helium balloon does) This is how thunderstorms form! 2km T = 11 o C T = -8.6 o C T = 1.2 o C 1km

29 Atmospheric Stability Atmospheric stability – a measure of the atmosphere’s susceptibility to vertical motion

30 Atmospheric Stability Atmospheric stability – a measure of the atmosphere’s susceptibility to vertical motion Atmospheric stability depends on the environmental lapse rate (Γ e )

31 Atmospheric Stability Atmospheric stability – a measure of the atmosphere’s susceptibility to vertical motion Atmospheric stability depends on the environmental lapse rate (Γ e ) Atmospheric stability comes in 3 flavors: 1) Absolutely stable

32 Atmospheric Stability Atmospheric stability – a measure of the atmosphere’s susceptibility to vertical motion Atmospheric stability depends on the environmental lapse rate (Γ e ) Atmospheric stability comes in 3 flavors: 1) Absolutely stable 2) Absolutely unstable

33 Atmospheric Stability Atmospheric stability – a measure of the atmosphere’s susceptibility to vertical motion Atmospheric stability depends on the environmental lapse rate (Γ e ) Atmospheric stability comes in 3 flavors: 1) Absolutely stable 2) Absolutely unstable 3) Conditionally unstable

34 Absolutely Unstable Air The slightest nudge sends the ball accelerating away…

35 Absolutely Unstable Air Absolutely unstable: Γ e > Γ d (unsaturated air) Γ e = 1.5 o C/100m Γ d = 1.0 o C/100m

36 Absolutely Unstable Air Absolutely unstable: Γ e > Γ m (saturated air) Γ e = 1.5 o C/100m Γ m = 0.5 o C/100m

37 Absolutely Stable Air Any push and the ball will go back to the valley and come to rest again…

38 Absolutely Stable Air Γ m = 0.5 o C/100m Γ e = 0.2 o C/100m Γ d = 1.0 o C/100m Γ e = 0.2 o C/100m

39 Conditionally Unstable Air If the ball is pushed high enough, it will go over the hump and accelerate away… (otherwise it comes back to rest)

40 Conditionally Unstable Air Γ m = 0.5 o C/100m Γ e = 0.7 o C/100m Γ d = 1.0 o C/100m Γ e = 0.7 o C/100m

41 Stability Summary Absolutely unstable: Γ e > both Γ d and Γ m

42 Stability Summary Absolutely unstable: Γ e > both Γ d and Γ m Absoutely stable: Γ e < both Γ d and Γ m

43 Stability Summary Absolutely unstable: Γ e > both Γ d and Γ m Absoutely stable: Γ e < both Γ d and Γ m Conditionally unstable Γ d > Γ e > Γ m

44 Absolutely Unstable Γ d – green solid line Γ m – blue dashed line Γ e – black solid line

45 Absolutely Stable Γ d – green solid line Γ m – blue dashed line Γ e – black solid line

46 Conditionally Unstable Γ d – green solid line Γ m – blue dashed line Γ e – black solid line

47 What Makes the Environmental Lapse Rate (Γ e )? Γ e is extremely variable in space and time (like AMA vs. MAF soundings!)

48 What Makes the Environmental Lapse Rate (Γ e )? Γ e is extremely variable in space and time (like AMA vs. MAF soundings!) Γ e is influenced by 3 factors: 1) Near surface heating/cooling

49 What Makes the Environmental Lapse Rate (Γ e )? Γ e is extremely variable in space and time (like AMA vs. MAF soundings!) Γ e is influenced by 3 factors: 1) Near surface heating/cooling 2) Differential temperature advection

50 What Makes the Environmental Lapse Rate (Γ e )? Γ e is extremely variable in space and time (like AMA vs. MAF soundings!) Γ e is influenced by 3 factors: 1) Near surface heating/cooling 2) Differential temperature advection 3) Air mass replacement

51 Surface Heating and Cooling Γ e in the lower atmosphere changes with daytime heating and nighttime cooling

52 Differential Temperature Advection Γ e can change if temperature advection changes with height

53 Air Mass Replacement Γ e can change if an entirely new air mass moves into an area

54 Limitations on Convection What stops vertical motion? - The only “stopper” is if air becomes more dense (colder) than its surroundings!!

55 Limitations on Convection What stops vertical motion? - The only “stopper” is if air becomes more dense (colder) than its surroundings!! This happens in 2 ways: 1) Stable air aloft

56 Limitations on Convection What stops vertical motion? - The only “stopper” is if air becomes more dense (colder) than its surroundings!! This happens in 2 ways: 1) Stable air aloft 2) Entrainment – intake of drier air from surroundings

57 Convection Lifting condensation level (LCL) – The level at which a cloud forms (altitude of cloud base) Level of Free Convection (LFC) – the level at which air becomes less dense (warmer) than its surroundings

58 Stable Air Aloft (Dry Example) Γ d – green solid line Γ e – black solid line Air is accelerating up Air stops accelerating

59 Inversions – Extremely Stable Air Inversion – when temperature increases with height

60 Inversions Γ d – green solid line Γ m – blue dashed line Γ e – black solid line

61 Types of Inversions 1) Radiation inversion – caused by nighttime cooling of surface air

62 Types of Inversions 2) Frontal inversion – occurs at fronts

63 Types of Inversions 3) Subsidence inversion – caused by sinking air above a static layer

64 Inversions and Agriculture

65 Entrainment Mixing with surrounding drier, cooler air cools rising parcels through: 1) Mixing 2) Evaporation

66 Cloud Types Old classification of clouds 1)Cirrus (high, thin, wispy)

67 Cloud Types Old classification of clouds 1)Cirrus (high, thin, wispy) 2)Stratus (layered)

68 Cloud Types Old classification of clouds 1)Cirrus (high, thin, wispy) 2)Stratus (layered) 3)Cumulus (puffy, vertically-developed)

69 Cloud Types Old classification of clouds 1)Cirrus (high, thin, wispy) 2)Stratus (layered) 3)Cumulus (puffy, vertically-developed) 4)Nimbus (rain-producing)

70 Cloud Types New classification of clouds 1)High clouds (higher than 19,000 ft.) 2)Middle clouds (b/w 6,000 and 19,000 ft.) 3)Low clouds (below 6,000 ft.) 4)Clouds with vertical development

71 Cloud Types

72 High Clouds (> 19,000 ft.) Composed of ice crystals

73 High Clouds (> 19,000 ft.) Composed of ice crystals Principal types: 1) Cirrus

74 High Clouds (> 19,000 ft.) Composed of ice crystals Principal types: 1) Cirrus 2) Cirrostratus

75 High Clouds (> 19,000 ft.) Composed of ice crystals Principal types: 1) Cirrus 2) Cirrostratus 3) Cirrocumulus

76 Cirrus

77 Cirrostratus

78 Cirrocumulus

79 Other High Clouds - Contrails

80 Middle Clouds (between 6,000 and 19,000 ft.) Composed mostly of supercooled water

81 Middle Clouds (between 6,000 and 19,000 ft.) Composed mostly of supercooled water Principal types: 1) Altostratus

82 Middle Clouds (between 6,000 and 19,000 ft.) Composed mostly of supercooled water Principal types: 1) Altostratus 2) Altocumulus

83 Altostratus

84 Altocumulus

85 Low Clouds (< 6,000 ft.) Composed of liquid water

86 Low Clouds (< 6,000 ft.) Composed of liquid water Principal types: 1) Stratus

87 Low Clouds (< 6,000 ft.) Composed of liquid water Principal types: 1) Stratus 2) Nimbostratus

88 Low Clouds (< 6,000 ft.) Composed of liquid water Principal types: 1) Stratus 2) Nimbostratus 3) Stratocumulus

89 Stratus

90 Nimbostratus

91 Stratocumulus

92 Cumulus Clouds Cumulus clouds can extend the entire depth of the atmosphere Principal types: 1) Cumulus - cumulus humilis (fair-weather cumulus) - cumulus congestus (fortress-like) 2) Cumulonimbus

93 Cumulus Humilis

94 Cumulus Congestus

95 Cumulonimbus

96 Other Types of Clouds Lenticular clouds – clouds that form in wavy airstreams after air goes over a moutain

97 Other Types of Clouds Banner clouds – clouds located at mountain peaks as they ascend a mountain

98 Other Types of Clouds Banner clouds – clouds located at mountain peaks as they ascend a mountain Mammatus clouds – balloon-like clouds hanging down from cumulonimbus clouds

99 Other Types of Clouds Nacreous clouds – stratospheric clouds (rare!)

100 Other Types of Clouds Nacreous clouds – stratospheric clouds (rare!) Noctilucent clouds – mesospheric clouds (rare!)

101 Lenticular clouds

102 Mammatus Clouds

103 Banner Clouds

104 Nacreous Clouds

105 Noctilucent Clouds

106 Observing Clouds Ceilometers – automated instrument that measures the height of the cloud base, or ceiling, as well as coverage

107 Cloud Coverage

108 Observing Clouds Both cloud ceilings and coverage is reported in the standard ASOS hourly observation

109 Observing Clouds Satellite imagery is also a primary tool for observing clouds and cloud motions Visible satellite imagery Infrared satellite imagery Water vapor satellite imagery

110 Visible Satellite Imagery

111 Infrared Satellite Imagery

112 Water Vapor Satellite Imagery


Download ppt "Chapter 6 – Cloud Development and Forms. Cloud Formation Condensation (i.e. clouds,fog) results from:"

Similar presentations


Ads by Google