Presentation is loading. Please wait.

Presentation is loading. Please wait.

CE 394K.2 Hydrology Atmospheric Water and Precipitation

Similar presentations


Presentation on theme: "CE 394K.2 Hydrology Atmospheric Water and Precipitation"— Presentation transcript:

1 CE 394K.2 Hydrology Atmospheric Water and Precipitation
Literary quote for today: “In Köhln, a town of monks and bones, And pavements fang'd with murderous stones And rags, and hags, and hideous wenches; I counted two and seventy stenches, All well defined, and several stinks! Ye nymphs that reign o'er sewers and sinks, The river Rhine, it is well known, Doth wash your city of Cologne; But tell me, nymphs, what power devine Shall henceforth wash the river Rhine?” Samuel Taylor Coleridge, “The City of Cologne”, 1800 Contributed by Eric Hersh

2 Questions for today (1)  How is net radiation to the earth’s surface partitioned into latent heat, sensible heat and ground heat flux and how does this partitioning vary with location on the earth? (2) What are the factors that govern the patterns of atmospheric circulation over the earth? (3)  What are the key variables that describe atmospheric water vapor and how are they connected? (4)  What causes precipitation to form and what are the factors that govern the rate of precipitation? (5)  How is precipitation measured and described? (Some slides in this presentation were prepared by Venkatesh Merwade)

3 Questions for today (1)  How is net radiation to the earth’s surface partitioned into latent heat, sensible heat and ground heat flux and how does this partitioning vary with location on the earth? (2) What are the factors that govern the patterns of atmospheric circulation over the earth? (3)  What are the key variables that describe atmospheric water vapor and how are they connected? (4)  What causes precipitation to form and what are the factors that govern the rate of precipitation? (5)  How is precipitation measured and described? (Some slides in this presentation were prepared by Venkatesh Merwade)

4 Heat energy Energy Internal energy Potential, Kinetic, Internal (Eu)
Sensible heat – heat content that can be measured and is proportional to temperature Latent heat – “hidden” heat content that is related to phase changes

5 Energy Units In SI units, the basic unit of energy is Joule (J), where 1 J = 1 kg x 1 m/s2 Energy can also be measured in calories where 1 calorie = heat required to raise 1 gm of water by 1°C and 1 kilocalorie (C) = 1000 calories (1 calorie = 4.19 Joules) We will use the SI system of units

6 Energy fluxes and flows
Water Volume [L3] (acre-ft, m3) Water flow [L3/T] (cfs or m3/s) Water flux [L/T] (in/day, mm/day) Energy amount [E] (Joules) Energy “flow” in Watts [E/T] (1W = 1 J/s) Energy flux [E/L2T] in Watts/m2 Energy flow of 1 Joule/sec Area = 1 m2

7 MegaJoules When working with evaporation, its more convenient to use MegaJoules, MJ (J x 106) So units are Energy amount (MJ) Energy flow (MJ/day, MJ/month) Energy flux (MJ/m2-day, MJ/m2-month)

8 Internal Energy of Water
Water vapor Water Ice Heat Capacity (J/kg-K) Latent Heat (MJ/kg) Ice Water 2.5/0.33 = 7.6 Water may evaporate at any temperature in range 0 – 100°C Latent heat of vaporization consumes 7.6 times the latent heat of fusion (melting)

9 Latent heat flux Water flux Energy flux Evaporation rate, E (mm/day)
Latent heat flux (W/m2), Hl r = 1000 kg/m3 lv = 2.5 MJ/kg 28.94 W/m2 = 1 mm/day Area = 1 m2

10 Radiation Two basic laws Stefan-Boltzman Law All bodies emit radiation
R = emitted radiation (W/m2) e = emissivity (0-1) s = 5.67x10-8W/m2-K4 T = absolute temperature (K) Wiens Law l = wavelength of emitted radiation (m) All bodies emit radiation Hot bodies (sun) emit short wave radiation Cool bodies (earth) emit long wave radiation

11 Average value of Rn over the earth and
Net Radiation, Rn Ri Incoming Radiation Ro =aRi Reflected radiation = albedo (0 – 1) Re Rn Net Radiation Average value of Rn over the earth and over the year is 105 W/m2

12 Average value of Rn over the earth and
Net Radiation, Rn H – Sensible Heat LE – Evaporation G – Ground Heat Flux Rn Net Radiation Average value of Rn over the earth and over the year is 105 W/m2

13 Energy Balance of Earth
70 20 100 6 6 26 4 38 15 19 21 Sensible heat flux 7 Latent heat flux 23 51

14 Energy balance at earth’s surface Downward short-wave radiation, Jan 2003
600Z

15 Energy balance at earth’s surface Downward short-wave radiation, Jan 2003
900Z

16 Energy balance at earth’s surface Downward short-wave radiation, Jan 2003
1200Z

17 Energy balance at earth’s surface Downward short-wave radiation, Jan 2003
1500Z

18 Energy balance at earth’s surface Downward short-wave radiation, Jan 2003
1800Z

19 Energy balance at earth’s surface Downward short-wave radiation, Jan 2003
2100Z

20 Latent heat flux, Jan 2003, 1500z

21 Questions for today (1)  How is net radiation to the earth’s surface partitioned into latent heat, sensible heat and ground heat flux and how does this partitioning vary with location on the earth? (2) What are the factors that govern the patterns of atmospheric circulation over the earth? (3)  What are the key variables that describe atmospheric water vapor and how are they connected? (4)  What causes precipitation to form and what are the factors that govern the rate of precipitation? (5)  How is precipitation measured and described? (Some slides in this presentation were prepared by Venkatesh Merwade)

22 Heating of earth surface
Heating of earth surface is uneven Solar radiation strikes perpendicularly near the equator (270 W/m2) Solar radiation strikes at an oblique angle near the poles (90 W/m2) Emitted radiation is more uniform than incoming radiation Amount of energy transferred from equator to the poles is approximately 4 x 109 MW

23 Warm air rises, cool air descends creating two huge convective cells.
Hadley circulation Warm air rises, cool air descends creating two huge convective cells.

24 Coriolis Force Cone is moving southward towards the pole
Camera fixed in the outer space (cone appears moving straight) Camera fixed on to the globe (looking southward, cone appears deflecting to the right) the force that deflects the path of the wind on account of earth rotation is called Coriolis force. The path of the wind is deflected to the right in the Northern Hemisphere and the to left in the Southern Hemisphere.

25 Atmospheric circulation
Circulation cells Polar Cell Hadley cell Ferrel Cell Polar cell Ferrel Cell Winds Tropical Easterlies/Trades Westerlies Polar easterlies Latitudes Intertropical convergence zone (ITCZ)/Doldrums Horse latitudes Subpolar low Polar high

26 Effect of land mass distribution
Uneven distribution of land and ocean, coupled with different thermal properties creates spatial variation in atmospheric circulation A) Idealized winds generated by pressure gradient and Coriolis Force. B) Actual wind patterns owing to land mass distribution

27 Shifting in Intertropical Convergence Zone (ITCZ)
Owing to the tilt of the Earth's axis in orbit, the ITCZ shifts north and south.  Southward shift in January Creates wet Summers (Monsoons) and dry winters, especially in India and SE Asia Northward shift in July

28 ITCZ movement

29 Questions for today (1)  How is net radiation to the earth’s surface partitioned into latent heat, sensible heat and ground heat flux and how does this partitioning vary with location on the earth? (2) What are the factors that govern the patterns of atmospheric circulation over the earth? (3)  What are the key variables that describe atmospheric water vapor and how are they connected? (4)  What causes precipitation to form and what are the factors that govern the rate of precipitation? (5)  How is precipitation measured and described? (Some slides in this presentation were prepared by Venkatesh Merwade)

30 Structure of atmosphere

31 Atmospheric water Atmospheric water exists
Mostly as gas or water vapor Liquid in rainfall and water droplets in clouds Solid in snowfall and in hail storms Accounts for less than 1/100,000 part of total water, but plays a major role in the hydrologic cycle

32 Water vapor Suppose we have an elementary volume of atmosphere dV and
we want quantify how much water vapor it contains Water vapor density dV ma = mass of moist air mv = mass of water vapor Air density Atmospheric gases: Nitrogen – 78.1% Oxygen – 20.9% Other gases ~ 1%

33 Specific Humidity, qv Specific humidity measures the mass of water vapor per unit mass of moist air It is dimensionless

34 Vapor pressure, e Vapor pressure, e, is the pressure that water vapor exerts on a surface Air pressure, p, is the total pressure that air makes on a surface Ideal gas law relates pressure to absolute temperature T, Rv is the gas constant for water vapor 0.622 is ratio of mol. wt. of water vapor to avg mol. wt. of dry air

35 Dalton’s Law of Partial Pressures
John Dalton studied the effect of gases in a mixture. He observed that the Total Pressure of a gas mixture was the sum of the Partial Pressure of each gas. P total = P1 + P2 + P Pn The Partial Pressure is defined as the pressure of a single gas in the mixture as if that gas alone occupied the container. In other words, Dalton maintained that since there was an enormous amount of space between the gas molecules within the mixture that the gas molecules did not have any influence on the motion of other gas molecules, therefore the pressure of a gas sample would be the same whether it was the only gas in the container or if it were among other gases.

36 Dry air ( z = x+y molecules)
Avogadro’s law Equal volumes of gases at the same temperature and pressure contain the same number of molecules regardless of their chemical nature and physical properties. This number (Avogadro's number) is X 1023 in L for all gases. Dry air ( z = x+y molecules) Moist air (x dry and y water vapor) Dry air Water vapor rd = (x+y) * Md/Volume rm = (x* Md + y*Mv)/Volume rm < rd, which means moist air is lighter than dry air!

37 Saturation vapor pressure, es
Saturation vapor pressure occurs when air is holding all the water vapor that it can at a given air temperature Vapor pressure is measured in Pascals (Pa), where 1 Pa = 1 N/m2 1 kPa = 1000 Pa

38 Relative humidity, Rh es e Relative humidity measures the percent
of the saturation water content of the air that it currently holds (0 – 100%)

39 Dewpoint Temperature, Td
Dewpoint temperature is the air temperature at which the air would be saturated with its current vapor content

40 Water vapor in an air column
We have three equations describing column: Hydrostatic air pressure, dp/dz = -rag Lapse rate of temperature, dT/dz = - a Ideal gas law, p = raRaT Combine them and integrate over column to get pressure variation elevation 2 Column Element, dz 1

41 Precipitable Water In an element dz, the mass of water vapor is dmp
Integrate over the whole atmospheric column to get precipitable water,mp mp/A gives precipitable water per unit area in kg/m2 2 Column Element, dz Area = A 1

42 Precipitable Water, Jan 2003

43 Precipitable Water, July 2003

44 January July

45 Questions for today (1)  How is net radiation to the earth’s surface partitioned into latent heat, sensible heat and ground heat flux and how does this partitioning vary with location on the earth? (2) What are the factors that govern the patterns of atmospheric circulation over the earth? (3)  What are the key variables that describe atmospheric water vapor and how are they connected? (4)  What causes precipitation to form and what are the factors that govern the rate of precipitation? (5)  How is precipitation measured and described? (Some slides in this presentation were prepared by Venkatesh Merwade)

46 Precipitation Precipitation: water falling from the atmosphere to the earth. Rainfall Snowfall Hail, sleet Requires lifting of air mass so that it cools and condenses.

47 Mechanisms for air lifting
Frontal lifting Orographic lifting Convective lifting

48 Definitions Air mass : A large body of air with similar temperature and moisture characteristics over its horizontal extent. Front: Boundary between contrasting air masses. Cold front: Leading edge of the cold air when it is advancing towards warm air. Warm front: leading edge of the warm air when advancing towards cold air.

49 Frontal Lifting Boundary between air masses with different properties is called a front Cold front occurs when cold air advances towards warm air Warm front occurs when warm air overrides cold air Cold front (produces cumulus cloud) Cold front (produces stratus cloud)

50 Orographic lifting Orographic uplift occurs when air is forced to rise because of the physical presence of elevated land.

51 Convective lifting Convective precipitation occurs when the air near the ground is heated by the earth’s warm surface. This warm air rises, cools and creates precipitation. Hot earth surface

52 Condensation Condensation is the change of water vapor into a liquid. For condensation to occur, the air must be at or near saturation in the presence of condensation nuclei. Condensation nuclei are small particles or aerosol upon which water vapor attaches to initiate condensation. Dust particulates, sea salt, sulfur and nitrogen oxide aerosols serve as common condensation nuclei. Size of aerosols range from 10-3 to 10 mm.

53 Precipitation formation
Lifting cools air masses so moisture condenses Condensation nuclei Aerosols water molecules attach Rising & growing 0.5 cm/s sufficient to carry 10 mm droplet Critical size (~0.1 mm) Gravity overcomes and drop falls

54 Forces acting on rain drop
Three forces acting on rain drop Gravity force due to weight Buoyancy force due to displacement of air Drag force due to friction with surrounding air D Fb Fd Fd Fg

55 Terminal Velocity Terminal velocity: velocity at which the forces acting on the raindrop are in equilibrium. If released from rest, the raindrop will accelerate until it reaches its terminal velocity D Fb Fd Fd Fg At standard atmospheric pressure (101.3 kpa) and temperature (20oC), rw = 998 kg/m3 and ra = 1.20 kg/m3 V Raindrops are spherical up to a diameter of 1 mm For tiny drops up to 0.1 mm diameter, the drag force is specified by Stokes law

56 Precipitation Variation
Influenced by Atmospheric circulation and local factors Higher near coastlines Seasonal variation – annual oscillations in some places Variables in mountainous areas Increases in plains areas More uniform in Eastern US than in West

57 Rainfall patterns in the US

58 Global precipitation pattern

59 Spatial Representation
Isohyet – contour of constant rainfall Isohyetal maps are prepared by interpolating rainfall data at gaged points. Austin, May 1981 Wellsboro, PA 1889

60 Texas Rainfall Maps

61 Temporal Representation
Rainfall hyetograph – plot of rainfall depth or intensity as a function of time Cumulative rainfall hyetograph or rainfall mass curve – plot of summation of rainfall increments as a function of time Rainfall intensity – depth of rainfall per unit time

62 Rainfall Depth and Intensity

63 Incremental Rainfall Rainfall Hyetograph

64 Cumulative Rainfall Rainfall Mass Curve

65 Arithmetic Mean Method
Simplest method for determining areal average P1 = 10 mm P2 = 20 mm P3 = 30 mm P1 P2 P3 Gages must be uniformly distributed Gage measurements should not vary greatly about the mean

66 Thiessen polygon method
Any point in the watershed receives the same amount of rainfall as that at the nearest gage Rainfall recorded at a gage can be applied to any point at a distance halfway to the next station in any direction Steps in Thiessen polygon method Draw lines joining adjacent gages Draw perpendicular bisectors to the lines created in step 1 Extend the lines created in step 2 in both directions to form representative areas for gages Compute representative area for each gage Compute the areal average using the following formula A1 A2 A3 P1 P2 P3 P1 = 10 mm, A1 = 12 Km2 P2 = 20 mm, A2 = 15 Km2 P3 = 30 mm, A3 = 20 km2

67 Isohyetal method Steps Construct isohyets (rainfall contours)
Compute area between each pair of adjacent isohyets (Ai) Compute average precipitation for each pair of adjacent isohyets (pi) Compute areal average using the following formula 10 20 P1 A1=5 , p1 = 5 A2=18 , p2 = 15 P2 A3=12 , p3 = 25 P3 30 A4=12 , p3 = 35

68 Inverse distance weighting
Prediction at a point is more influenced by nearby measurements than that by distant measurements The prediction at an ungaged point is inversely proportional to the distance to the measurement points Steps Compute distance (di) from ungaged point to all measurement points. Compute the precipitation at the ungaged point using the following formula P1=10 P2= 20 d1=25 d2=15 P3=30 d3=10 p

69 Rainfall interpolation in GIS
Data are generally available as points with precipitation stored in attribute table.

70 Nearest Neighbor “Thiessen” Polygon Interpolation
Rainfall maps in GIS Nearest Neighbor “Thiessen” Polygon Interpolation Spline Interpolation

71 NEXRAD NEXt generation RADar: is a doppler radar used for obtaining weather information A signal is emitted from the radar which returns after striking a rainfall drop Returned signals from the radar are analyzed to compute the rainfall intensity and integrated over time to get the precipitation NEXRAD Tower Working of NEXRAD

72 NEXRAD data NCDC data (JAVA viewer) West Gulf River Forecast Center
West Gulf River Forecast Center National Weather Service Animation


Download ppt "CE 394K.2 Hydrology Atmospheric Water and Precipitation"

Similar presentations


Ads by Google