CE 394K.2 Mass, Momentum, Energy Begin with the Reynolds Transport Theorem Mass – continuity equation Momentum – Manning and Darcy eqns Energy – conduction,

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Presentation transcript:

CE 394K.2 Mass, Momentum, Energy Begin with the Reynolds Transport Theorem Mass – continuity equation Momentum – Manning and Darcy eqns Energy – conduction, convection, radiation Reading: Applied Hydrology Sections 3.1 and 3.2

Reynolds Transport Theorem Total rate of change of B in the fluid system Rate of change of B stored in the control volume Net outflow of B across the control surface

Continuity Equation B = m; b = dB/dm = dm/dm = 1; dB/dt = 0 (conservation of mass)  = constant for water or hence

Continuity equation for a watershed I(t) (Precip) Q(t) (Streamflow) dS/dt = I(t) – Q(t) Closed system if Hydrologic systems are nearly always open systems, which means that it is difficult to do material balances on them What time period do we choose to do material balances for?

Continuous and Discrete time data Continuous time representation Sampled or Instantaneous data (streamflow) truthful for rate, volume is interpolated Pulse or Interval data (precipitation) truthful for depth, rate is interpolated Figure 2.3.1, p. 28 Applied Hydrology Can we close a discrete-time water balance?

Momentum B = mv; b = dB/dm = dmv/dm = v; dB/dt = d(mv)/dt =  F (Newtons 2 nd Law) so For steady flow For uniform flow In a steady, uniform flow

Surface and Groundwater Flow Levels are related to Mean Sea Level Earth surface Ellipsoid Sea surface Geoid Mean Sea Level is a surface of constant gravitational potential called the Geoid

Vertical Earth Datums A vertical datum defines elevation, z NGVD29 (National Geodetic Vertical Datum of 1929) NAVD88 (North American Vertical Datum of 1988) takes into account a map of gravity anomalies between the ellipsoid and the geoid

Energy equation of fluid mechanics Datum z1z1 y1y1 bed water surface energy grade line hfhf z2z2 y2y2 L How do we relate friction slope,to the velocity of flow?

Open channel flow Manning’s equation Channel Roughness Channel Geometry Hydrologic Processes (Open channel flow) Physical environment (Channel n, R) Hydrologic conditions (V, S f )

Subsurface flow Darcy’s equation Hydraulic conductivity Hydrologic Processes (Porous medium flow) Physical environment (Medium K) Hydrologic conditions (q, S f ) A q q

Comparison of flow equations Open Channel Flow Porous medium flow Why is there a different power of S f ?

Energy B = E = mv 2 /2 + mgz + E u ;  = dB/dm = v 2 /2 + gz + e u ; dE/dt = dH/dt – dW/dt (heat input – work output) First Law of Thermodynamics Generally in hydrology, the heat or internal energy component (E u, dominates the mechanical energy components (mv 2 /2 + mgz)

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

Energy Units In SI units, the basic unit of energy is Joule (J), where 1 J = 1 kg x 1 m/s 2 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

Energy fluxes and flows Water Volume [L 3 ] (acre-ft, m 3 ) Water flow [L 3 /T] (cfs or m 3 /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/L 2 T] in Watts/m 2 Energy flow of 1 Joule/sec Area = 1 m 2

MegaJoules When working with evaporation, its more convenient to use MegaJoules, MJ (J x 10 6 ) So units are –Energy amount (MJ) –Energy flow (MJ/day, MJ/month) –Energy flux (MJ/m 2 -day, MJ/m 2 -month)

Internal Energy of Water Heat Capacity (J/kg-K)Latent Heat (MJ/kg) Ice Water Ice Water Water vapor 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) 2.5/0.33 = 7.6

Water Mass Fluxes and Flows Water Volume, V [L 3 ] (acre-ft, m 3 ) Water flow, Q [L 3 /T] (cfs or m 3 /s) Water flux, q [L/T] (in/day, mm/day) Water mass [m =  V] (Kg) Water mass flow rate [m/T =  Q] (kg/s or kg/day) Water mass flux [M/L 2 T =  q] in kg/m 2 - day Water flux Area = 1 m 2

Latent heat flux Water flux –Evaporation rate, E (mm/day) Energy flux –Latent heat flux (W/m 2 ), H l Area = 1 m 2  = 1000 kg/m 3 l v = 2.5 MJ/kg W/m 2 = 1 mm/day

Radiation Two basic laws –Stefan-Boltzman Law R = emitted radiation (W/m2)  = emissivity (0-1)  = 5.67x10 -8 W/m2-K 4 T = absolute temperature (K) –Wiens Law  = wavelength of emitted radiation (m) Hot bodies (sun) emit short wave radiation Cool bodies (earth) emit long wave radiation All bodies emit radiation

Net Radiation, R n R i Incoming Radiation R o =  R i Reflected radiation  albedo (0 – 1) R n Net Radiation ReRe Average value of R n over the earth and over the year is 105 W/m 2

Net Radiation, R n R n Net Radiation Average value of R n over the earth and over the year is 105 W/m 2 G – Ground Heat Flux LE – EvaporationH – Sensible Heat

Energy Balance of Earth Sensible heat flux 7 Latent heat flux 23 19

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

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

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

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

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

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

Latent heat flux, Jan 2003, 1500z

Digital Atlas of the World Water Balance (Temperature)

Digital Atlas of the World Water Balance (Net Radiation) Why is the net radiation large over the oceans and small over the Sahara?