CE 394K.2 Mass, Momentum, Energy
description
Transcript of CE 394K.2 Mass, Momentum, Energy
![Page 1: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/1.jpg)
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
![Page 2: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/2.jpg)
![Page 3: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/3.jpg)
Reynolds Transport Theorem
cv cs
dAvddt
dB.
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
![Page 4: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/4.jpg)
Continuity Equation
cv cs
dAvddt
d
dt
dB.
B = m; b = dB/dm = dm/dm = 1; dB/dt = 0 (conservation of mass)
cv cs
dAvddt
d.0
= constant for water
cv cs
dAvddt
d.0
IQdt
dS0 QI
dt
dSorhence
![Page 5: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/5.jpg)
Continuity equation for a watershed
I(t) (Precip)
Q(t) (Streamflow)dS/dt = I(t) – Q(t)
dttQdttI )()(Closed system if
Hydrologic systems are nearly alwaysopen systems, which means that it isdifficult to do material balances on them
What time period do we chooseto do material balances for?
![Page 6: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/6.jpg)
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?
![Page 7: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/7.jpg)
![Page 8: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/8.jpg)
Momentum
cv cs
dAvddt
d
dt
dB.
B = mv; b = dB/dm = dmv/dm = v; dB/dt = d(mv)/dt = F (Newtons 2nd Law)
cv cs
dAvvdvdt
dF .
0 Fso
For steady flow cv
dvdt
d0
For uniform flow 0. cs
dAvv
In a steady, uniform flow
![Page 9: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/9.jpg)
Surface and Groundwater Flow Levels are related to Mean Sea Level
Earth surface
EllipsoidSea surface
Geoid
Mean Sea Level is a surface of constant gravitational potential called the Geoid
![Page 10: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/10.jpg)
http://www.csr.utexas.edu/ocean/mss.html
![Page 11: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/11.jpg)
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
![Page 12: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/12.jpg)
Energy equation of fluid mechanics
g
V
2
21
fhg
Vyz
g
Vyz
22
22
22
21
11
Datum
z1
y1
bed
water surface
energy grade line
hf
z2
y2
g
V
2
22
L
How do we relate friction slope, L
hS f
f to the velocity of flow?
![Page 13: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/13.jpg)
Open channel flowManning’s equation
2/13/249.1fSR
nV
Channel Roughness
Channel Geometry
Hydrologic Processes(Open channel flow)
Physical environment(Channel n, R)
Hydrologic conditions(V, Sf)
![Page 14: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/14.jpg)
Subsurface flowDarcy’s equation
fKSA
Hydraulic conductivity
Hydrologic Processes(Porous medium flow)
Physical environment(Medium K)
Hydrologic conditions(q, Sf)
Aq q
![Page 15: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/15.jpg)
Comparison of flow equations
2/13/249.1fSR
nA
QV
fKSA
Open Channel Flow
Porous medium flow
Why is there a different power of Sf?
![Page 16: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/16.jpg)
Energy
cv cs
dAvddt
d
dt
dB.
B = E = mv2/2 + mgz + Eu; = dB/dm = v2/2 + gz + eu; dE/dt = dH/dt – dW/dt (heat input – work output) First Law of Thermodynamics
cv cs
uu dAvegzv
degzv
dt
d
dt
dW
dt
dH.)
2()
2(
22
Generally in hydrology, the heat or internal energy component(Eu, dominates the mechanical energy components (mv2/2 + mgz)
![Page 17: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/17.jpg)
Heat energy
• Energy– Potential, Kinetic, Internal (Eu)
• 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
fhg
Vyz
g
Vyz
22
22
22
21
11
![Page 18: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/18.jpg)
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
![Page 19: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/19.jpg)
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 of1 Joule/sec
Area = 1 m2
![Page 20: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/20.jpg)
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)
![Page 21: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/21.jpg)
Internal Energy of Water
0
1
2
3
4
-40 -20 0 20 40 60 80 100 120 140
Temperature (Deg. C)
Inte
rna
l En
erg
y (
MJ
)
Heat Capacity (J/kg-K) Latent Heat (MJ/kg)Ice 2220 0.33Water 4190 2.5
Ice
Water
Water vapor
Water may evaporate at any temperature in range 0 – 100°CLatent heat of vaporization consumes 7.6 times the latent heat of fusion (melting)
2.5/0.33 = 7.6
![Page 22: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/22.jpg)
Water Mass Fluxes and Flows
• Water Volume, V [L3] (acre-ft, m3)
• Water flow, Q [L3/T] (cfs or m3/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/L2T = q] in kg/m2-day
Water flux
Area = 1 m2
![Page 23: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/23.jpg)
Latent heat flux
• Water flux– Evaporation rate, E
(mm/day)
• Energy flux – Latent heat flux
(W/m2), Hl
Area = 1 m2
ElH vl = 1000 kg/m3
lv = 2.5 MJ/kg
)/)(1000/1(*)/)(86400/1(*/1)/(105.2)/(1000/ 632 mmmsdaydaymmkgJmkgmW
28.94 W/m2 = 1 mm/day
![Page 24: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/24.jpg)
Radiation
• Two basic laws– Stefan-Boltzman Law
• R = emitted radiation (W/m2)
= emissivity (0-1) = 5.67x10-8W/m2-K4
• T = absolute temperature (K)
– Wiens Law = wavelength of
emitted radiation (m)
4TR
T
310*90.2
Hot bodies (sun) emit short wave radiationCool bodies (earth) emit long wave radiation
All bodies emit radiation
![Page 25: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/25.jpg)
Net Radiation, Rn
Ri Incoming Radiation
Ro =Ri Reflected radiation
albedo (0 – 1)
Rn Net Radiation
Re
ein RRR )1(
Average value of Rn over the earth and over the year is 105 W/m2
![Page 26: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/26.jpg)
Net Radiation, Rn
Rn Net Radiation
GLEHRn
Average value of Rn over the earth and over the year is 105 W/m2
G – Ground Heat Flux
LE – EvaporationH – Sensible Heat
![Page 27: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/27.jpg)
http://www.uwsp.edu/geo/faculty/ritter/geog101/textbook/energy/radiation_balance.html
Energy Balance of Earth
6
4
10070
51
21
26
38
6
20
15
Sensible heat flux 7Latent heat flux 23
19
![Page 28: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/28.jpg)
Energy balance at earth’s surfaceDownward short-wave radiation, Jan 2003
600Z
![Page 29: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/29.jpg)
Energy balance at earth’s surfaceDownward short-wave radiation, Jan 2003
900Z
![Page 30: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/30.jpg)
Energy balance at earth’s surfaceDownward short-wave radiation, Jan 2003
1200Z
![Page 31: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/31.jpg)
Energy balance at earth’s surfaceDownward short-wave radiation, Jan 2003
1500Z
![Page 32: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/32.jpg)
Energy balance at earth’s surfaceDownward short-wave radiation, Jan 2003
1800Z
![Page 33: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/33.jpg)
Energy balance at earth’s surfaceDownward short-wave radiation, Jan 2003
2100Z
![Page 34: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/34.jpg)
Latent heat flux, Jan 2003, 1500z
![Page 35: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/35.jpg)
Digital Atlas of the World Water Balance(Temperature)
http://www.crwr.utexas.edu/gis/gishyd98/atlas/Atlas.htm
![Page 36: CE 394K.2 Mass, Momentum, Energy](https://reader033.fdocuments.net/reader033/viewer/2022051518/56815b1b550346895dc8ca39/html5/thumbnails/36.jpg)
Digital Atlas of the World Water Balance(Net Radiation)
http://www.crwr.utexas.edu/gis/gishyd98/atlas/Atlas.htm
Why is the net radiation largeover the oceans and small over the Sahara?
GLEHRn