ce 394k.2 mass, momentum, energy

36
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

Upload: orsin

Post on 07-Feb-2016

35 views

Category:

Documents


0 download

DESCRIPTION

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. - PowerPoint PPT Presentation

TRANSCRIPT

Page 1: CE 394K.2  Mass, Momentum, Energy

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
Page 3: CE 394K.2  Mass, Momentum, Energy

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

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

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

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
Page 8: CE 394K.2  Mass, Momentum, Energy

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

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

http://www.csr.utexas.edu/ocean/mss.html

Page 11: CE 394K.2  Mass, Momentum, Energy

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

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

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

Subsurface flowDarcy’s equation

fKSA

Qq

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

Comparison of flow equations

2/13/249.1fSR

nA

QV

fKSA

Qq

Open Channel Flow

Porous medium flow

Why is there a different power of Sf?

Page 16: CE 394K.2  Mass, Momentum, Energy

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

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

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

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

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

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

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

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

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

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

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

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

Energy balance at earth’s surfaceDownward short-wave radiation, Jan 2003

600Z

Page 29: CE 394K.2  Mass, Momentum, Energy

Energy balance at earth’s surfaceDownward short-wave radiation, Jan 2003

900Z

Page 30: CE 394K.2  Mass, Momentum, Energy

Energy balance at earth’s surfaceDownward short-wave radiation, Jan 2003

1200Z

Page 31: CE 394K.2  Mass, Momentum, Energy

Energy balance at earth’s surfaceDownward short-wave radiation, Jan 2003

1500Z

Page 32: CE 394K.2  Mass, Momentum, Energy

Energy balance at earth’s surfaceDownward short-wave radiation, Jan 2003

1800Z

Page 33: CE 394K.2  Mass, Momentum, Energy

Energy balance at earth’s surfaceDownward short-wave radiation, Jan 2003

2100Z

Page 34: CE 394K.2  Mass, Momentum, Energy

Latent heat flux, Jan 2003, 1500z

Page 35: CE 394K.2  Mass, Momentum, Energy

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

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