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Page 1: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Surface Water BalanceSurface Water Balance

Page 2: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Review of last lecture: Surface energy balanceReview of last lecture: Surface energy balance

dT/dt

SWdn =Scos

SWup =SWdn

LWdn =Tair4

LWup=Ts4

LH=CdLV(qsurface- qair)

SH=CdCpV(Tsurface- Tair)

Fc = - dT/dz

Incoming shortwave + Incoming longwave = Reflected shortwave + Emitted longwave + Latent heat flux + Sensible heat flux + Subsurface conduction

• What is sensible heat flux? What is latent heat flux?

• Bowen ratio B= SH/LH = Cp(Tsurface - Tair) / L(qsurface - qair) provides a simple way for estimating SH and LH when the net radiative flux Fr is available LH=Fr/(B+1), SH=Fr B/(B+1)

• Factors affecting soil thermal conductivity

• Other heat sources: precipitation, biochemical, anthropogenic

Page 3: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

The global water cycleThe global water cycle

Page 4: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Video: Weather WetVideo: Weather Wet

Page 5: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Components of global water cycleComponents of global water cycle

• Atmosphere (water vapor, clouds, precipitation)• Land (soil moisture, rivers, snow, ice sheet and glaciers)• Sea ice• Ocean• Biosphere (including human beings)

Page 6: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Atmosphere: water vaporAtmosphere: water vapor

Page 7: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Atmosphere: PrecipitationAtmosphere: Precipitation

GPCP Annual Mean Precipitation for 1979-2005 (mm/day)

Inter-tropical convergence zone (ITCZ)

Strong rainfall (heating)

Weak rainfall

Page 8: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Land snow/Ice cover provide a reservoir Land snow/Ice cover provide a reservoir

Page 9: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Flow of >1000 rivers on the seven continentsFlow of >1000 rivers on the seven continents

Amazon river Yangtze riverMississippi river

Page 10: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Land: Soil moistureLand: Soil moisture

Page 11: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Flow of ocean currentsFlow of ocean currents

Page 12: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

A significant fraction of the human body is A significant fraction of the human body is water (~75%)water (~75%)

About every 16 days nearly 100% of the water in a human body is exchanged.

The remaining: fat, protein, carbonhydrate, other solids

Page 13: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

So the water we drink may come from …So the water we drink may come from …

Therefore we need to protect the environment because any pollution we put into the environment may someday come back into our bodies

Page 14: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Surface water balanceSurface water balance

dS/dt

Precipitation (P)

Evaportranspiration (E)

Runoff (Rs)

Irrigation (I)

Infiltration (Rg)

The changing rate of soil moisture S

dS/dt = P - E - Rs - Rg + I

Page 15: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Evaporation from bare soil (Eb)

EvaportranspirationEvaportranspiration• Is equivalent to latent heat flux

• Has four components: E = Eb + Ei + Es + TR

Evaporation from inception storage

(Ei)

Transpiration (TR)

Snow sublimation (Es)

Page 16: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Evaportranpiration: Penman-Monteith equationEvaportranpiration: Penman-Monteith equation

where λ is latent heat of evaporation, Rn is the net radiation, G is the soil heat flux, (es - ea) represents the vapour pressure deficit of the air, a is the mean air density at constant pressure, cp is the specific heat of the air, represents the slope of the saturation vapour pressure temperature relationship, is the psychrometric constant (=66 Pa/K), and rs and ra are the (bulk) surface and aerodynamic resistances.

Page 17: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Soil moistureSoil moisture• Typically expressed as ‘volumetric soil water content’

S = Vwater / Vsoil

• Increases with depth• Complicated to measure

Root zone

Intermediate zone

Ground water

Page 18: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Soil moisure regimesSoil moisure regimes

Page 19: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

US Soil moisture mapUS Soil moisture map

Page 20: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Palmer drought severity index (PDSI)Palmer drought severity index (PDSI)

• was developed by Wayne Palmer in the 1960s and uses temperature and rainfall information in a model to determine dryness of soil moisture.

• is most effective in determining long term drought (a matter of several months) and is not as good with short-term forecasts (a matter of weeks).

• It uses a 0 as normal, and drought is shown in terms of minus numbers; for example, minus 2 is moderate drought, minus 3 is severe drought, and minus 4 is extreme drought.

Page 21: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Change of PDSI in the last 100 yearsChange of PDSI in the last 100 years

Page 22: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

PSDI for US in January 2015PSDI for US in January 2015

Page 23: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

A different index: U.S. Drought MonitorA different index: U.S. Drought Monitor

Page 24: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Video: Crippling Drought in the Video: Crippling Drought in the Golden State: California Soul Golden State: California Soul

• https://www.youtube.com/watch?v=lmUwjk4S3gw

Page 25: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Glacier mass balanceGlacier mass balance

Page 26: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Structure of a glacierStructure of a glacier

• A glacier forms when the accumulation of snow and ice exceeds its overall loss of mass by ablation (sublimation and melting).

• A glacier can be divided into two zones; the zone of accumulation and the zone of ablation. They are separated by the “equilibrium line”.

Page 27: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Accumulation zoneAccumulation zone

• Surface accumulation processes include snow and ice from direct precipitation, avalanches and windblown snow.

• There may be minor inputs from hoar frost (radiation frost).

• The snow and ice is then transferred downslope as the glacier flows.

Page 28: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Ablation zoneAblation zone

• Surface ablation processes include surface melt, surface meltwater runoff, sublimation, avalanching and windblown snow.

• Glaciers on steep slopes may also dry calve, dropping large chunks of ice onto unwary tourists below.

• Other processes of ablation include subaqueous melting, and melting within the ice and at the ice bed

Page 29: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Glacier mass balance for the globeGlacier mass balance for the globe

Page 30: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Glacier mass balance for different regionsGlacier mass balance for different regions

Page 31: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Summary:Summary:Components of global water cycleComponents of global water cycle

• Atmosphere (water vapor, clouds, precipitation)• Land (soil moisture, rivers, snow, ice sheet and glaciers)• Sea ice• Ocean• Biosphere (including human beings)

Page 32: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Surface water balanceSurface water balance

dS/dt

Precipitation (P)

Evaportranspiration (E=Eb+Ei+Es+TR)

Penman-Monteith eq

Runoff (Rs)

Irrigation (I)

Infiltration (Rg Darcy’s law)

The changing rate of soil moisture S

dS/dt = P - E - Rs - Rg + I

(PDSI, desertification)

Page 33: Surface Water Balance. Review of last lecture: Surface energy balance dT/dt SWdn =Scos  SWup =SWdn  LWdn =  Tair 4 LWup =  Ts 4 LH=  C d LV(q surface

Works citedWorks cited

• http://ffden-2.phys.uaf.edu/212_spring2011.web.dir/Jocelyn_Simpson/Slide3.htm

• http://www.antarcticglaciers.org/modern-glaciers/introduction-glacier-mass-balance/