lecture%15% - university of chicago
TRANSCRIPT
GEOS 24705 ENST 24705 ENSC 21100
Lecture 15
Electricity markets, turbines, hydro
Copyright E. Moyer 2016
What sets the amounts that people pay?
In the old days
The uBliBes owned everything, and would charge customers enough to recover their costs. The state uBliBes commission would approve the rates.
Nowadays
Generator price set by the day-‐ahead market: Sets the hour by hour price that generators receive for power or for capacity.
Wholesale price set by market and by FERC: Sets the markup that the RTO can charge over market. Sets the transmission rates.
Retail price set by state u=li=es commissions: Determines the rates that the uBliBes can charge their customers. Flat rates – no hourly changes.
“The duck has landed” in California ResidenBal solar wipes out mid-‐day demand. (Home genera&on counts as canceling demand). Then demand spikes as the sun sets – by 2020 power demand will ~ double in 2.5 hours.
Features that may matter to turbine design
• Fluid velocity • Fluid density • Pressure drops
if molecules just push on blades: “impulse turbine” if turbine exploits pressure drop: “reacBon turbine” if elements of both: “impulse-‐reacBon”
Features that may matter to turbine design
Wind: low velocity, low density, no pressure drop Water wheel or run-‐of-‐river hydro: low velocity, high density, no pressure drop Dam hydro: low velocity, high density, large pressure drop Gas or steam turbine: high velocity, low density, large pressure drop
Invented in 1884 (Parsons) 80% of world’s electricity today (all external combusBon) Power growth rapid: first turbine 75 kW (1890), by 1912 Chicago (Fisk!) was 25 MW, > 50 MW in Parson’s lifeBme, > 1 GW now
1. STEAM TURBINE
First built in 1903 (Elling). (Conceived of in 1791, but was not buildable) Adop=on slow: no commercializaBon Bl 1918, no rouBne use Bl 1930s.
2. GAS TURBINE
Invented in 1848 (James Francis). For the texBle mills at Lowell, MA – improved efficiency over tradiBonal water wheel design Most common hydro turbine in use today
3. HYDRO TURBINE (Francis)
4. HYDRO TURBINE (Pelton wheel)
Invented in 1870s (Lester Pelton). Improvement on tradiBonal water wheel used in CA gold mining in small streams Preferred hydro turbine in certain condiBons: small flow, large drop
Why dam a river to get energy from its flow?
dam vs. run-‐of-‐river If the point is just to get kine=c energy from the
river’s flow, why do you need a dam at all? less environmentally damaging if you didn’t dam…
Photo: L. PapaKaster Photography
Dam increases extractable energy
Water is guided to the turbine via a “penstock” that controls flow and pressure Image: Xeneca Corp.
Raising “head” allows harnessing energy that is otherwise lost during flow of river
Energy flux and power
Power = ε � ρ � A � v
f f
Flux = flow of something per area per Bme
A
l = v * t
Volume flux = V/A � t = (A � v � t)/(A � t) = v Mass flux = volume flux � (mass/volume) = v � ρ
Energy flux = mass flux � (energy/mass) = v � ρ � ε
Energy/mass in a flow: Bernoulli’s equa=on
Energy/mass = ½ v2 + g h + p/ρ
kineBc gravitaBonal pressure gradient
Can swap energy back and forth between these terms. This form is for incompressible fluids only.. Assumes no change in volume or temperature. Gases are compressible -‐ heat on adiabaBc compression, cool on adiabaBc expansion. Need to add in a term for the thermal energy (“internal energy”) of the gas, since energy swaps into and out of heat in gas.
Energy in a flow: wind power (kine&c term)
Energy/mass = ½ v2 + g h + p/ρ
kineBc gravitaBonal pressure gradient
P = ε � ρ � A � v energy density is kine&c term: ε =½ v2
P = ½ ρ A v3
Flow f = mass/Bme f f
Power = energy/mass * mass/volume * volume/Bme
Energy in a flow: dam hydro (pot. energy term)
Energy/mass = ½ v2 + g h + p/ρ
kineBc gravitaBonal pressure gradient
P = ε � ρ � A � v energy density is pot. energy term: ε =gh
P = g h ρ � (A � v)
Flow f = mass/Bme f f
Power = energy/mass * mass/volume * volume/Bme
Energy in a flow: dam hydro (recover in pressure term)
Energy/mass = ½ v2 + g h + p/ρ
kineBc gravitaBonal pressure gradient
P = ε � ρ � A � v energy density is pressure term: ε =p/ρ
P = p � (A � v)
Flow f = mass/Bme f f
Power = energy/mass * mass/volume * volume/Bme
Pelton (1870s) High head, low flow Impulse turbine used with dam
3 main dam hydro turbine designs choice governed by flow rate and pressure
Images: L. Voith Siemens M. Copyright unknown R. Photo V.O. Kanninen
Francis (1848) Medium head, all but highest flows Pure reac<on turbine
Kaplan (1922) Low head, all flows Pure reac<on turbine
Francis turbine: reaction turbine medium head (10 - 500 m), high flow Hydro getting bigger…over 800 MW max Efficiency already near max – but larger scale lowers cost
Francis turbine runner from Three Gorges Dam project, China (700 MW)
Runner is only small part of turbine assembly Inlet spiral is even larger
Francis turbine intake spiral from Grand Coulee Dam
Turbine assembly contains more than just runner
What is the input spiral for? Why does it decrease in radius? What is the funcBon of the drap tube? Why does it fan outwards?
Turbine assembly contains more than just runner
What is the input spiral for? Why does it decrease in radius? The spiral directs water radially to the runner. Because water flows in to center and is lost, the diameter has to narrow to keep velocity constant. What is the funcBon of the drap tube? Why does it fan outwards? To produce a slow-‐down of moBon and drop in pressure. (It’s an “anB-‐nozzle”)
How fast does the turbine rotate?
15 m rotor for 400 MW generator at Son La hydroelectric facility, Vietnam (L). Rewinding the rotor for a small hydroelectric plant (R)
Will a hydro turbine rotate as fast as a gas or steam turbine? No – gas turbines rotate at 60 Hz but hydro turbines rotate more slowly, someBmes ~1 Hz How does it make 60 Hz AC electricity? By increasing the number of poles in the rotor magnet