Stanford Summer Energy School Fundamentals of the Electric Grid ! Kevin Tomsovic CTI Professor and EECS Department Head tomsovic@tennessee.edu Overview – Part 1 • Broad overview of power grid fundamentals • DC vs. AC • Edison and Westinghouse (Edison may yet win) • Three phase systems • Power concepts • Traditional generation technologies • Synchronism as the foundation of operation • Load – Frequency control • Load following – frequency control • The power system in the steady-state • Transmission system and power flows • Reactive power/voltage and real power/phase • Power system reliability • Security vs. adequacy Components of the Grid • Generation • Transmission – 115 kVolts 765 kVolts – Networked • Distribution – 4 kVolts to 69 kVolts – Radial • Load http://www.nerc.com/page.php?cid=1|15 DC vs. AC • Direct current (DC) – DC machines – Batteries – Fuel cells – Photovoltaic ! i (t ) = I ! • Alternating current (AC) – AC machines – Power electronic converters – 60 Hertz in the US i(t ) = I sin(2πft ) Edison vs. Tesla/Westinghouse • DC – Pushed by Thomas Edison (GE) – Could not change voltage levels (no transformer) so cannot transmit over long distances – DC generator (high maintenance) – Difficult to interrupt high currents (no zero crossing) • AC – Nikola Tesla (moved from Edison to Westinghouse) – Can efficiently change voltage levels (transformer) and so transmit over long distances (high voltage) – Induction and synchronous machines – Easier to interrupt high currents ! ➔ DC actually has many advantages Frequency and Phase • The number of “cycles” per second (Hertz) – Zero for DC – Many options for AC – Grid - 60 in the US, 50 in Europe, both in Japan – Aircraft – 400, Some trains in Europe – 16.67 • Phase – relative relationship between two signals – Usually measured in degrees (easy to translate to time) ! ! ! ! – 30 degrees or 1.4 msec i1 (t ) = I sin(2πft ) i2 (t ) = I sin(2πft − π / 6) Phasors • Need a simpler notation and all that matters is magnitude and relative phase if single frequency • Define δ i(t ) => I∠δ ! • We properly do this using Euler’s identity ! e j 2πft + jδ = cos(2πft + δ ) + j sin(2πft +Oδ ) • with j an imaginary number or 90 Three phase power an extremely useful trick • All large scale power applications i!a (t ) = I sin(2πft ) i!b (t ) = I sin(2πft − 2π / 3) i!c (t ) = I sin(2πft − 4π / 3) ! ! i!a (t ) + ib (t ) + ic (t ) = 0 • No need for return line to carry current Electric power • By definition ! ! ! p(t ) = v(t )i(t ) i(t ) = I sin(2πft ) v(t ) = V sin(2πft + π / 6) • Average power is what does useful work ! ! • P 1T P = ∫ p(t )dt oftenT called real 0 power Three phase electric power another major benefit • Assume balanced in all three phases ! p ( t ) = p a ( t ) + pb ( t ) + p c ( t ) ! ! ! ! • Constant power output – far more efficient Apparent Power S calculation using phasors • By definition ! S = VI * = P + jQ P – real part of S Q – imaginary part of S, reactive power S Q V I P What is reactive power? And why should we worry about it? • The part of p(t) which does no work on average (but it may be needed to get work done) • Analogies – Pressure in a water hose • – Foam on the beer (just takes up room in glass) • Physically – Primarily line charging (magnetic fields) associated with transmission lines and motor windings • Practically – Needed to maintain voltage for long distance transmission and to supply induction machines P (Watts – you pay for this) Energy Conversion Three phase synchronous Machines • DC supplied to rotor which is driven at some constant speed of rotation (say 3600 RPM for two pole machine resulting in 60 Hz) • Three phase windings spaced by 120 degrees • Power is produced only at this frequency (else p(t)=0) • Relative angle between fields determines real power output STATOR b' c ROTOR a N c' S b a' Generator mix 80% Thermal (nuclear, coal, gas, etc.) 20% Hydro Essentially all synchronous Steam Turbine/Generator Coulee Hydro Units at Synchronism Since most generation is from synchronous machines, the interconnected power system swings together. Frequency • To maintain frequency, load and generation (minus losses) must balance • An increase in load decreases frequency so generators respond to frequency dip by increasing output • Coordination from control centers results in a simple but very effective means of load following ! • Load frequency control • Inputs – scheduled and actual tie line flows (difference is area control errors), frequency deviation (also frequency response characteristic) • Output – generator set point adjustments around once every 4 seconds North American Control Areas Frequency Monitoring (FNET – Yilu Liu, UT) Frequency Monitoring (FNET – Yilu Liu, UT) Frequency Event Nigeria – Shows system dependence Summary Comments and Opinions • Electricity grid is central to solving energy problems • Wind has perhaps the greatest potential – difficulty of variability may have been overstated by media and utilities • Appropriate control methods need to be developed with greater demand side response and new storage • Shifting of greater load to grid has benefits both for reduced emissions and for easier control References • A few useful websites http://tcip.mste.uiuc.edu/applet1.html http://tcip.mste.uiuc.edu/applet2.html http://www.eia.doe.gov/ ! • Some general introductory power texts Bergen and Vittal, Power Systems Analysis, Prentice Hall, 2000. 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