Electrical Systems And Electric Energy Management Main Topics Discussed • Electric Rates • Electrical system utilization • Power quality • Harmonics • Power factor improvement Session 14.2 2 Review of Electric Cost Components Energy cost - e.g. $0.05/kWh Demand cost - e. g. $6.50/kW/mo Fuel adjustment - e.g. $0.005/kWh Power factor penalty - e.g. $6.50/kVA/mo or kW billed = kW u (0.85/PF) Ratchet clause - e.g. Maximum of (kW this month, or 70% of maximum kW in last 11 months) Session 14.3 3 Power Computation Formulas Single-phase system P = 1 u V u I u PF Where PF = power factor Three-phase system P = 3 u V u I u PF 3 = 1.732 Session 14.4 4 Examples a) For a 10 ampere, 120 volt, electric space heater P = 1 x 120 u 10 u 1.0 = 1200 watts b) For a three phase 460 volt, 20 ampere motor with power factor of 90% at full load P = 3 u 0.460 u 20 u 0.9 = 14.34 kW 5 Session 14.5 Electric Motor Equations Pr [kW]= 3 u kV u I u PF Ps[kVA]= 3 u kV u I PF kW/kVA = = Pr [kW]= cos) HP u 0.746 kW u Load Factor Efficiency Session 14.6 6 Power Quality • Power Quality is related to how well a bus voltage—usually our facility load bus voltage—maintains a pure sinusoidal waveform at rated voltage and frequency. • PQ issues involve all momentary phenomena including spikes, notches and outages; as well as harmonics and power factor. • Modern electronic equipment both causes and is affected by the problem. • Power Quality is becoming one of the most important issues in energy management today. Session 14.7 7 Harmonics • Harmonics are a multiple of the fundamental frequency. If the fundamental frequency is 60 hertz, the 2nd harmonic is 120 Hz, the 3rd is 180 Hz, the 4th is 240 Hz, etc. • Harmonics are usually generated by solid-state-based equipment such as switching power supplies in PCs, DC drives, variable frequency drives (VFDs), electronic ballasts, arc welders and ovens. Session 14.8 8 Importance of Grounding • Up to 80 percent of PQ problems in facilities today may be caused by wiring and grounding systems that met the NEC at the time, but do not meet the needs of today's sensitive electronic equipment. • The first step taken to deal with PQ problems should be to inspect the wiring and grounding, and clean and tighten all connections. Loose connections come from vibration, oxidation, corrosion, and age. Session 14.9 9 What Problems Occur Because of Harmonics? • Circuit breakers tripping • Neutrals overheating (smoke, fire) • Panel or transformer overheating • RFI – Radio Frequency Interference • Errors/damage in Electronic Equipment • Digital clocks running fast • Failures in power factor correction capacitors Session 14.10 10 Mitigation of Harmonic Problems • Derate equipment (symptom treatment) 50% Transformers 70% Load centers Circuit breakers Neutrals • Install preventive equipment Inductors Harmonic filters Isolation transformers Locate near drive if possible Connect back to "strongest" point of power system – the load center 11 Session 14.11 Power Triangle kW ) kVAR kVA Session 14.12 12 Schematic arrangement showing how capacitors reduce total kVa by supplying magnetizing requirements locally. 13 Session 14.13 Sample Power Factor Example A facility is operating with a demand of 2000 kW. The 2500 kVa transformer is fully loaded. How many kVARS are required to bring the power factor back to unity? kW2 + kVAR2=kVa2 kVAR2= kVa2-kW2 kVAR 2500 2 2000 2 Session 14.14 1500 14 Sample Power Factor Problem During my last energy audit I saw a 100 HP electric motor that had the following information on the nameplate: 460 volts; 114 amps; three phase; 95% efficient – all at full load . What is the power factor of this motor? [(100 hp)*(0.746 kW/HP)/0.95] =[(1.73)*(0.46 kV)*(114 amp)*(PF)] 78.52 kW = (90.72 kVa)*(PF) PF = (78.52 kW / 90.72 kVa) = 0.866 Session 14.15 Transformer M 15 Where to Put Power Factor Correction Capacitors Session 14.16 16 Sample CEM Test Question • A facility is operating at a power factor of 70% with a real power load of 2000 kW. How much corrective capacitance in kVAR is needed to improve the facility power factor to 90%? • kVAR = Table Factor x Real power load in kW Session 14.17 17 Short Power Factor Table Session 14.18 18 CEM Review Questions 1. If power factor correction capacitors are located at the utility meter, but on the customer’s side of the meter, the power factor in the customer’s facility will not be improved. A. True B. False 2. A facility has a 100 kW electric resistance oven for drying parts. What is the power factor of the oven? A. 0 % B. 50% C. 90% D. 100% Session 5.1.19 19 3. A facility has a motor that draws 200 kVA and has a power factor of 70.7%. How many kW and how many kVAR does it draw? 4. A facility has a motor that draws 200 kVA and has a power factor of 80%. How many kW and how many kVAR does it draw? Session 5.1.20 20 Electric Motors and Motor Management Session 15.1 Electric Motor Management Why Bother? • Electric motors use over ½ all U.S. electricity • Motor driven systems use over 70% electric energy for many plants • Motor driven systems cost about $90 billion to operate per year • A heavily used motor can cost 10 times its first cost to run one year Session 15.2 Electric Motor Management Why So Difficult? • Load on most driven systems is unknown at least on retrofits • Very difficult to determine load accurately through measurements • Electric motor management is FULL of surprises • Yet, savings can be large (small percentage of a big number is a big number) • Important note: Often oversized wiring (above code) is cost effective in heavily used systems as it reduces I2R losses. (CDA and Southwire Corp.) Session 15.3 Electric Motor Management Types of Motors • AC Synchronous motors – One to two percent or so (but larger) – Large HP and slow speed applications typical – Similar in construction to induction motors, but more expensive – More efficient, can be run at leading PF – Can generate or absorb reactive power Session 15.4 Electric Motor Management Types of Motors • DC Motors – Good for precise speed control and strong torque properties – Not efficient, (historically) high maintenance, and higher down time (commutator and brushes need inspection and maintenance) – Newer brushless motors much better – Less than 5% of the motors today are DC – Replacing with a VFD driven AC motor may be cost effective especially if down time is reduced Session 15.5 Electric Motor Management Motor Types Cont. • AC Induction motors – AC induction motors work on electromagnetic field principles – Lagging power factor – Many different types (ODP, TEFC, etc.) – Approximately 95% of motors today are induction – Concentration for this discussion – Run on single- or three- phase power (most) Session 15.6 Electric Motor Basics Name Plates • • • • • • • • • HP ____ (shaft power design- output) NLRPM (synchronous speed) FLRPM (running RPM at design load) LRA (starting amps – 1 sec?) FLA (amps at design load and voltage) Volts (design voltage) Max. capacitor Efficiency (test vs. guaranteed) Service factor Session 15.7 Name Plate Example One Session 15.8 Session 15.9 Terminology (NEMA) • NEMA (National Electrical Manufacturers Association) • Standard Efficiency Motors: Pre Epact 92 motor • Energy Efficient Motors: Motors meeting EPACT requirements • Premium Efficiency Motors: Motors exceeding EPACT requirements (extra efficient, ultra high efficient, but these terms are not used by NEMA) Session 15.10 Electric Motor Basics Motor Speeds • Alternating current, thus speed will vary with pole pairs (inside motor, pole pairs between stator and rotor) • One pole pair (2 poles) - one RPM per cycle (60 cps or Hertz); two pole pairs – ½ rpm per cycle, etc. • Thus cycles sec u 60 sec min number of pole pairs 60 SPEED • SPEED = 3600, 1800, 1200, 900, 720, etc. (no other choices) for 60 Hz power Session 15.11 Electric Motor Basics Slip • • • • % Load = (True Slip)/(Design Slip) Design Slip = (NLRPM – FLRPM) True Slip = (NLRPM – RPM measured) Perfect indicator but very difficult to measure accurately (+- 1% typical) • Many don’t use this - why? – Difficult to measure accurately – Large motors are more efficient than small motors (more later) Session 15.12 Electric Motor Basics Slip Example • • • • • • • • • • FLRPM = 1760 (off name plate) Design HP = 50 (off name plate) Measured RPM = 1776 NLRPM = ? (obviously 1800) Design slip = 1800 – 1760 = 40 True slip = 1800 – 1776 = 24 % load = 24/40 = 0.6 or 60% True load = 50HP(0.6) = 30 HP See plot next slide, motors run very well at 60% load This motor will run very cool, is not causing a problem, why bother!! Session 15.13 Efficiency and PF vs. Load: % % Rated Load Session 15.14 Session 5.2.15 Session 15.16 Efficiency and PF (Cos phi) vs. Size % Rating Source: Electrical and Energy Management, IEES, Ga,Tech., Atlanta, GA. Session 15.17 Session 5.2.18 Electric Motor Management—Losses in Motors Note: This graph explains the efficiency drop off with load reduction Source: “Electrical Motors and Energy Conservation”, Ronald Cota, Specifying Engineer, July, 1978. Session 15.19 Motor Performance as Supply Voltage Varies Session 5.2.20 Voltage Imbalance • Problems can occur because of voltage imbalance between the three phases. This can be a serious problem in motors. • Percent voltage imbalance is found as the ratio of the largest phase voltage difference from average, divided by the average voltage. • For example, if we have 220, 215 and 210 volts, the voltage imbalance is 5/215 = .023, or 2.3 percent. Session 15.21 Voltage Imbalance Impact Source: Electrical and Energy Management, IEES, Ga,Tech., Atlanta, GA. Session 15.22 Approach to Motors • Leave existing motors alone until they fail except: – Exceptionally oversized motors (25% loading or so) – Sizes that are needed elsewhere (requires inventory) • When they fail, maybe buy new energy efficient motors (EPACT or Premium) instead of paying for rewind (much more on this later) • If financial incentives are available, much more may be done • Premium efficient motors need economic help in much of the country (PUC, Utility, motor mfgs.) Session 15.23 Motor Basics-Motor Rewinds • Most rewind motors over ___ HP • Typical rewinds cost 60+% of a new motor • New motor could be an energy efficient motor • Motor efficiency often suffers during rewind. Average drop about 1% according to one study and sometimes significantly more. • If efficiency drops, losses increases, motor runs hotter and won’t last as long Session 15.24 Electric Motor Management Energy Efficient Motors • Energy efficient motor characteristics – More efficient, and often higher power factor – Save energy and reduce demand – Reduce load on cables, transformers, etc. (note double whammy with higher efficiency and higher PF) – Speed is slightly higher (can be critical) – Significantly larger inrush (LRA) Session 15.25 Energy Efficient Motors Calculating Savings • Power and energy savings depends of efficiency of standard vs. energy efficient motor Power savings kWe § HP u 0.746 u LF · § HP u 0.746 u LF · ¸ ¸ ¨ ¨ EFF EFF ¹ EE ¹Stan © © • Energy savings = Power savings x Time = kWe X Operating hours Session 15.26 Electric Motor Principles Review ELECTRICAL MOTOR PRINCIPLES A three phase 50-hp motor with a load factor of 0.8 has an efficiency of 90%, what is the kW electrical power input? kW u 0.80 Hp 0.90 50 Hp u 0.746 1. kW 33.15 kW 33.15 kW Session 15.27 Electric Motor Principles Review 2. For the motor in 1. If the PF = cos ș = 0.7 and voltage is 480 V, what is the kVA and what is the amp draw? PF = 0.7 = kW/kVA 0.7 = 33.15/kVA or kVA = 33.15/0.7 = 47.36 kVA Also kVA = ¥3(kV)I = (¥3)(0.480) I = 47.36 kVA 33.15 kW I = 47.36 / (¥3 x 0.480) = 56.96 amps Session 15.28 47.36 Electric Motor Principles Review 3. Next, we want to correct the PF to 0.90. What size capacitor is needed and what is the impact on the amperage? ¨kVAR = 33.15 (tan cos-1 0.7 – tan cos-1 0.9) = 17.77 kVAR You will find the quantity in ( ) above in PF table (see Appendix) New kVA = 33.15/0.9 = 36.83 kVA = 36.83 = (kV)I¥3 I = 36.83/(0.480¥3) = 44.30 amps Thus, PF correction dropped amperage (upstream of the capacitor) from 56.96 to 44.30 amps or 22% 33.15 kW 36.83 47.36 ¨ kVAR=17.77 Also, new kVA = ¥3 kV I = 36.83 kVA Session 15.29 Tools to Help • The following software packages are available free from OIT of DoE. Contact OIT Clearinghouse 800-862-2086 or clearinghouse@ee.doe.gov They are also downloadable from the DoE web site. – MotorMaster: An energy-efficient motor selection and management tool. Motor inventory management, maintenance log tracking, efficiency analysis, savings evaluation, energy accounting, and environmental reporting – Pump System Assessment Tool (PSAT): Efficiency of pumping system operations. Pump performance and potential energy and other cost savings – ASD Master: Adjustable speed drive evaluation methodology and application software. Available from EPRI also. – Steam Sourcebook: Guide to improved steam system performance. Session 15.30 Motor Sample Problem • A recent advertisement said a premium efficiency 50 hp motor is available at 94.5%. It would replace a motor that presently runs at 90.7%. Given the parameters below, calculate the cost of operating both motors and the savings for conversion: – – – – Motor runs 8760 hours/year Demand cost is $10 per kW month Energy cost is $0.06/kWh Motor runs at 80% load all the time Session 15.31 Motor Sample Problem • Cost to operate existing motor – Demand – Energy – Total Session 15.32 Motor Sample Problem • Cost to operate premium efficiency motor – Demand – Energy – Total • Savings Session 15.33 Session 5.2.34 Motors, Drives and Air Compressors Session 16.1 Electric Motor Management Drives • Motors are fixed speed devices likely running between NLRPM and FLRPM • Other speeds on the driven end have to be engineered (which will affect the load on the motor) • Because of the “fan” laws (pumping or blowing) centrifugal devices are desired applications for varying CFM or GPM Session 16.2 Electric Motor Management Fan Laws (Centrifugal Devices ONLY) • CFM2 = CFM1(RPM2/RPM1) 1st law • SP2 = SP1(RPM2 /RPM1)2 2nd law • HP2 = HP1 (RPM2/RPM1)3 3rd law Session 16.3 Electric Motor Management Fan Laws Example • A 40 HP centrifugal blower is on a forced draft cooling tower. It is basin temperature controlled but conversion to a variable speed drive is being considered. When the blower is running at ½ speed, what is the impact on the CFM and what is the HP requirement? Session 16.4 Electric Motor Management Fan Laws Example • New CFM is __________old CFM • New HP requirement is: • These type savings are why variable speed drives are so popular today Session 16.5 Electric Motors Variable Volume Options • Outlet damper control (see sketch, location 1) • Inlet vane control (see sketch, location 2) • Magnetic clutching (see sketch, location 3) – Eddy current clutch – Permanent magnetic clutch • Variable Frequency Drives (see sketch, location 4) • Hydraulic drives, variable sheaves, etc. Session 16.6 Electric Motors Variable Volume Options Sketch 4 Session 16.7 Variable Speed Drive Alternatives Performance • The next page shows performance expectations from an older EPRI report • The page after that shows performance from a more recent PNL test • The third page shows an “average” VAV loading profile. It can be used as a default loading if better figures are not available. Quick Fan from DoE presents another default possibility. Session 16.8 Typical Power Consumption of Various Control Systems Session 16.9 Session 16.10 VFD: Default Loading Profile Session 16.11 Variable Frequency Drive Example • A large (50 HP) blower with inlet vane control drives a VAV system operating 6500 hours per year. Energy costs $0.04/kWh. What is the total savings per year for removing the inlet vane control and replacing it with a VFD? – Assume the performance figures in slide 9 apply – Assume the loading figures in slide 11 apply. – Construct an Excel spread sheet to do the calculations (will be done for you on next page) Session 16.12 Variable Frequency Drive Example Profit Improvement With Variable Frequency Drives Annual Savings for a Large Air Handler Session 16.13 Variable Frequency Drive Example • Calculation for 50% load row in Spread Sheet: (50HP)(0.746kW/HP)(0.72-0.20)(0.23)(6500hr/yr)($0.04/kWH) = $1159 Spread Sheet repeats this for all rows Session 16.14 Electric Motor Management Selection of Best Option • Magnetic clutches (permanent magnet or eddy current) – Bulky and heavy on motor shaft – No harmonics – Close to same savings as VFDs, but less Session 16.15 Electric Motor Management Other Drives • Variable sheaves – Very closely approach fan laws – Repeatability and maintenance often a problem – Many lock blades and install VFDs • Hydraulics – Effective – Expensive – Not often used as discussed here Session 16.16 Electric Motor Management Axial and Reciprocating • Centrifugal laws do not apply • More difficult to predict savings • If linear, no “real energy savings” over present on/off operation (certainly improved soft start operations and perhaps control) • Obviously, savings if converting from constant volume to variable volume Session 16.17 $$$$ Variable Speed Drive Applications • Any large centrifugal blower or pump that runs a lot! – Constant volume? Convert to var. volume – Variable volume with inlet or outlet control • Chilled water pumps, large campus • Cooling water pumps • VAVs using inlet vane • Forced draft (blower) cooling towers Session 16.18 Industrial Systems Compressed Air Management • Most expensive utility for many companies • Large cost reduction potential (20 to 30% common) • Management – Demand side – Supply side Session 17.2 Compressed Air Management • Each 100 hp compressor costs approximately $25,000 per year to operate • Try it: 8000 hours/year, $80/kW-yr, $0.05/kWh, running at 70% load. – Cost: • Typical first cost is $30,000 to $50,000 Session 17.3 Session 17.4 Air Systems Components Mgmt. • Demand side: should be managed first – Air leaks: large cost (see diagram), often 20% or more of capacity goes to leaks (artificial demand). Air leak detection and repair is extremely cost effective. – Air motors: great torque properties, small handprint, will not spark, but VERY ENERGY INEFFICIENT (7 hp air vs. 1 hp electric common) Session 17.5 Air Systems Components Mgmt. • Pressure supplied: proper level critical – Approximately 1% energy savings for each 2 psig drop (increase) in air pressure – Productivity cost can greatly exceed energy savings so be careful – Distribution drop should not be more than about 10% (90 psig at tank to supply 80 psig to tool) so receivers, better looping, etc. may enable pressure to be dropped without affecting tool Session 17.6 System Components • Supply Side – Air Compressor – Aftercooler – Receiver tank (storage) – Dryer – Distribution lines – Users (demand side) Session 17.7 Air System Components Mgmt. • Air Compressors – Screw: convenient, fairly efficient, skid mounted, most popular (100 HP or so) – Reciprocating: usually large, expensive, very efficient, part load well, often two stage – Centrifugal: usually quite large, modulates efficiently down to a point (surge), often VFD – Others: other types exist but these cover the vast majority Session 17.8 Air Systems Components Mgmt. • Intake air should be as cool and dry as possible • Intake air filter should be large with low pressure drop (2 psig), changed frequently • Multi stage with interstage cooling helps • Drivers can be electric motor (most), gas engine (load management or hybrid), or steam • Significant waste heat available (250,000 Btu/100 HP.) Easy to recover on packaged screw air cooled machines. Session 17.9 Air Systems Components Mgmt. • Sequencers: For multiple compressor dispatching – Use a remote (not in compressors) PID control loop to dispatch multiple compressors – Dramatically reduces control differential and smoothes operation – Can be extremely cost effective Session 17.10 Air Systems Components Mgmt. • After coolers: Air leaves a compressor at approximately 100% RH. – Cooling removes significant moisture; must be trapped and drained (exhausted) – Air cooled or water cooled and they are quite cost effective; save energy in dryer and provide dryer air. – Water cooled more effective but water should be used elsewhere or reused through small cooling tower Session 17.11 Air Systems Components Mgmt. • Receivers: storage devices to smooth demand on compressor – Further cooling removes more water (traps) – Can significantly reduce demand fluctuation on compressor controls – 2 to 4 gallons per CFM (but this varies a great deal) – Located before dryer (wet), after dryer (dry), throughout plant, and at large loads Session 17.12 Air Systems Components Mgmt. • Dryers: Further reduce dew point to avoid moisture in plant equipment – Refrigerated: cools air to about 40 F and reheats by precooling incoming air. Thus, dew point around 40 F. Not dry enough for many plants. – Desiccant: chemically removes moisture saturating media which must be dried before reusing. Usually two stacks. Expensive but dew point around -10 F. – Deliquescent: similar to desiccant but wet material is removed and replaced. Session 17.13 Air Systems Components Mgmt. • Distribution lines: get air where needed and provide further storage – Large lines are good for systems operating full time (often 4 inch) – All lines should be “looped” so air comes at any need from two directions • Traps and drains: traps and drains located throughout system to remove moisture. Can be a large source of air leaks. Session 17.14 Waste Heat Recovery • Successful waste heat recovery requires – Sufficient quantity – Sufficient quality (sufficiently high temperature) – Appropriate use – Timely production (or storage) – Economic use Session 17.15 Waste Heat Recovery • How much waste heat is available? • Conduct a waste heat survey – Temperature of waste stream – Quantity of waste stream – Heat available is q MC P (Tinitial Tfinal ) Session 17.16 Waste Heat Recovery • Other concerns – How close is location where heat is needed? – Is the waste heat available when needed? – Is the waste heat compatible with a suitable heat exchanger? • Fouling • Plugging • Corrosion Session 17.17 Waste Heat Recovery • Heat exchanger effectiveness, ɽ İ actual heat transfer to cold fluid maximum possible heat transfer – Effectiveness generally increases with heat exchanger area but not linearly – At some point a large area increase produces only a small effectiveness increase – 50% < ɽ < 90% Session 17.18 Waste Heat Recovery—Equipment Types • Shell and tube—for liquids and gases at all temperatures *B.L. Capehart, et. al., Guide to Energy Management, 5th ed., Fairmont Press, 2003, p. 320. Session 17.19 Waste Heat Recovery—Equipment Types • Radiation recuperator—for gases from medium to high temperatures *. *B.L. Capehart, et. al., Guide to Energy Management, 5th ed., Fairmont Press, 2003, p. 319. Session 17.20 Waste Heat Recovery—Equipment Types • Rotary heat wheel—for gases at all temperatures *B.L. Capehart, et. al., Guide to Energy Management, 5th ed., Fairmont Press, 2003, p. 321. Session 17.21 Waste Heat Recovery—Equipment Types • Heat pipes (capillary tubes)—for liquids and gases at all temperatures *B.L. Capehart, et. al., Guide to Energy Management, 5th ed., Fairmont Press, 2003, p. 253. Session 17.22 Industrial Insulation • Industrial insulation problems – Walls of vats, tanks, pipes or machines that were never insulated. – Damaged insulation. – Insulation removed for a repair and never replaced. Session 17.23 Industrial Insulation • Uninsulated walls result in the following temperature profile: Hot source at Th wall Twall, unins Tair inside surface outside surface of wall Session 17.24 Industrial Insulation • With insulation the profile changes: Hot source at Th wall insulation Inside surface outside surface of insulation Twall, ins=Twall, unins Touter ins Tair outside surface of wall Session 17.25 Industrial Insulation • From the Building Envelope Section recall• At steady-state, the heat loss in Btu/ft2·°F·hr is q A u 'T ȈR ª Btu º «¬ h »¼ • Where q is heat loss rate and ȈR is the sum of the resistances to the heat flow Session 17.26 Air Film Resistances (Industrial) *B.L. Capehart, et. al., Guide to Energy Management, 5th ed., Fairmont Press, 2003, p. 392. Session 17.27 Industrial Insulation • Thus for the uninsulated case with metal walls, q unins A(Th Tair ) R surface And both Th and Tair are easily measured. Session 17.28 Industrial Insulation • For the insulated metal wall case, ¦R R wall R insulation R surface • And again, the resistance of the wall can be neglected so that ¦R R insulation R surface Session 17.29 Industrial Insulation • Rinsulation is given by the general formula for R. R insulation t k • In general, R is proportional to the thickness of the substance resisting the heat flow. Session 17.30 k* for common materials Tm is mean temperature of Thot & Tsurf. P/C is pipe covering. *B.L. Capehart, et. al., Guide to Energy Management, 5th ed., Fairmont Press, 2003, p. 401. Session 17.31 Industrial Insulation • Personnel safety is often a concern. • Determine insulation thickness to bring the Touter ins to the “safe touch value” • 130 Tsafe touch, ºF 150* • For a specified surface temperature, the thickness of insulation needed is t insulation ª Th Touter insulation º k insulation R surface « » T T «¬ outer insulation air » ¼ *W. C. Turner, Energy Management Handbook, 5th Edition, Fairmont Press, 2005, p. 457. Session 17.32 Industrial Insulation • The North American Insulation Manufacturers Association (NAIMA) has a useful insulation program, 3E Plus • 3E Plus calculates – Insulation thicknesses – Energy loss and gain – Economic thicknesses – CO2, NOx, and carbon equivalent (CE) reductions • Useful software can be downloaded from http://www.pipeinsulation.org Session 17.33 Typical Pump System* *Drawing Figure 1 from Energy Reduction in Pumps and Pumping Systems, Hydraulic Institute. Photo courtesy Oklahoma State University Industrial Assessment Center. Session 17.34 Pump and System Curves Pump Curve (larger impeller) Head, H Pump Curve (smaller impeller) Velocity and Friction Head Elevation Head Pressure Head Volume Flow Rate, Q Session 17.35 Pump Summary 1. 2. 20% Savings on Normal Systems Keep Head to Minimum a. minimize capacity b. reduce process pressures c. lower outlet tanks d. use siphons e. reduce nozzle velocities f. use larger pipes g. use lower loss fittings h. eliminate throttle valves Session 17.36 System Curve Conclusions (cont.) 3. Avoid excessive safety margins 4. Select proper pump 5. Utilize VSDs 6. Utilize multiple pumps in parallel 7. Use pumps as HPRT Session 17.37 Conclusions (cont.) 8. Maintain, Maintain, Maintain! Session 17.38 Bibliography 1. IMPROVING PUMPING SYSTEM PERFORMANCE, A SOURCEBOOK FOR INDUSTRY, The Hydraulic Institute, (DOE Motor Challenge Program), Parsippany, NJ, 1997 2. Chelette, Garry, “A Pump Primer”, ENGINEERED SYSTEMS, August 2001, page 72 3. Rishel, James B., “Wire to Water Efficiency of Pumping Systems” ASHRAE JOURNAL, page 40, April 2001 Session 17.39 Appendix Session 17.40 Compressed Gas Systems • Quantifying air leaks – Compute the volume of all the receivers and major air headers. – Small air lines (under about 1 inch diameter) can be neglected. – Leaving some volume out makes the calculation conservative. Session 17.41 Compressed Gas Leaks • Quantifying air leaks – Apply the following formula to find standard cubic feet per minute (SCFM) lost R V (P1 - P2 ) ('T) 14.7 R average leakage rate (Scfm) V P1 system volume (ft 3 ) initial pressure (psig) P2 final pressure (psig) 'T Session 17.42 time interval over which leaks are measured (minutes) Compressed Gas Systems • Quantifying air leaks – Find the compressor specific efficiency in BHP/SCFM from the curve on the next page. – Then multiply [R x specific efficiency x 0.746 kW/Hp x operating hours x cost of energy (in $/kWh)]/Ș to arrive at annual cost of leaks. Session 17.43 Compressed Gas Systems *Compressed Air Systems, Varigas Research, Inc., Timinium, Maryland,1984 DOEICSI 40520 – T2, page 61. Session 17.44 Compressed Gas Systems • Quantifying air leaks – The figure is for 100 psig. Other pressures require a correction factor.* Pressure, psig Correction factor 130 1.15 120 1.11 110 1.05 100 1.00 90 0.942 80 0.880 *Nutter, DW, Britton AJ, and Heffington WM, “Five Common Energy Conservation Projects in Small and Medium-Sized Industrial Plants”, Fifteenth National Industrial Energy Technology Conference, Houston, Texas, Mar 24-25, 1993. pp 112-120. Session 17.45 Compressed Gas Systems • Quantifying air leaks – Other methods include measuring compressor run times and amp draws. – Drawbacks to all these methods include lack of location of leaks. – One method includes identifying the locations and trying to assign the size of an equivalent round hole to the leaks. – Then a chart such as the one on the next page is applied. Session 17.46 Compressed Gas Systems • Quantifying air leaks – Leak rate in SCFM through equivalent area round holes* *M.D. Oviatt and R.K. Miller, Industrial Pneumatic Systems, Fairmont Press, 1981, p. 64. Session 17.47 Compressed Gas Systems • Other energy conservation techniques (cont): Relocate air intakes to cooler positions* Air Intake Temp, °F Power Savings**, % 30 7.5 50 3.8 70 0 90 (3.8) 110 (7.6) *MD Oviatt and RK Miller, Industrial Pneumatic Systems, Fairmont Press, 1981, p. 49. ** Relative to 70ºF Session 17.48 Compressed Gas Systems • Other energy conservation techniques (cont): – Recover heat for personnel comfort from air compressor Heat recovered from air compressors* Compressor Size, Hp Heat Available, Btu/min 40 1870 100 4660 125 5830 150 6990 200 300 9330 14,000 400 18,700 *From Sullair screw compressor data Session 17.49 Compressed Gas • AIRMaster+ – Software tool sponsored by US Department of Energy – Estimates potential savings from selected energy efficiency measures and calculates paybacks • • • • • • • Reduce air leaks Improve use efficiency Reduce air pressure Use unloading controls Adjust set points Reduce operating time Add receiver volume Session 5.3.50 Compressed Gas • AIRMaster+ available for download from http://www1.eere.energy.gov/industry/bestpractices/software.html Session 5.3.51 Industrial Insulation Example • Consider the wall of a mild steel tank with these conditions based on measurements or observations at a plant – thickness = 0.5 inch – finish = dull metal – temperature of contents Th = 180 ºF – outside air temperature Tair = 80 ºF – air velocity = 0 (still air) Session 17.52 Industrial Insulation Example • Find these properties in tables • Rsurface = 0.46 h·ft2·°F/Btu (for dull metal) • Basic equation yields Th Tair ȈR q A (180 80) o F hr ft 2 o F 0.46 Btu 220 Btu hr ft 2 Session 17.53 Industrial Insulation Example • Add 1 inch of fiberglass insulation with a 3/32 inch shiny aluminum protective cover. • The resistance of the aluminum will be negligible, just as the resistance of the steel wall is negligible. However, the shiny surface affects the surface film coefficient • R for the fiberglass (at the correct mean temp): R insulation t k 1.0 inch Btu inch 0.33 hr ft 2 o F Session 17.54 hr ft 2 o C 3 Btu Industrial Insulation Example • Now Rinsulation= 3 hr·ft2·ºF/Btu Rsurface = 0.9 hr·ft2·ºF/Btu (for shiny aluminum where the surface temperature will now be near that of the surrounding air) • The basic equation yields q Th Tair ȈR (180 80) o F hr ft 2 o F (3.0 0.9) Btu 26 Btu hr ft 2 Session 17.55 Industrial Insulation Example • Savings = quninsulated-qinsulated = 194 Btu/hr·ft2 • If energy costs $8/million Btu, and the heat is supplied with an efficiency of 80%, what are the savings? The savings are $16.99/yr·ft2. Session 17.56 Boilers and Steam System Session 18.1 Temperature vs. Enthalpy Properties of Steam (@ 14.7 psia = 0.0 psig) Hf Latent Heat of Vaporization (Work) Hfg 350 Temperature (F) 300 1192.6 180 250 1150.9 200 150 Hg 100 100 50 50 0 0 0 200 400 600 800 Enthalpy (h) Session 18.2 1000 1200 1400 Boiler System Session 18.3 Firetube Boilers Session 18.4 Watertube Boilers Session 18.5 Boiler System Session 18.6 Balance Diagram Session 18.7 Boiler and Fired System Survey • Demand Analysis • Combustion Optimization • Waste Heat Recovery – – – – Condensate Return Blowdown Recouperator Economizer • Steam Traps Session 18.8 Combustion Analysis Session 18.9 Session 6.2.10 Boiler Efficiency Calculation • A check on the combustion system indicates a stack temperature rise of 700°F and an excess Oxygen level of 5.5%. What is the impact of trimming the excess Oxygen to 3%? % Savings NewEfficiency OldEfficiency NewEfficiency Session 18.11 Session 6.2.12 Boiler Efficiency Calculation • Result % Savings NewEfficiency OldEfficiency NewEfficiency % Savings 77 75 77 2.6% That means the fuel consumption will be reduced by 2.6% Now, If we add an Economizer to drop the stack temperature rise to 500°F, how much more can we reduce the fuel consumption? Session 18.13 Session 6.2.14 Boiler Efficiency Calculation • Result % Savings NewEfficiency OldEfficiency NewEfficiency % Savings 81 77 81 4.9% The fuel consumption will be further reduced by 4.9% Session 18.15 Waste Heat Recovery 1. Return more Condensate 2. Economizer preheats Make-up/Feed Water 3. Shell & Tube HX for Skimmer Blowdown 4. Recouperator preheats Combustion Air 5. Pressurize Condensate Return Tank 2 4 5 CR Tank 1 Feedwater Tank 3 Blowdown Session 18.16 Steam Traps – Inverted Bucket Session 18.17 Steam Traps – Float & Thermostatic Session 18.18 Steam Traps –Thermostatic Condensate Session 18.19 Steam Traps – Disc Session 18.20 Steam Steam Trap Maintenance • Purposes: – Reject Condensate – Reject Non-condensables (Air) – Hold Back Steam • A poorly maintained system has 20 – 30% of the traps failed open. • Maintenance Methods: – – – – Sight (watch the discharge) Sound (listen to the operation) Temperature (delta T across trap) Conductivity Session 18.21 Flash Steam Calculation • Condensate at steam pressure has too much heat to exist as saturated liquid at lower pressures, causing a portion of the liquid to “Flash” back to steam. % Flash H f steam Pr essure H f condensate Pr essure H fg condensate Pr essure Session 18.22 Flash Steam Calculation • 1000 lb/hr of blowdown at 60 psia is sent to an unpressurized tank. How much water is lost? % Flash % Flash H f 60 psia H f 14.7 psia H fg 14.7 psia 262.2btu / lb 180.2btu / lb 970.3btu / lb LostMass 0.0841000lb / hr 8.4% 84lb / hr Session 18.23 Flash Steam Calculation • If the tank is pressurized to 20 psia and the steam is recovered, how much can be produced? % Flash % Flash H f 60 psia H f 20 psia H fg 20 psia 262.2btu / lb 196.3btu / lb 960.1btu / lb LostMass 0.0691000lb / hr Session 18.24 6.9% 69lb / hr Steam Tables Session 18.25 Session 6.2.26 Session 6.2.27 Combined Heat and Power, Distributed Generation, and Renewable Energy Session 19.1 Distributed Generation Renewable Energy Combined Heat and Power Session 19.2 Combined Heat and Power • Also known as: – CHP – Cogeneration – Combined cooling, heating and power (CCHP) – Building cooling, heating and power (BCHP) • Definition: – Simultaneous production and use of useful mechanical and useful thermal energy – Mechanical energy is frequently used to turn a generator producing electrical energy – Thermal energy can be used to generate cooling (i.e., absorption chiller) Session 19.3 Why Cogeneration? • CHP has the opportunity to: – Improve system efficiency (as compared to typical power generation without useful heat recovery) – Reduce total operating costs (compared to purchasing or generating electricity and heat energy in separate systems) – Improve system reliability and availability (when CHP is used a primary and the utility systems are used as a back-up source) Session 19.4 CHP Energy Balance Source: EPA Combined Heat and Power Partnership (www.epa.gov/chp) Session 19.5 Types of Cycles • Three primary types of cycles: – Topping cycle – Bottoming cycle – Combined cycle (which is usually a dual topping cycle) • Why is the type of cycle important? – Regulations apply differently based on type of cycle Session 19.6 Topping Cycle • Primary energy first produces mechanical energy and residual thermal energy is recovered and used – Example 1: High-pressure boiler steam is used to power a turbine. The resulting shaft power turns a motor or generator. In addition, steam out of the turbine provides useful heat energy to a process. – Example 2: Diesel engine turns a generator producing electric power. Waste heat recovery is applied to the exhaust gas and engine coolant producing useful hot water. Session 19.7 Topping Cycle Example 1 Intermediate-Pressure Steam High-Pressure Steam Steam Turbine Generator Process/ Heating Very Low-Pressure Steam Steam Generator Condenser Low-Pressure Steam DA Feedwater Tank Condensate Return Make-Up Water Session 19.8 Topping Cycle Example 2 Return IC Engine Useful Heat Supply Radiator Engine Coolant Heat Recovery Generator Return Exhaust Gas Heat Recovery Exhaust Gas Useful Heat Supply Session 19.9 Bottoming Cycle • Primary energy first satisfies a thermal demand, such as a furnace, and residual thermal energy is recovered and used to produce useful mechanical or electrical power. – Example: A large combustion process, such as a heat treating furnace, where the exhaust is used in a waste heat boiler to develop steam that is used to power a turbine. The resulting shaft power turns a motor or generator. Session 19.10 Bottoming Cycle Example High-Pressure Steam Steam Turbine Process/ Heating Generator Very LowPressure Steam Steam Generator or Furnace Low-Pressure Steam Condenser Condensate Return DA Feedwater Tank Make-up Water Session 19.11 Combined Cycle • Cycle produces useful mechanical energy at two different stages within the process. Residual thermal energy is utilized at least once in the process. – Example: A combustion (gas) turbine creates shaft power, which powers a generator (a topping cycle). The exhaust gas (perhaps with supplemental firing) is used in a waste heat recovery boiler to develop steam, which is used to power a steam turbine. The shaft power from the turbine is used to power a motor or generator (normally a topping cycle but used here as a bottoming cycle). In addition, steam out of the turbine, either as extraction or back-pressure steam, provides useful heat energy to a process. (the useful thermal energy makes this CHP). Session 19.12 Combined Cycle Example Steam Turbine High-Pressure Steam Fuel Compressed Air Burner Exhaust Gases Generator Intermediate-Pressure Steam Waste heat Boiler Process/ Heating Generator Air Low Pressure Steam Gas Turbine Condensate Return DA Feedwater Tank Make-up Water Session 19.13 PURPA • Public Utility Regulatory Policy Act (PURPA) gave qualifying facilities (QF), for both CHP and small power producers (SPP), certain regulatory advantages if they met certain efficiency and ownership requirements. • Regulatory advantages granted – QFs and SPPs not regulated as a utility – Utility must buy excess electricity (at the utility’s avoided cost)—repealed with EPACT 2005 if access is available to competitive wholesale market. – Utility must provide back-up power (at a nondiscriminatory rate) )—repealed with EPACT 2005 if access if appropriate market access is available. Session 19.14 Other EPACT 2005 PURPA Changes • FERC is to establish new standards that prevent QFs from being built and operated as “PURPA machines.” • These new standards will require that the thermal and electric output be used fundamentally for industrial, commercial or institutional purposes; and not primarily for sale to electric utilities. Session 19.15 Intent of PURPA • Promote and support highly efficient systems (CHP) • Promote and support renewable energy systems (SPP) • People still argue advantages and limitations of PURPA Session 19.16 Sample Problem • A CHP facility consumes 81,900 Mcf/yr natural gas [Assume gas HHV is 1,050 Btu/ft3 and the cost is $10/Mcf] • The CHP generates 6,000,000 kWh/yr plus 300,000 therms/yr of useful heat energy. • Electricity generated offsets electricity that would be purchased at $0.08/kWh • Useful thermal energy recovered offsets a gas-fired boiler. Assume gas cost is the same as above and the net boiler efficiency is 80%. • Estimate the net reduction in annual energy cost delivered by the CHP. Solution to Sample Problem • CHP Gas Consumed = - (81,900 Mcf/yr)*($10/Mcf) = - $819,000/yr • Electricity Cost Offset =(+6,000,000 kWh/yr)*($0.08/kWh) =$480,000/yr • Boiler Gas Cost Offset =(+300,000 therm/yr)*(100,000 Btu/therm) *(1 ft3/1050 Btu)*(1 Mcf/1000 ft3)*($10/Mcf) /(.80) =$357,143/yr • Net Reduction in Energy Cost =(-$819,000/yr)+($480,000/yr)+($357,143/yr) =$18,143/yr Other Items • CHP is (typically) a type of DG • CHP can work well with – District heating systems – Thermal energy storage systems – Gas cooling systems • Energy security and surety issues are giving CHP and DG more justification Session 19.19 Distributed Generation • Also known as: – Distributed Generation (DG) – Distributed Energy (DE) – Distributed Energy Resources (DER), although DER can include more that DG (flywheels, batteries, etc.) – Self generation • Definition: (and there are several) – Any small-scale power generation that provides electric power at a site closer to the end user than central generation, and is usually interconnected to the distribution system or directly to the end user’s facility [Reference 2] – Any method of producing power that will be used on or near the site at which it is generated [Reference 5] Session 19.20 DG Technologies • Internal combustion engines – Fuel can include natural gas, diesel, biogas, gasoline, propane, and more – Available in sizes typically from 30 kW to 3,000 kW. Some systems are available as low as 1 kW for home energy systems, including CHP. – Efficiencies up to 37% electric, over 80% when heat recovery added – Basic equipment costs around $300 to $600/kW, without CHP • Combustion turbines – Fuels are typically gas (natural gas, biogas, etc.) but liquid systems are available – Most efficient systems are greater than 40 MW but systems as low as 500 kW are available Session 19.21 DG Technologies • Wind-Powered Generators – Large systems (600 kW and above) are becoming cost effective in select locations – Smaller systems (2 kW to 500 kW) are commercially available but more expensive – Wind is an intermittent source, so another power source is frequently required for a stable supply • Photovoltaics (PV) – Still very expensive but the cost continues to come down. Equipment around $10,000/kW today – PV is an intermediate source, so another power source (i.e., battery) is frequently required for a stable supply – Can be cost effective in remote locations Session 19.22 DG Technologies • Microturbines – Fuels are typically gas but liquid systems are being developed – Size range is limited because technology is still being developed. 30 kW, 60 kW, 70 kW and 250 kW systems are available – Electrical efficiency is low but emission levels are attractive • Fuel Cells – Fuel cells use a chemical reaction rather than a combustion process. They require hydrogen as a fuel source. – Fuel processors extract hydrogen from other fuels – Emission levels are excellent because of non combustion reaction – Technology is still developmental and very (very) expensive – Fuel processor, maintenance costs, and fuel cell stack life are current concerns Session 19.23 Renewable Energy • Definition: Energy that comes from a renewable source • What is a renewable energy source? • Renewable energy is energy from natural resources, which are naturally replenished in the short term, typically within a year or so. Session 19.24 Renewable Energy • The definition gets political – High-head hydro, which can disrupt stream flows and fish habitat, is frequently excluded from the definition. – Ground-source heat pumps, which consume conventional electric energy but can be more efficient because of heat sink/source temperatures, are frequently included. – Biomass, or the burning of agricultural products, increases local emissions, but is included because we assume the emissions (CO2 and mineral ash) support the growth of new agricultural products. Session 19.25 Renewable Energy-Electric • Photovoltaic (fixed or tracking) • Wind-power generators – Horizontal axis – Vertical axis • Hydropower – High-head – Low-head and “kinetic” hydropower • Ocean Energy – Surface wave or wave column – Tidal and current power Session 19.26 Renewable EnergyElectric or Thermal • Concentrating solar thermal – Tower or dish, usually tracking • Dish Stirling • Geothermal (usable heat from below ground) • Biomass and bagasse • Waste-to-energy • Landfill gas Session 19.27 Renewable-Thermal • Solar thermal panels • Concentrating solar thermal • Transpired solar collectors (solar air preheaters) • Thermal mass systems (Trombe wall) • Ocean energy – Thermal gradient – Ocean thermal energy conversion (OTEC) uses the temperature difference that exists between deep and shallow waters to run a heat engine Session 19.28 Net Metering • In general, the utility bills you for the “net” energy consumed. • This means that excess electricity generated is valued at the retail price, provided you are a net consumer of electricity (not a net generator). • Any excess energy you generate goes into the electric grid and creates a “credit” for future energy consumed. • “Net” may be defined as a billing period (monthly) or annually, depending on the utility. Session 19.29 Net Zero Energy • Several organizations have the goal of developing net zero energy buildings • Net zero energy buildings are highly efficient but still consume energy • Energy needs are met through self generation and interconnection to the utility grid and utilize net metering • “Net” zero is typically defined on an annual basis Session 19.30 Net Zero Energy • Efficiency is still “job one” • Reducing energy requirements through energy efficiency is generally less expensive than renewable energy • Make the building as efficient as possible until renewable energy resources become cost effective • General rule of thumb: 75% EE & 25% RE Session 19.31 Power-Purchase Agreements Popular for Renewable Energy • 3rd Party finances project installation • 3rd Party sells you the solar energy produced on your site (at a known price) for 15-25 years. – They like it because it will likely payback for them in 10 years or less. • You get “green” power and a known future energy cost (lower risk) Session 19.32 References 1. Kowlanowski, Bernard F. Small Scale Cogeneration Handbook, The Fairmont Press, Inc. Atlanta, GA, 2000. 2. McKinley, Sarah, “Untapped,” Energy Decisions, JanuaryFebruary 2000, pages 34-38. 3. Parks, William, et al. Reliable and Economic Natural Gas Distributed Generation Technologies, US Department of Energy, Washington DC. 4. Petursson, Gestur, Reducing Operating Costs Through On-Site Generation of Electricity, Working Paper, Oklahoma Industrial Assessment Center, Oklahoma State University, Stillwater, OK. 5. Sturdevant, Nicole, “Getting On Track with On-Site Power,” Building Operating Management, July 2000, pages 79-88. 6. Wong, Jorge B. and Kovacik, John M., “Cogeneration,” Energy Management Handbook (Chapter 12), 5th edition, The Fairmont Press, Inc., Atlanta, GA. References 7. Landreth, Michael, “On-Site Power Generation: Items to Consider,” Proceedings Strategic Energy Forum, May 18, 2000. 8. Blazewicz, Stan and Walker, Stow, “Distributed Generation: What Will it Take to Deliver Grid Reliability?” Power Value, July-August 2000, page 12. 9. Gas Research Institute, “Natural Gas-Fueled Reciprocating Engines; Fastest-growing Prime Movers for Distributed Generation,” Natural Gas Application in Industry, GRI. 10. US Department of Energy-Federal Energy Management Program, “Using Distributed Energy Resources—A How-to Guide for Federal Energy Managers,” Cogeneration and Competitive Power Journal, Vol. 17, No. 4, The Fairmont Press, Atlanta, GA, Fall 2002, pages 37-68. Summary Table of Typical Cost and Performance Characteristics by CHP Technology1 Steam Turbine2 Recip. Engine Gas Turbine Microturbine Fuel Cell Power efficiency (HHV) 15-38% 22-40% 22-36% 18-27% 30-63% Overall efficiency (HHV) 80% 70-80% 70-75% 65-75% 55-80% Effective electrical efficiency 75% 70-80% 50-70% 50-70% 55-80% Typical capacity (MWe) 0.5-250 0..01-5 0.5-250 0.03-0.25 0.005-2 Typical power to heat ratio 0.1-0.3 0.5-1 0.5-2 0.4-0.7 1-2 ok ok poor ok good 430-1,100 1,100-2,200 970-1,300 (5-40 MW) 2,400-3,000 5,000-6,500 0.032-0.038 Technology Part-load CHP Installed costs ($/kWe) O&M costs ($/kWhe) Availability Hours to overhauls Start-up time <0.005 0.009-0.022 0.004-0.011 0.012-0.025 near 100% 92-97% 90-98% 90-98% >95% >50,000 25,000-50,000 25,000-50,000 20,000-40,000 32,000-64,000 1 hr - 1 day 10 sec 10 min - 1 hr 60 sec 3 hrs - 2 days Fuel pressure (psig) n/a 1-45 100-500 (compressor) 50-80 (compressor) 0.5-45 Fuels all natural gas, biogas, propane, landfill gas natural gas, biogas, propane, oil natural gas, biogas, propane, oil hydrogen, natural gas, propane, methanol Noise Uses for thermal output Power Density (kW/m2) high High Moderate moderate low LP-HP steam hot water, LP steam heat, hot water, LPHP steam heat, hot water, LP steam hot water, LP-HP steam >100 35-50 20-500 5-70 5-20 NOx ( lb/MMBtu) (not including SCR) Gas 0.1-.2 Wood 0.2-.5 Coal 0.3-1.2 0.013 rich burn 3-way cat. 0.17 lean burn 0.036-0.05 0.015-0.036 0.0025-.0040 lb/MWhTotalOutput (not including SCR) Gas 0.4-0.8 Wood 0.9-1.4 Coal 1.2-5.0. 0.06 rich burn 3-way cat. 0.8 lean burn 0.17-0.25 0.08-0.20 0.011-0.016 1. Data are illustrative values for typically available systems. All costs are in 2007 dollars. 2. For steam turbine, not the entire boiler package. Source: Catalog of CHP Technologies, EPA, 2008. 35 Performance Comparisons Technology Size Range (kW) Installed Cost ($/kW) (2) Heat Rate (Btu/kWhe) Approx. Efficiency (%) Variable O&M ($/kWh) Diesel Engine 1-10,000 350-800 7,800 45 0.025 0.017 1.7 Natural Gas Engine 1-5,000 450-1,100 9,700 35 0.025 0.0059 0.97 Natural Gas Engine w/CHP (3) 1-5,000 575-1,225 9,700 35 0.027 0.0059 0.97 Dual-Fuel Engine 1-10,000 625-1,000 9,200 37 0.023 0.01 1.2 15-60 950-1,700 12,200 28 0.014 0.00049 1.19 Microturbine Microturbine w/CHP (3) Emissions (1) (lb/kWh) NOx CO2 15-60 1,100-1,850 12,200 28 0.014 0.00049 1.19 Combustion Turbine 300-10,000 550-1,700 11,000 31 0.024 0.0012 1.15 Combustion Turbine w/CHP (3) 300-10,000 700-2,100 11,000 31 0.024 0.0012 1.15 100-250 5,500++ 6,850 50 0.01-0.05 0.000015 0.85 Photovoltaic 0.01-8 8,000-13,000 -- N/A 0.002 0.0 0.0 Wind Turbine 0.2-5,000 1,000-3,000 -- N/A 0.010 0.0 0.0 Battery 1-1,000 1,100-1,300 -- 70 0.010 (4) (4) Flywheel 2-1,600 400 -- 70 0.004 (4) (4) SMES 750-5,000 600 -- 70 0.02 (4) (4) Hybrid System 1-10,000 (6) (5) (5) (5) (5) (5) Fuel Cell (1) Nationwide utility averages for emissions from generating plants are 0.0035 lb/kWh of NOx and 1.32 lb/kWh of CO2. (2) The high end of the range indicates costs with NOx controls for the most severe emissions limits (internal combustion technologies only). (3) Although the electric conversion efficiency of the prime mover does not change much, CHP significantly improves the fuel utilization efficiency of a DER system. (4) Storage devices have virtually no emissions at the point of use. However, the emissions associated with the production of the stored energy will be those from the generation source. (5) Same as generation technology selected. (6) Add cost of component technologies. SOURCE; DOE-FEMP. Reference 10 Comparison of DG Technologies Comparison Factor Diesel Engine Gas Engine Simple Cycle Gas Turbine Microturbine Fuel Cell Photovoltaic Product Availability Commercial Commercial Commercial 1999-2005 1996-2010 Commercial Size Range (kW/unit) 20 to 10,000+ 50 to 5,000+ 1,000 to 30,000 20 to 200 50 to 1000+ 1+ 200 to 2,000 300 to 3,000 1,000 to 10,000 20 to 100 50 to 200 1 to 5 Efficiency (HHV) 36 to 43% 28 to 42% 21 to 40% 25 to 30% 35 to 54% n.a. Genset Package Cost ($/kW) 125 to 300 250 to 600 300 to 600 300 to 600 1,500 to 3,000 n.a. Turnkey CostWith no heat recovery ($/kW) 350 to 500 600 to 1,000 650 to 900 650 to 900 1,900 to 3,500 5,000 to 10,000 Heat Recovery Added Cost ($/kW) 100 to 200 75 to 150 100 to 200 75 to 350 Included n.a. 0015 to 0.010 0.007 to 0.015 0.003 to 0.008 0.005 to 0.010 0.005 to 0.010 0.001 to 0.004 Typical DG Range (kW/unit) O&M Cost ($/kWh) Source: Gas Research Institute (2000) Comparison of CHP Technologies