wpcawpca.info/pdf/newsletters/2009_wpca_news_issue_15.pdf · mist and solid particulate materi-al...

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Background Mercury, present in only trace amounts in coal, is released during the coal combustion process, and can appear in several forms in the flue gas. In the solid phase, it is referred to as particulate mercury, and in the gaseous phase it is referred to as vapor-phase mer- cury. Due to the high volatility of mercury and many of its compounds, most of the mercury produced by coal combustion is found in the gas phase. Vapor- phase mercury from coal-fired power plants is consid- ered a hazardous air pollutant by the EPA. Regula- tions are in place in many states and are being reworked at the Federal level to regulate gaseous mer- cury emissions. The concentration of mercury in the coal is primarily dependant on the coal type. Bitumi- nous and lignite coals have the highest concentration of mercury, while subbituminous coal contains less. The form of mercury present in the flue gas (oxidized or elemental), commonly referred to as speciation, is a key factor in the development of emissions control strategies. Continued on page 14 WPCA NEWS A Bi-Annual Newsletter Sponsored by the WPCA ISSUE 15 - 2009 www.wpca.info Introduction When the U.S. Environmental Protection Agency (EPA) originally developed Reference Methods for measuring emissions from stationary sources in the early to mid 1970’s, emission levels were much higher than they are today – sometimes by an order of magnitude or more. These Reference Methods may have been acceptable for these higher emission levels, but today, many of these methods are proving problematic or even inade- quate for accurate determination of low-level emissions. Inherent biases in these methods that were insignifi- cant when measuring emissions of 1000 ppm become unacceptable when measuring at 10 ppm. Even more important, state and local regulatory agencies are driv- ing emission limits ever lower through permit limita- tions. In some cases, these regulatory limits are set lower than the capability of the Reference Method to accurately measure them; that is, they are set below the detection limit of the method. What is a Detection Limit? While this may seem at first a simple question, the concept of detection limit is one of the most controver- sial in analytical chemistry. It has undergone much change over the past 40 years and is still an unsettled issue. Debates on this topic at analytical chemistry conferences are passionate with two or more sides each vigorously defending their point of view. Until recently, the subject of detection limits was rarely considered in the field of air emissions testing. Most Reference Methods specify detec- tion or “sensitivity” limits and not much was thought about them. However, over the past few years, the drive to lower NOx emissions and to an even greater extent, SO 3 emissions, has fueled an intense interest in air measurement detection limits. Vendors of air pollution control equipment, in particu- lar, are struggling how best to insure they can meet performance guarantees for emission concentrations in the sub-ppm range. Continued on page 12 WORLDWIDE POLLUTION CONTROL ASSOCIATION Mercury capture: Not as easy as 1,2,3 Cost Effective Integrated Approach to Mercury Removal By Albert L. Moretti, John L. David, Ashley N. Krout, and Tim G. Ruppelli, The Babcock & Wilcox Power Generation Group, Inc. Don’t overlook the indiscernable Dealing with Non-Detects in Air Emissions Testing (Part 1) By Scott Evans, Clean Air Engineering Inside Acid Mist Formation . . . . . . . . . . . . . . . . . . . . . . . . . . . .page 2 Impact of High Frequency TRs on ESP Performance . .page 3 Cliffside 6 Integrated Emissions Control System . . . . .page 5 Help - I’ve Been Blinded! . . . . . . . . . . . . . . . . . . . . . . .page 18 Figure 1: Example of Blank Probability Distribution Function -20 -15 -10 -5 0 5 10 15 20

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Page 1: WPCAwpca.info/pdf/Newsletters/2009_WPCA_News_Issue_15.pdf · mist and solid particulate materi-al from the flue gas. Wet electrostatic precipitation (WESP) ... neering design concurrently

BackgroundMercury, present in only trace amounts in coal, isreleased during the coal combustion process, and canappear in several forms in the flue gas. In the solidphase, it is referred to as particulate mercury, and inthe gaseous phase it is referred to as vapor-phase mer-cury. Due to the high volatility of mercury and manyof its compounds, most of the mercury produced bycoal combustion is found in the gas phase. Vapor-phase mercury from coal-fired power plants is consid-ered a hazardous air pollutant by the EPA. Regula-tions are in place in many states and are beingreworked at the Federal level to regulate gaseous mer-cury emissions. The concentration of mercury in the

coal is primarily dependant on the coal type. Bitumi-nous and lignite coals have the highest concentrationof mercury, while subbituminous coal contains less.The form of mercury present in the flue gas (oxidizedor elemental), commonly referred to as speciation, isa key factor in the development of emissions controlstrategies. Continued on page 14

WPCANEWSA Bi-Annual Newsletter Sponsored by the WPCA ISSUE 15 - 2009

www.wpca.info

IntroductionWhen the U.S. Environmental Protection Agency(EPA) originally developed Reference Methods formeasuring emissions from stationary sources in theearly to mid 1970’s, emission levelswere much higher than they aretoday – sometimes by an order ofmagnitude or more. These ReferenceMethods may have been acceptablefor these higher emission levels, buttoday, many of these methods areproving problematic or even inade-quate for accurate determination oflow-level emissions. Inherent biasesin these methods that were insignifi-cant when measuring emissions of 1000 ppm becomeunacceptable when measuring at 10 ppm. Even moreimportant, state and local regulatory agencies are driv-ing emission limits ever lower through permit limita-tions. In some cases, these regulatory limits are setlower than the capability of the Reference Method toaccurately measure them; that is, they are set belowthe detection limit of the method.

What is a Detection Limit? While this may seem at first a simple question, theconcept of detection limit is one of the most controver-sial in analytical chemistry. It has undergone much

change over the past 40 years and isstill an unsettled issue. Debates onthis topic at analytical chemistryconferences are passionate with twoor more sides each vigorouslydefending their point of view. Untilrecently, the subject of detectionlimits was rarely considered in thefield of air emissions testing. MostReference Methods specify detec-tion or “sensitivity” limits and not

much was thought about them. However, over the pastfew years, the drive to lower NOx emissions and to aneven greater extent, SO3 emissions, has fueled anintense interest in air measurement detection limits.Vendors of air pollution control equipment, in particu-lar, are struggling how best to insure they can meetperformance guarantees for emission concentrations inthe sub-ppm range. Continued on page 12

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Mercury capture: Not as easy as 1,2,3Cost Effective Integrated Approach to Mercury Removal

By Albert L. Moretti, John L. David, Ashley N. Krout, and Tim G. Ruppelli,The Babcock & Wilcox Power Generation Group, Inc.

Don’t overlook the indiscernable

Dealing with Non-Detects in Air Emissions Testing (Part 1)By Scott Evans, Clean Air Engineering

InsideAcid Mist Formation . . . . . . . . . . . . . . . . . . . . . . . . . . . .page 2Impact of High Frequency TRs on ESP Performance . .page 3 Cliffside 6 Integrated Emissions Control System . . . . .page 5Help - I’ve Been Blinded! . . . . . . . . . . . . . . . . . . . . . . .page 18

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Figure 1: Example of Blank Probability Distribution Function

-20 -15 -10 -5 0 5 10 15 20

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Depending upon the type of FGD technology installed, aconsiderable portion of ammonia salts and sulfuric acidmay exit the stack as respirable sub-micron fine particleemissions.Sulfur trioxide (SO3), when hydrated with moisture in thegas stream or in the atmosphere, forms sulfuric acid(H2SO4), which contributes to visible plume and may vio-late local opacity regulations. Control of sulfuric acid mistpresents an extremely difficult air pollution control prob-lem due to its uniform 0.3-0.5 sub-micron size.

Sulfuric acid emissions are problematic in both wet anddry FGD processesIn wet processes, where the flue gas leaving the absorberis saturated with moisture, sulfuric acid mist formsinstantly after the flue gas is saturated and creates a stackopacity problem. Dry processes, where the flue gas is notsaturated with moisture, typically remove fine particlessuch as (NH4)2SO4. However, dry processes typicallyhave lower removal efficiency for SO3 vapors. Upon exitfrom the stack, these vapors convert to sulfuric acid mistand produce significant visible emissions.

Sulfuric acid formation takes place through the oxida-tion of SO2 to SO3, followed by reaction with H2O toform H2SO4.

During the combustion process, the sulfur in the fossil fuelreacts to form about 95-97 percent sulfur dioxide (SO2)and the remainder sulfur trioxide (SO3). Most of the SO3in boiler flue gas likely forms during the several secondswhen the combustion gas cools from 2900-3100° F toabout 1830° F. SCR technologies will generate an addi-tonal quantity of SO3 through catalytic conversion of SO2to SO3 even at low temperatures.

There are two primary mechanisms for sulfuric acidmist formation.The first mechanism is the reac-tion between H2O vapors and SO3vapors that form liquid droplets.The second mechanism is sulfuricacid vapor condensation in thebulk gas phase when the gasstream temperature is loweredbelow the H2SO4 dew point.While an FGD system willremove some H2SO4, the majoritywill exit the stack.

If reductions of mass emissions,stack opacity, or both arerequired, it is necessary to use atechnology that will simultane-ously remove both sulfuric acidmist and solid particulate materi-al from the flue gas. Wet electrostatic precipitation(WESP) technology can satisfy

this requirement and has the added potential for abatementof heavy metals (including mercury), as well as water mistcarryover from an FGD scrubber system.

Future PM2.5 and Regional Haze regulations willrequire control of SO3 and sub-micron particulate. Any plant planning to install an FGD system for SO2 con-trol should consider leaving room for the future additionof a WESP (Figure 2) and performing preliminary engi-neering design concurrently with the FGD to minimizefuture outage time and cost. þ

For more information, contact Wayne Buckley, Siemens,at [email protected]; or James “Buzz” Reynolds, Siemens, at [email protected]

Is there a simple solution?Acid Mist Formation

By Wayne Buckley & James “Buzz” Reynolds, Siemens Environmental Systems & Services

Figure 2: New Coal Fired APC System with WESP

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Is what you see, what you get?Application Calculations on the Impact of High Frequency T-Rs

on Electrostatic Precipitator Performanceby Robert Mastropietro / Clive Cottingham / K. S. Park, Lodge-Cottrell / KC Cottrell

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SummaryElectrostatic precipitator (ESP) mathematical models canbe used to calculate the ESP size increase that wouldcause an equivalent performance enhancement to thatobserved by adding high frequency transformer-rectifiers(T-Rs). This information can be used to predict perform-ance enhancements on existing ESPs when adding highfrequency T-Rs.

DiscussionIn recent years, many papers have been presented bytransformer-rectifier manufacturers that show perform-ance enhancements caused by adding high frequency T-Rs. Typically these opacity based performance demon-strations take the form show on Figure 3.

The best performance enhancements reported in these“sales oriented” papers show opacities to be cut in half(i.e. approximately, the ESP is making an additional 50%collection of outlet particulate). Let’s suppose for calcu-lation of the upper end of our ESP enhancement rangethat this performance enhance-ment was solely due to the highfrequency T-Rs. What does anadditional 50 % collectionmean in terms of ESP sizing?This can be calculated using themodified Deutsch equation;

y Efficiency = 1 – e-(A/V*wk)

As shown on Figure 4 , the col-lection efficiency of an ESPdrops from inlet to outlet fields

due to particle size effects. Also, collection efficiency ofthe outlet field of the ESP approaches 50%. This isapproximately the same collection efficiency as the mostoptimistic claims for high frequency T-Rs.

Note that the outlet field of this ESP comprises 20% ofthe total ESP treatment time. If high frequency T-Rs trulyreduced particulate emissions by about one half, this

would correspond to arequired ESP sizedecrease of 20% (i.e.since the outlet fieldof the ESP reducesemissions by one-half). However, theobservations of per-formance improve-ment levels are notsolely caused by theuse of high frequencywaveforms alone.

Sales people tend to only publish the best cases. Theytend to avoid mention of less successful improvements inperformance. They also fail to mention that when ESPsare refurbished, there are a number of other improve-ments that occur. Some examples would be;

4 Electrodes cleaned by rapping and thermal effects.4 Electrodes realigned and broken electrodes taken

out.4 Insulators cleaned and broken insulators replaced.4 Replace weighted wires with rigid

mast type designs.

Figure 3: Opacity Based Performance Demonstrations

Figure 4: ESP Performance Calculations as Predicted by the Modified Deutsch Equation with 0.6 Exponent

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4 Collecting plates that “ring” betterwith rapping.

4 Adding rappers to reduce electrodebuildup & reentrainment.

4 Adding T-Rs reduces % of surfaceaffected by each spark.

4 Gas flow modifications and hopperbaffling.

4 High frequency T-Rs maximize power/minimizesparking.

So very often, other factors serve to reduce opacity incombination with the change to high frequency T-Rs.Therefore, a conservative approach to our upper boundfor performance enhancement on ESP size, solely fromthe T-R change alone, must be reduced from the opti-mistic 20% value.

Additionally, the concept of performance enhancementfrom adding high frequency T-Rs results from the capa-bility to get more power into the ESP. It is a well knownfact in the ESP industry that the collection efficiency ofESPs behave as follows in Figure 5.

So for high frequency T-Rs to make the ESP benefit fromhigher power, the ESP should have low power before theaddition. If the ESP has high power already, adding highfrequency T-Rs would have very little effect. Note thatthis gives us a lower bound on our range of enhancementsnear 0%. This also means that one should assume greaterenhancements if the ESP is electrically sick, than if it iselectrically healthy.

Conclusion1. If the ESP has properly designed electrode geometryand is getting high power levels with conventional 60 HzT-Rs, then the ESP size enhancement from changing tohigh frequency T-Rs should be estimated in the 0-10%range.

2. If the ESP has poorpower levels, and the onlychange being made to theESP is changing from con-ventional to high frequencyT-Rs, then the ESP sizeenhancement should be esti-mated in the 5-10% range.3. If the ESP has poorpower levels, and the ESP isbeing refurbished at thesame time that the T-Rs areconverted to high frequency,then the ESP size enhance-ment should be estimated inthe 10-20% range.

Sample CalculationsHow are these conclusionsuseful? Suppose, for exam-ple, that an existing ESP had

10 seconds of treatment time and conventional T-Rs. ESPsizing models are then used to analyze the coal and ashchemistry and these indicate that the minimum treatmenttime (with conventional T-Rs) to get the required outletparticulate emission is say, 18 seconds. This informationtells you that changing the T-Rs to high frequency is notgoing to get you where you need to be. This is becauseat best, enhancements in ESP performance would make a10 second treatment time ESP work like a 10 x 1.2 = 12second treatment time ESP (i.e., 20 % enhancement if theESP is electrically sick, we add high frequency T-Rs, andrefurbish the ESP). It would only be possible to get theperformance you need if your models indicate requiredtreatment times in the range of 12 seconds.

In simple terms, adding high frequency T-Rs and refur-bishment is making the ESPs act like they have one morefield. Simply adding high frequency T-Rs without refur-bishment is making the ESPs act like they have anotherhalf field. þ

For more information, contact Bob Mastropietro,Lodge-Cottrell, at [email protected];

Clive Cottingham, Lodge-Cottrell, at [email protected]; or K. S. Park, at Lodge-Cottrell, [email protected]

Figure 5: Typical ESP Power vs. Performance

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With approval of the final air permit in January 2008,Duke Energy has begun construction of a new nominal800 MW unit as part of an overall modernization of theirexisting Cliffside, NC facility. This paper will focus on theadvanced Integrated Emissions Control System (IECS)that will be supplied by Alstom. The IECS combinesAlstom’s dry and wet flue gas desulfurization systems inan innovative way. In the IECS process, sulfuric acid mist,hydrogen chloride, mercury, and particulate are removedby the DFGD stage with SO2 and additional HCl and mer-cury removal occurring in the downstream WFGD. TheWFGD purge stream is sent to the DFGD where it is spraydried and collected in the fabric filter thus avoiding theneed for wastewater treatment and discharge.

Major cost savings are achieved by employing the spraydryer in place of a wet electrostatic precipitator to controlacid mist emissions. Further savings are accomplished byeliminating the need for wastewater treatment equipmentfor the WFGD system. Other advantages of the IECSprocess include improved fuel flexibility, reduced waterconsumption, and the ability to employ low cost materialsfor construction for the WFGD absorber. This article willdescribe the IECS process planned for Cliffside as well aspresent a lifecycle cost analysis comparing Alstom’s IECSto conventional technologies.

IntroductionIn response to the anticipated base electrical load growthand the need for clean energy solutions, Duke Energy isconstructing a new nominal 800 MW unit as part of anoverall modernization of their existing Cliffside, NC facil-ity. The complete project involves the retirement of four1940s vintage units, the addition of a WFGD system onUnit 5, and the construction of a new super-critical coal-fired generating facility (Unit 6). Unit 6 is currently underconstruction and expected to be in commercial service in2012.

Like all new generating facilities, Cliffside Unit 6 is subjectto strict emission limits for sulfur dioxide (SO2), sulfuricacid mist, mercury, and total and filterable particulate. Inaddition, effective control of other acid gases, includingHCl and HF, is an important consideration from both anenvironmental standpoint as well as impacts on equipmentoperation and maintenance. After extensive review, Dukedetermined that the Integrated AQCS was the most cost-effective approach to meet all these limts for Cliffside.

System DesignAlstom’s Integrated Air Quality Control System (IAQCS)combines two proven technologies – dry (DFGD) and wet(WFGD) flue gas desulfurization systems – in an innova-tive way that reliably achieves stringent emission require-ments at a lifecycle cost well below that of competingtechnologies. In the integrated process, sulfuric acid mist,hydrogen chloride, mercury, and particulate are removedby the DFGD stage, with SO2 and additional mercury andHCl removal occurring in the downstream WFGD. TheWFGD purge stream is sent to the DFGD, where it isspray dried and collected in the fabric filter, thus avoidingthe need for wastewater treatment and discharge.

Process DescriptionThe principal process steps are as follows:

¶ The flue gas is cooled in the Spray Dryer Absorber(SDA) using a lean, lime slurry (see Figure 6). Since theSDA outlet temperature is well below the acid dew point,the SO3 in the flue gas condenses as sulfuric acid (H2SO4)mist. The sulfuric acid mist reacts with the lime slurry andis captured in the fabric filter (FF) as calcium sulfate.Experience with DFGD systems and recent pilot testinghas shown that sulfuric acid mist emissions are expectedto be less than 1 ppm (~0.004 lb/MBtu).

· Significant mercury capture also occurs in the DFGD.Depending on the fuel and boiler/SCR design, more than85-90% mercury capture is expected in the DFGD stage.¸ Significant HCl and HF capture occurs in SDA. TheHCl and HF react with lime to form dry solids (i.e. calci-um chloride and fluoride), which are removed in the FF.

Page 5Spring 2009

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WPCA News

It’s not old hat!Cliffside 6 Integrated Emissions Control System

By D. Gregory McGinnis, Duke Energy; Philip C. Rader and Raymond R. Gansley, Alstom Power Inc.;and Wuyin Wang, Alstom Power Sweden AB

Figure 6: Integrated AQCS PFD

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WPCA News

¹ Sulfur dioxide (SO2) capture in the DFGD stage is min-imized by temperature control and sub-stoichiometricreagent feed in order to minimize lime usage. The smallamount of SO2 that is captured reacts to form a mixture ofcalcium sulfite and sulfate which is removed as a dry solidin the FF. º SO2 removal is accomplished in a conventional mannerin the WFGD stage with low-cost limestone. Wallboardquality or landfill gypsum is produced. Alstom’s provenopen spray tower technology is capable of achieving>99% SO2 removal.» Additional HCl, HF, and oxidized mercury removaloccurs in the spray tower as well.¼ The purge stream that is required to control chloridesand inert fines for wallboard gypsum production isreturned as a component of the lime slurry feed to theDFGD stage where it is spray dried in the SDA. Dissolvedand suspended solids in the purge stream are captured inthe FF and removed as dry solids with the ash. ½ No wastewater treatment system is required to treat thepurge stream from the WFGD dewatering system. In addi-tion to the capital cost savings, the operating costs associ-ated with this equipment (i.e. energy costs, treatmentchemicals, maintenance, etc.) are avoided.

System BenefitsThe main features and benefits of the IAQCS process arediscussed below.

Sulfuric Acid Control Using Proven DFGD TechnologyLike other specifications for new high-sulfur coal-firedunits, the Cliffside specifications initially called for analloy WESP (Wet Electrostatic Precipitator) as the meansof controlling sulfuric acid emissions. In the IAQCSprocess, total particulate and sulfuric acid mist concentra-tions are reduced to the required permit levels through theuse of DFGD technology consisting of a rotary atomizerSpray Dry Absorber (SDA) and fabric filter. Benefits ofdoing so include:

R Lower material costs by employing carbon steelSDA in place of an alloy WESP

R Lower construction costs due to simple SDA design(compared to WESP) and reduction in amount ofalloy field welding

R Reduced exposure to alloy price volatilityR Improved O&M cost predictability with DFGD vs.

WESP

Fuel Flexibility and Lower Cost Alloy Construction forthe WFGDAs a substantial quantity of the incoming HCl is removedby the DFGD stage, chloride levels in the WFGD absorber

can easily be controlled to low levels (<12,000 ppm). Thisallows the use of lower grade stainless steel, resulting incapital cost and operating cost savings. The Cliffside proj-ect original fuel specification had fuel sulfur levels up to5.0 lbs SO2/MMBtu and up to 1,300-ppm chloride in the

fuel. During further development of the project, it wasdecided to include fuel chloride levels up to 3,000-ppm toallow added flexibility of fuel sourcing. The integratedAQCS design was readily able to address the higher chlo-ride condition by increasing the lime addition to the

DFGD area for more HCl removal and increasing theWFGD purge rate sent to the DFGD area for evaporation.Because additional HCl could be removed in the DFGDarea, the WFGD absorber operating chloride design levelwas maintained at 12,000-ppm, even at the highest fuelchloride condition. Thus, the material choice for theabsorber remained alloy 2205 instead of a more expensivealloy needed for higher operating chloride designs.

No FGD Waste Water Treatment SystemAs noted above, a purge stream is required to control chlo-ride and inert fines contamination in WFGD gypsum.NPDES limits on dissolved/suspended solids, heavy met-als, and other constituents typically require that the purgestream be treated in multi-stage processing facilities toreduce suspended solids, heavy metals, and organic com-

Figure 8: Make-up Water Savings

Figure 7: Cliffside 6 Integrated AQCS

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pounds. By evaporating the purge stream in the SDA,the IAQCS process eliminates the significant capitaland operating costs associated with purge streamtreatment. An added benefit is that the plant ownerdoes not have to permit, monitor, and report on thepurge stream discharge. See Figure 7 on page 6.

For Cliffside, a wastewater treatment system, alongwith the ongoing operating and maintenance costs,is not required for the Unit 6 AQCS. Because theUnit 5 WFGD system needs to operate independ-ently of Unit 6, a wastewater treatment system(WWTS) is planned for Unit 5. However, when Unit 6 isoperating, most or all of the Unit 5 purge can be accommo-dated in the Unit 6 SDA, thus reducing or eliminating theO&M costs associated with the Unit 5 WWTS.

Reduced Make-up Water Consumption Traditional WFGD systems remove nearly all of the HCl inthe flue gas into the absorber slurry and generate a waste-water purge stream to maintain the dissolved chloride levelwithin the design limit for the selected materials of con-struction and control gypsum quality. Eliminating the needfor a wastewater purge stream results in a reduction inmake-up water consumption for the integrated AQCSdesign. This is significant make-up water savings/waste-water elimination, particularly as the fuel chloride levelincreases, is seen in Figure 8 on page 6. Additional waterconservation measures on the project are being included toallow use of cooling tower blowdown (CTB) or a blend ofCTB with river water as make-up water to both the Unit 5and Unit 6 AQCS systems.

Mercury Capture CapabilityBased on the fuel chloride levels and the presence of anSCR, a high degree of mercury oxidation is expected atCliffside. Based on testing, high levels of oxidation areconducive to mercury capture in both wet and dry FGD sys-tems.1 Since the integrated AQCS design includes DFGDand WFGD systems in series,the majority of the mercurywill be expected to beremoved in the DFGD area,which includes a fabric filter,and the WFGD absorber isexpected to act more as a pol-ishing stage for oxidizedmercury that is not capturedby the DFGD. Since only asmall portion of the totalmercury removed is project-ed in the WFGD, the potential for mercury re-emissionfrom the WFGD is reasoned to be low relative to a design

where the WFGD removes the majority of the mercury. Themercury content in the gypsum is also expected to be lowerthan in a conventional WFGD-only system.

Potential Fly Ash ResaleSince a lean feed of lime slurry is used in the DFGD areato remove sulfuric acid and a portion of the HCl, theimpact on the ash composition is small as compared to aconventional DFGD application. There is also a smallcontribution of solids, mainly gypsum solids from theWFGD purge stream that is added to the ash. For the Cliff-side performance basis fuel (17.96 wt.% ash, 3.55 lbsSO2/MMBtu, 531 ppm Cl in fuel), the total addition ofsolids to the fly ash collected is expected to be less than5%. The impact on ash composition increases for highflue gas sulfuric acid and HCl levels and for lower fuel flyash content.

Analysis of representative ash samples from the pilotplant study by a firm that re-sells power plant ash to the

Figure 9: Cliffside Design Fuel Range

Figure 10: Flue Gas Design Conditions

Figure 11: Emission Requirements

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cement industry has been completed. Noproblematic issues for cement use were iden-tified with the pilot samples. Chemical com-position and mix testing provided positiveresults. It is expected that final determinationof suitability for cement use will not bedetermined until actual plant operation, andit will then depend on the characteristics(sulfur, chloride and ash levels) of the fuelsburned due to the wide range of fuels speci-fied.

Specific Details for Clifffside Unit 6Design RequirementsDuke Energy’s new Cliffside Unit 6 willinclude a pulverized coal-fired supercriticalboiler equipped with selective catalytic NOxreduction (SCR). The plant is located nearCliffside, North Carolina at an existingpower plant site. The plant is nominally sizedat 800 MW and is permitted to fire up to 7,850 MMBtu/hr.

The design of the AQCS considers a wide range of fuelsincluding both eastern bituminous and western sub-bitu-minous coals. Design includes fuel blends with sulfur lev-els up to 5.0 lbs SO2 per MMBtu, and chloride levels up to3,000 ppm on a weight basis. Figure 9 on page 7 presentsdesign ranges for the fuel blends. Design conditions for theflue gas leaving the air heaters and entering the AQCSscope are shown in Figure 10 on page 7. In Figure 11 onpage 7, system emission requirements are stringent to meetpermit requirements for this new coal-fired power plant.

Flue Gas PathThe flue gas leaves the two air heater out-lets (by others) and is combined into acommon duct that rises vertically to theinlet of two 50% Spray Dryer Absorbers(SDA). Separate gas paths are maintainedthrough the fabric filters.

Gas leaves the fabric filter to the two axialflow ID fans. The gas is combined in acommon duct and enters the single OpenSpray Tower (OST) absorber. A new two-flue stack will serve both Units 5 and 6.

Common SystemsThe WFGD portion of the Unit 6 AQCSshares common equipment with the newWFGD system for the existing CliffsideUnit 5. The limestone preparation system

has two (one operating and oneredundant) horizontal ball mills,each rated at 48 tph. Redundantreagent slurry storage tanks, pumpsand feed loops to both absorbers areincluded. Hydrocyclones are usedfor the primary dewatering step withthe underflow collected in filter feedtanks (two provided). Two horizon-tal belt filters are provided to pro-duce wallboard-quality gypsum.

DFGD AreaTwo 68 ft diameter SDAs are pro-vided to intimately contact the fluegas with the lime reagent, and par-tially quench the flue gas whileevaporating the purge flow from theWFGD system. The capacity of theSDAs to evaporate water not only

allows for all of the purge from Unit 6 to be evaporated,but also allows for the complete WFGD purge stream fromUnit 5 to be evaporated in the SDAs under most scenarioswhen Unit 6 is operating. The SDA is a standard Alstomdesign employing three top-entry gas inlets per vessel,each equipped with a rotary atomizer.

The lime preparation system includes three detention typeslakers. Each slaker is sized for 50% of the maximumdemand condition. Since the plant had a wide range inlime demand due largely to the wide range in fuel chloride

level (up to 3000 ppm Cl in fuel), thechoice of 50% slakers allows for theoperation of one slaker only under lowerchloride operating scenarios and avoidsturndown issues on the slaker for theseconditions.

Slaked lime slurry is combined with thepurge from the WFGD absorbers in apre-mix tank. (See Figure 12.) The pre-mix tank overflows to an SDA feed tank,which provides suction to an SDA feedpump that delivers the slurry to the atom-izers. Any additional make-up waterneeded to quench the flue gas is added tothese tanks. A redundant set of tanks,feed pump and feed line to the SDAs isincluded for reliability.

The fabric filter is Alstom’s LKP inter-mediate pressure, pulse jet design. Twocasings are provided, each with 12 com-

Figure 12: Spray Tower Absorber

Figure 13: Rotary Atomizer

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partments with a3.6-ft/min net-1air-to-cloth ratio.The bags are 26.5ft. long of a blend-ed PPS/P84 mate-rial with an intrin-sic coating.

WFGD AreaThe spray towerabsorber is de-signed for 99%SO2 removal overthe range of fuelsulfur levels. SeeFigure 13 on page8. The absorber is Alloy 2205 construction designed forcontinuous operation with dissolved chloride levels of upto 12,000 ppm. The design includes five normally operat-ing spray levels for the maximum sulfur condition, witheach spray levelfed by a singleslurry pump. Theabsorber is de-signed for up to13 ft/sec saturatedflue gas velocity.The reaction tankdiameter is ex-panded relative tothe absorptionsection to allowfor adequate gyp-sum residencetime. Absorberdesign featuresinclude dual ori-fice spray nozzleson the bottomfour spray levelswith a highdegree of sprayoverlap and wall ring technology. An organic acid additivesystem is included (shared with Unit 5 absorber); its in-tended use is to maintain SO2 removal in the event of anunplanned spray pump outage.

Lifecycle Cost AnalysisThe principle quantitative benefit of the Integrated AirQuality Control System is a savings in lifecycle costs. Thefollowing paragraphs present a lifecycle cost comparisonof the IAQCS to conventional solutions as follows:

Integrated AQCSAlstom Integrated AQCS as described in this paper (spraydryer, fabric filter, spray tower absorber).

FF/WFGD/WESPFabric filter with WFGD system followed by WESP forSO3/total particulate control.

Alk Inj/FF/WFGDDry alkali injection (MgO) for SO3 control followed byfabric filter and WFGD system. (Note that this configura-tion is included for illustrative purposes only as alkaliinjection has not been proven to consistently achieve themodern SO3 permit limits for Cliffside.)

Figure15: Operating Cost Inputs

Figure 14: Lifecycle Cost Inputs (5)

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MethodologyThe capital and operating costs were compared by com-bining the sum of the present day capital cost and the dis-counted value of future operating costs over the period ofconcern. The Net Present Value (NPV) method is com-monly used in the engineering project business to com-pare the economic merits and viability of alternative sce-narios in which expenditures are made and the economicimpact is felt over a period of time. In this method, theannual O&M costs were calculated based on the plant/unitcapacity factor and AQCS system operating performance(e.g. power consumption, reagent consumption, etc.). Thelong-term impact of each O&M cost component was eval-uated using the net present value method.

The NPV of a series of future payments is defined as:where, NPV = Net Present Value of future payments, $

n = Number of equally-spaced paymentsP = Value of individual payment, $R = Discount rate, %

The Net Present Value can be thought of as the amount ofmoney that, if in the possession of the owner at the begin-ning of the lifecycle and used to pay for future operatingexpenses, would be exhausted at the end of the period.The time-value of money is incorporated in the analysisby assuming a certain discount rate. The sum of the capi-tal cost and the NPV of the O&M costs is a reasonablerepresentation of the total lifecycle cost.

Capital Cost Figure 14 on page 9 presents the capital costs and finan-cial assumptions used to calculate the lifecycle costs. The

Total Plant Capital Costs are indicative estimates for aplant like Cliffside. The capital costs include the majorprocess equipment (i.e. absorbers, fabric filters, WESP,reagent handling/feed systems, byproduct handling sys-tems, etc.), balance of plant (i.e. foundations, electrical,plant services, etc.), construction, and commissioning.

Operating and Maintenance CostsThe following O&M costs were considered in the analysis:

Ü Power – The power consumed by both the AQCS sys-tem and ID fans is considered and are shown separately.Power consumption was calculated by summing the indi-vidual electrical loads for the major components.

Ü Reagent – The following reagents are considered in thelifecycle cost analysis:

© Limestone – Used in all cases for removal of SO2 andother acid gases (e.g. HCl, HF).

© Lime – Used in the Integrated AQCS to react withSO3 and other acid gases (e.g. HCl, HF).

© Magnesium hydroxide – Used in the FF/WFGD/ WESP to neutralize the SO3 collected in the WESPand in the Alk Inj/FF/WFGD for SO3 control.

© WWTS (Waste Water Treatment) chemicals – Usedin the FF/WFGD/WESP and Alk Inj/FF/WFGDcases to treat the WFGD purge stream. These chemi-cals are used to remove heavy metals and suspended solids prior to discharge.

Ü Byproduct – The revenue from gypsum sale was con-sidered. Ash disposal/sales were not considered in thisanalysis as the costs/revenues are considered to be equiv-alent for all cases.

Figure 16: Lifestyle Cost Comparison

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Quantities and unit costs/credits for major O&M items areindicated in Figure 15 on page 9.

Lifecycle Cost ComparisonFigure 16 on page 10 indicates the annual O&M costs andlifecycle cost for the Conventional and Integrated AQCSoptions.

Based on the analysis in Figure 16, the Integrated AQCSapproach is clearly preferred. Contributing factorsinclude:

Ü The use of relatively low-cost lime reagent for SO3 inthe Integrated AQCS control results in a substantial oper-ating cost savings compared the use of MgO in theFF/WFGD/WESP and Alk Inj/FF/WFGD cases.

Ü Eliminating the need for WWTS (Waste Water Treat-ment System) chemicals in the Integrated AQCS results ina $1.3 M per year O&M cost savings.

Ü The AQCS capital costs for the Integrated AQCS aresignificantly less than the FF/WFGD/WESP approach dueto:

© Material cost savings due to the elimination of theWWTS

© Material cost saving associated with replacing theWESP with a spray dryer

© Corresponding lower erection costs

Ü Although the capital cost of the Integrated AQCS isslightly higher than the Alk Inj/FF/WFGD approach, theoperating costs are lower, making the IAQCS the betterchoice on an overall lifecycle cost basis. Also, the IAQCScan reliably achieve the proposed permit limits for sulfu-ric acid mist emissions.

Pilot Plant TestingAlthough the Cliffside Integrated AQCS is based onproven dry and wet FGD technologies, pilot plant testingwas conducted to:

R Establish the removal efficiencies/limits of SO3 andHCl

R Confirm the drying properties of scrubber bleed liquidR Perform parametric studies related to stoichiometric

ratio, temperature, and bleed flowR Examine the impact of trace pollutants R Collect/analyze ash samples

Pilot testing of the DFGD stage was performed on a ~1 MWequivalent slipstream at Cliffside Unit 5. The pilot plantconsisted of a dual-fluid nozzle spray drying and fabric

filter, along with related auxiliary equipment (e.g. ducts,fans, lime slurry and scrubber purge feed systems, etc.).Purge liquor was collected from the existing WFGD sys-tem at Duke Energy’s Marshall Steam Station and trans-ported to Cliffside for testing. Provisions were made tospike the Unit 5 slipstream with SO2, SO3, and HCl tosimulate the range of Unit 6 operating conditions. See fig-ure 17.

Pilot plant testing at Cliffside confirmed:R Low SO3 emissions (<<1 ppm)R Selective removal of HCl in the presence of SO2R Lime stoichiometric ratio requirementsR Effective drying of WFGD purge stream

Ash/byproduct samples were collected and submitted foranalysis and testing for use in cement. Initial testing indi-cated that the byproduct was within the required specifi-cations for cement manufacture. þ

REFERENCES:1) J. E. Locke, Withum, J. A., Tseng, S. C., CONSOLEnergy, “Mercury Emission from Coal-Fired Facilitieswith SCR-FGD Systems,” Proceedings of Air Quality VConference, Sept. 2005.

For more information, contact D. Gregory McGinnis, Duke Energy,at [email protected]; Philip Rader, Alstom Power,at [email protected]; Raymond Gansley, Alstom Power,at [email protected]; or Wuyin Wang, Alstom Power Sweden AB, [email protected]

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Figure 17: IAQCS Pilot Plant

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Conceptually, the detection limit is simply the minimumamount or concentration of a substance that must be pres-ent for a measurement process (MP) to distinguish it fromthe background. However, any specific numerical valuerepresenting a detection limit, say 2 ppm, is not absolute.It is the result of several factors any one of which, ifaltered, will change the number. Some of the most impor-tant ones are:

6 The risk of a false positive (deciding the substance ispresent, when it is not)

6 The risk of a false negative (deciding the substance is not present, when it is)

6 The matrix in which the substance is contained6 The skill and experience of the person taking the meas-

urement.6 The current state of maintenance and calibration of the

measuring equipment.6 Sampling error.

This last factor is of particular importance to air emissionstesting and one we shall discuss in more detail below.

It’s important to remember that the output of any meas-urement process is not a number but a range, more pre-cisely a distribution. If, for example, measurements aretaken when the substance is not present, one would hopethat the MP output is close to zero. But it will rarely beexactly zero. A good MP will output tightly bunched data,both positive and negative values, centered at the zeropoint. These data can then be used to define a curve thatrepresents expected data scatter (see Figure 1 on frontcover). For measurements taken in the absence of the sub-stance of interest, this curve is usually the familiar normaldistribution. This distribution represents the backgroundagainst which the MP must distinguish the signal from thesubstance of interest must be discerned.

This measurement, the matrix without the substance ofinterest present, is the blank and it is fundamental to thedetermination of the detection limit. The better the distri-bution of the blank measurement is known, the more con-fidence one has in the determination of the detection limit.This is discussed in more detail below.

What constitutes a blank for air emissions testing is worthdiscussing for a moment. In a perfect world, a blankwould be composed of the entire matrix in which the sub-

stance of interest will be measured, but with the substanceitself absent. Even in a laboratory setting, this is often dif-ficult or impossible to achieve. For air emissions testing,it’s almost always impossible. Because of this, detectionlimits for reference methods are often based on preparedlaboratory standards or zero gases. This approach doesnot take into account potential matrix effects and interfer-ence.

A more fundamental issue is that these detection limits arederived solely from the analytical portion of the method.This is the most serious flaw in the determination ofdetection limits for air reference methods. The vast major-ity of variation in air reference methods does not occur inthe analytical portion of the method, but rather in the sam-pling portion. Typically, sampling and matrix effects arecompletely ignored when detection limits are determinedduring method validation. This results in detection limitsthat are far lower than what is actually achieved in thefield.

This can be a major problem for affected sources usingthe method. Permit writers may use these unrealisticallylow limits to set emission standards for the source. Airpollution control vendors may also rely on these detectionlimits when establishing performance guarantees. Prob-lems are then encountered when compliance or guaranteetests are performed which cannot produce reliable data atthese low levels.

One example of this is EPA Method 8 “Determination OfSulfuric Acid and Sulfur Dioxide Emissions from Station-ary Sources.” While there are a number of problems withthis method, the focus here will be only on the detectionlimit issue. The detection limit (referred to as “sensitivity”in the method) listed in the method is 0.05 mg/m3 orabout 0.01 ppm. After some research (Evans 2007) intothe validation of this method, it was determined that thislimit was based upon the sensitivity of the analytical tech-nique, in this case, titration.

To check whether this limit was realistic in the field, testswere conducted (Evans 2007) to determine the trueMethod Detection Limit (MDL) of Method 8. The MDLencompasses the entire measurement process includingsampling uncertainty and matrix effects. The resultsshowed that the MDL, under controlled conditions, wasno better than 0.2 ppm - an order of magnitude higher than

Dealing with Non-Detects in Air Emissions Testing (Part 1)

continued from front page

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Figure 16: Alloy ALRD

stated in the method. In the field, this number is most like-ly even higher. Further field studies are on-going.

Determining Realistic Method Detection Limitsfor Air MethodsThe MDL is fundamentally related to the variability of theMP output at or near zero. The problem comes with deter-mining that variability in a manner that encompasses theentire method including sampling uncertainty and matrixeffects. The best way to accomplish this would be in fieldsampling an actual source. The question, of course, isunder these circumstances, how do you obtain a blank?

EPA has already addressed this issue, although not in thecontext of detection limits, with its Method 301 “FieldValidation of Pollutant Measurement Methods from Vari-ous Waste Media.” This method is used to demonstrate theequivalence of unvalidated test methods to validated refer-ence methods. In this method, paired sampling trains (orquadruplet sampling trains) are used to determine methodvariability. Although the words “detection limit” are notfound in Method 301, the same approach can be used todetermine MDLs.

By comparing the variability in the differences betweenpaired sampling trains, the precision of the method isdetermined. This is all that is required to determine thedetection limit. However, since any matrix effects shouldbe the same for both sampling trains, these would not betaken into account. Dynamic spiking can be used to deter-mine any biases caused by matrix effects, although thedetails of this are a topic for another paper. This key pointhere is that both sampling uncertainty and matrix effectscan be determined from this method.

There are a couple of considerations when using the “dif-ferences” approach. First, it is not uncommon for theabsolute variability of a method to increase proportionate-ly with concentration (although the relative variability willusually stay the same). This phenomenon is referred to as“heteroscedasticity.” Therefore, when determining MDLwith this technique, sampling should be performed whenthe amount of the substance of interest is very low, i.e.after a control device. An interesting study might be tocompare method variability at the inlet and outlet of a con-trol device.

Another issue is that of potential bias between the pairedtrains. Since the sampling trains employ the same methodand sample at or near the same point, the distribution ofthe differences should be centered around zero. If this dis-tribution is significantly shifted, this indicates a problemwith one of the sampling trains causing a bias. If this is

seen, it must be identified and corrected.

A minimum of seven valid paired runs should be used indetermining the MDL. Of course, a larger number pro-vides better results. Once this is done, the standard devia-tion can be calculated and an appropriate upper confi-dence level (e.g. 95%, 99%) can be determined. The cal-culations for this are left to the reader and are readilyavailable. This value is then equivalent to Currie’s CriticalLevel (LC) (Currie 1968 and IUPAC 2005) or EPA’s Limitof Detection (LOD) (EPA 2007). þ

In Part 2 of this paper, which will appear in the Fall Issueof the WPCA Newsletter, we will discuss how to reportdata that is below the detection limit.

REFERENCESCurrie, L. A., “Limits for qualitative detection and quan-

titative determination—application to radiochemistry”, Ana-lytical Chemistry, 1968, 40(3), 586.

Currie, L. A. (Ed.), Detection in Analytical Chemistry:Importance, Theory, and Practice, ACS Symposium Series,vol. 361, American Chemical Society, Washington, DC,1988

Environmental Protection Agency, “Emission Measure-ment Technical Information Center Guideline Document 038 -- Description of In-Stack Detection Limit”, 1992

Environmental Protection Agency, “Revised Assess-ment of Detection and Quantitation Approaches”, EPA-821-B-04-005, Washington, DC, 2004

Environmental Protection Agency, “Report of the Feder-al Advisory Committee on Detection and QuantitationApproaches and Uses in Clean Water Act Programs”, Wash-ington, DC, 2007

Evans, S., Aita, K., O’Halloren, K., and Chi, E., “AStudy of the Precision and Detection Limits of USEPAMethod 8 at Low SO3 Concentrations”, Clean Air Engineer-ing White Paper, Palatine, IL, 2007.

Helsel, D. R., Nondetects and Data Analysis: Statisticsfor Censored Environmental Data; Wiley: New York, 2005.

Helsel, D.R., “Fabricating Data: How Substituting Val-ues For Nondetects Can Ruin Results, And What Can BeDone About It”, Chemosphere (65), 2434–2439, 2005

Travis, C., “Estimating The Mean of Data Sets WithNondetectable Values”, Environmental Science and Technol-ogy, (24)7, 1990

Analytical Methods Committee of the Royal Society ofChemistry, “Measurement of near zero concentration:recording and reporting results that fall close to or below thedetection limit”, The Analyst, (126) 256-259, 2001

For more information, contact Scott Evans, Clean AirEngineering, at [email protected]

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Vapor-phase mercury, appearing in coal combustion fluegas, will be present as either elemental mercury or oxi-dized mercury, with proportions largely dependent on thetype of coal being burned. It has been recognized byindustry experts that a loose empirical positive relation-ship holds between the chloride content of coal and theextent to which its inherent mercury becomes oxidized.Therefore, a higher percentage of oxidized mercury isproduced from high-sulfur, high-chloride coal, such aseastern U.S. bituminous coals. For low-sulfur, low-chlo-ride coal, such as subbituminous and lignite, a higher per-centage of elemental mercury is produced. Capturing oxi-dized mercury is easier than capturing elemental mercury.

Environmental equipment alreadyinstalled at some electric generating plantscan remove a portion of vapor-phase mer-cury, both elemental and oxidized. Forexample, the SCR catalyst in place for NOxremoval aids in the oxidation of the elementalmercury when in the presence of a halogensuch as chlorine or bromine. Then, due tooxidized mercury’s water solubility, oxidizedmercury is dissolved and readily removed bywet and dry FGD scrubbers during the SO2removal process. While somewhat effective,simply relying on environmental equipmentalready in place may not be adequate to meetcurrent or pending mercury emissions limitsset by the regulatory agencies.

Following is a discussion of general mer-cury technology including how it works,when and where it is used, a system overview, limitations,and potential economic savings.

Use of Powdered Activated Carbon (PAC) forRemoving HgSorbent technology is the most proven method presentlyemployed for total mercury control. Sorbents are particu-late matter injected into the flue gas that provide foradsorption of chemical species from the flue gas. Ofthese, powdered activated carbon (PAC) is the most estab-lished technology for mercury control, and can provide upto 90% mercury capture for coals with high chorine con-tent. By adsorbing onto the surface of the PAC, the ele-mental mercury converts into oxidized mercury and par-ticulate mercury, which may be subsequently removed inparticulate control devices (ESP or fabric filter). Chemi-

cal modification of the PAC, such as halogenation, canimprove the ability of the sorbent to capture mercury, butcan also increase material costs. Though 90% total mer-cury removal for PRB coal is unlikely using standardPAC, the increased reactivity provided by halogenatedPAC makes this target more realistic. Due to the relativeconcentrations of mercury in the flue gas as compared toother reactive species, the amount of sorbent needed toachieve a target removal rate is not determined by calcu-lations based on the amount of mercury in the flue gas.While such relations may be developed eventually, empir-ical correlations based on field data are currently used toguide estimation of injection rates.

As mentioned, PAC is the mostwidely used sorbent for mercurycontrol in the utility industry. PAC

is carbon that has been treated with high tem-perature steam using a proprietary

process to create large surfaceareas. Figure 18, at left,

presents a diagram of aPAC particle. Each PACparticle consists of a car-

bon skeleton with numerousbranching pores that providea very high ratio of surfacearea to volume. One gram of

PAC will have a surface area of500-1500 m2 (5 grams of carbon is

approximately equivalent to the area of onefootball field). Pollutants, such as mercury,

become adsorbed in the nanopores of the PAC particles,and are effectively sequestered from the flue gas stream.The sorbent activity varies with respect to each chemicalspecies, with oxidized mercury having a greater rate ofadsorption by PAC than elemental mercury. Sorbent reac-tivity with respect to a given chemical species is deter-mined by testing the sorbent with that species. Further,the reaction kinetics of PAC are temperature dependent.Standard PAC is only effective for mercury control at fluegas temperatures below about 330oF for bituminous coaland about 350oF for PRB coal. Therefore, total mercuryremoval of over 90% may be attained for bituminous coalusing standard PAC when an SCR is part of the air pollu-tion control system, but only about 60% removal could beexpected for untreated PRB coal using standard PACinjection. However, over 90% total mercury removalwhen burning subbitumuous coal has been achieved using

Cost Effective Integrated Approach to Mercury Removal continued from front page

Figure 18: Powdered Activated CarbonParticle[1].

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halogenated PAC. See Figure 19.

A typical PAC injection system consists of the following:A storage silo, as shown in Figure 20, is used for on-sitePAC storage. Air fluidization valves and nozzles at theconical discharge pulse instrument quality dry com-pressed air into the bulk carbon to promote mass flow.From the storage silo, the PAC is conveyed to a volumet-ric feed hopper for temporary storage. Screw feeders thentransport the carbon into a drop tube, from which it is fedto the eductor inlet, below the feeder discharge. The car-bon-in-air mixture is metered into the flue gas ductworkwith an array of injection lances.

As discussed above, by halogenating the PAC, sorbentaffinity for mercury capture may be increased. Therefore,lower sorbent injection rates are required to achieve thesame mercury capture. Halogenated PAC is purchasedfrom suppliers, who use proprietary methods to impreg-nate the carbon with the halogen species. In addition, thehalogenation process alters the PAC properties such thathalogenated sorbents may be effective at flue gas temper-atures up to 400°F, while standard PAC decreases in use-fulness as flue gas temperatures exceed 350°F when burn-ing PRB coal. Brominated PAC is the most commonlysold carbon for Hg control, since bromine is far morereactive than chlorine. Unlike standard PAC, injection ofbrominated PAC alone may provide adequate mercuryremoval rates for many plants to meet pending State andFederal Regulations. As an example, for a cold-side ESPand a pulse-jet fabric filter (PJFF), total mercury removalswould be anticipated to improve from baseline rates of

10-30% and 30-50% to 50-70% and 70-90%, respective-ly, with brominated PAC injection.

Another unique challenge is PAC poisoning bySO3. When burning medium to high sulfurcoal, SO2 to SO3 conversion (up to 2%) occursin the boiler and across the SCR system. PACconsumption increases as SO3 concentrationincreases above 5 ppm. At greater than 15ppm, the PAC is much less effective in remov-ing mercury. To mitigate this SO3 impact, sor-bent injection systems utilizing lime or tronathat remove SO3 before the point of PAC injec-tion can be installed.

Mercury Removal Optimization Using aCoal Additive - MercPlus™As mentioned earlier, there exists a looseempirical positive relationship between thechloride content of coal and the extent to whichits inherent mercury becomes oxidized. Coalswith less than 100 ppmw of chlorine (Cl) havemore elemental mercury at the inlet of their

respective environmental control equipment while coalswith greater than 500 ppmw Cl have less than 20 percentelemental mercury.

Figure 19: Mercury Removal as a Function of Sorbent Injection forVarious Coal Types across a FF or ESP[2] .

FIgure 20: PAC Injection Silo [3].

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WPCA News

The chlorine content of bituminous coals varies from sev-eral hundred to several thousand ppmw. Conversely, thechlorine content of low-rank coals has a much lower anda more narrow range: from 5 to 200 ppmw. In both cases,chlorine compounds in the flue gas decrease the amount

of gaseous elemental mercury presentat the inlet to pollution control equip-ment and increase the amount of oxi-dized mercury there. Figure 21 illus-trates the impact of chloride on the spe-ciation of mercury.

One way to improve the overall captureof mercury in the system would be toincrease the fraction of mercuryappearing in oxidized form. Byincreasing the chloride content of thecoal this goal can be achieved. As anadded benefit of chloride addition, thequantity of activated carbon consumedto meet mercury emissions limits canbe considerably reduced. B&W PGG’sMercPlus™ additive works in tandemwith standard or brominated PAC toenhance the PAC adsorption capabili-ties. Typically, standard PAC is onlyused if there is an SCR system.

The equipment needed to implement a MercPlus™ addi-tive injection system is a storage tank and a self containedpump skid which injects the MercPlus™ additive solu-tion into the coal feeders through a single feed line foreach coal feeder. The initial equipment investment is

FIgure 21: Impact of Chloride Addition on Mercury Speciation.

FIgure 22: Cost Savings example using MercPlusTM additive with an AQCS consisting of SCR/SDA/FF or SCR/FF.

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minimal when compared to the potential long term dollarsavings realized in the reduced usage of activated carbon.Figure 22 on page 16 gives an example of estimated sav-ings in carbon consumption in a plant burning a PRB coaland using a brominated PAC.

The proposed addition of chlorides to the coal to enhancemercury oxidation can raise potential concerns about theimpacts of the added chlorides on boiler materials andoperation, and on the downstream equipment. The targetchloride content for most applications is less than 500ppm which does not exceed the chloride concentration ofbituminous coals that have been successfully fired formany years at eastern U.S. utility plants.

Use of a WFGD Additive to Inhibit Mercury Re-emission - Absorption Plus (Hg) TM

Since oxidized mercury is soluble in water, wet flue gasdesulfurization (WFGD) units have been useful as mercu-ry control systems. In a wet scrubber, the mercury isexposed to a complex environment of gas/liquid/solidphase electrolytic chemistry. The oxidized mercury willrapidly dissolve into the WFGD slurry, but some oxidizedmercury may react with dissolved constituents to be sub-sequently reduced to elemental mercury and then re-emit-ted in the vaporous, elemental form. While the exactcause of elemental Hg re-emission is being evaluated, thefollowing parameters are important: temperature, mer-curic sulfite complexes, pH, soluble chloride and the typeof solid present. B&W PGG is currently offering theAbsorption Plus (Hg)TM system as a patented technologyfor controlling re-emission of elemental mercury fromWFGD units. See Figure 23. The Absorption Plus (Hg)TM

system is readily utilized with B&WPGG’s proprietary Absorption Plus(Hg)TM additive, thereby providing anoptimal environment to react with thedissolved oxidized mercury and form aninsoluble chemical species that is subse-quently precipitated and removed fromthe WFGD.

ConclusionsThe control of mercury emissions pres-ents several unique challenges. Variablessuch as mercury speciation, mercury re-emission, and SO2 to SO3 conversion willall have an impact on the chosen mercuryreduction solution depending upon thefuel being fired and the emissions controlequipment installed at the plant.

When selecting a mercury control system,a multi-faceted approach that includes

many variables such as the air quality control system,fuel, flue gas composition, fly ash characteristics, stackmercury limits, and many other operational factors shouldbe evaluated. In conclusion, an integrated approach tomercury removal can lead to the best mix of cost andeffectiveness. þ

REFERENCES[1] Jankura, Bryan. “Wygen 1 2006 Mercury Control Project: Back-ground, Equipment and Test Results.” The Babcock & Wilcox Com-pany, 5 April 2007.[2] C. Jean Bustard, et al., ADA-ES, US DOE, Southern Co., HamonResearch-Cottrell, EPRI.[3] David, John. “B&W’s Mercury Control Program.” The Babcock& Wilcox Company, December 2006.

Copyright© 2009 Babcock & Wilcox Power Generation Group,Inc., a Babcock & Wilcox company

All rights reserved.No part of this work may be published, translated or reproduced inany form or by any means, or incorporated into any informationretrieval system, without the written permission of the copyrightholder. Permission requests should be addressed to: MarketingCommunications, Babcock & Wilcox Power Generation Group,Inc., P.O. Box 351, Barberton, Ohio, U.S.A. 44203-0351.

For more information, contact the following atBabcock & Wilcox Power Generation Group, Inc:Albert L. Moretti at [email protected],John L. David at [email protected],Ashley N. Krout at [email protected], orTim G. Ruppelli at [email protected]

Figure 23 - The use of the Absorption Plus (Hg)TM system is designed to inhibit mercury re-emission and remove nearly all of the oxidized mercury in a Wet FGD system.

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Your FGD system has been running along normallywhen suddenly

ä The limestone feed valve is completely openä The pH is staying the sameä The SO2 removal efficiency is dropping

What has happened and what should you do?

These are the classic symptoms of limestone blinding. Ifyou are lucky, it will be a temporary phenomenon cause byan excess of dissolved sulfites in the slurry precipitatingonto the surface of the limestone particles blocking thelimestone dissolution.

If you have a forced oxidation system, check the air flowto the absorber. A low air flow can cause an excess of sul-fites since there is not enough oxygen to convert all ofthem to sulfates. Once the air flow returns to normal, thesulfites will dissolve from the limestone surface and theabsorber performance will return to normal.

Another mode for limestone blinding is if the absorbertower has been at low load for several days. Then if theload returns to normal rather quickly, the sudden increasein SO2 can form an excess of dissolved sulfites. The bestway to recover from this is to shut off the limestone feed.The pH will remain the same for some period of time.Once the pH begins to fall, return the limestone feed valveto normal control and the system will return to normaloperation.

The other possibility is permanent blinding if largeamounts of fly ash have entered the absorber tower. Thealuminum in the fly ash reacts with the fluoride in the slur-ry to coat the surface of the limestone particles with alu-minum fluoride. The only cure for this is to flush out thesystem and start with fresh slurry. þ

For more information, contact Ron Richard,RE Consulting, at [email protected]

Is it temporary or permanent?Help! – I’ve Been Blinded!

By Ron Richard, RE Consulting

The WPCA Presents Two Seminars

Dry Scrubber Trainingand

Particulate Training

Sunday, July 12, 1–4 p.m., at the 2009 APC/PCUG Conference

The Woodlands Resort, The Woodlands, TX

Don’t miss out on this unique opportunity to learn all about O&M of dry scrubbersand particulate control equipment.

The two Training Seminars will be held simulateneously in adjacent rooms.Choose the one that suits you best and sign up on-line at www.reinholdenvironmental.com

by selecting the “Register On-line” link on the home page.

These seminars are free of charge to all registered attendees of the 2009 APC/PCUG Conference. For complete details, go to www.reinholdenvironmental.com

and scroll down to conference info on the home page. The particulars of both seminars will be posted as soon as they become available.

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The Worldwide Pollution Control Association (WPCA) is a non-profit organization.It is comprised of a group of internationally diverse individuals and companies whoare experts in various aspects of air pollution control. WPCA members and advisorsare motivated by a desire to improve pollution control through better technical communication.Today, the WPCA is accomplishing this goal via its newsletters,seminars, a website and an expanding worldwide membership.

What is the WPCA?

The WPCA is a partnership which includes system/equipment/services suppliers,consultants and users. The WPCA President, Vice President and Advisory Commit-tee are equipment users. The Corporate Sponsors and Board of Directors are suppli-ers. Together they develop annual seminars and events to achieve their goal of bettertechnical communication for users of air pollution control systems.

Who Directs the WPCA?

In order to be a WPCA member, you must be an end user of air pollution controlequipment. When you register on-line for any WPCA sponsored seminar, you auto-matically become a member. If you would like to join, but cannot attend a seminar atthis time, please download and send in the Registration Form at the top of the members list at www.wpca.info. You will then be emailed regarding upcoming eventsand sent future copies of the WPCA News.

How do I become a Member of the WPCA?

Your membership in the WPCA includes sponsored seminars that are presented several times each year around the U.S. and the globe. As a member, you can attendthese informative seminars and have access to the most up-to-dateinformation on air pollution control from leading industry experts.

Your membership also includes a semi-annual free emailed copy of the WPCA newsletter. The “WPCA News” is a technical newsletter that includes current topics ofinterest written by corporate sponsors and members of the utility advisory committee.

What are the Benefits of Joining the WPCA?

Page 20: WPCAwpca.info/pdf/Newsletters/2009_WPCA_News_Issue_15.pdf · mist and solid particulate materi-al from the flue gas. Wet electrostatic precipitation (WESP) ... neering design concurrently

WPCA NewsPage 20

WPCA News

©2009 Reinhold Environmental Ltd.

is a bi-annual newsletter sponsored

by and for the

Worldwide Pollution Control Association

www.wpca.info

Purpose:To foster new ideas and greaterawareness concerning pollution control in the energy industry

Publisher:Reinhold Environmental Ltd.

Graphic Design Editor:Nadine D. Burge

Comments & OtherInquiries to:

Reinhold Environmental Ltd.3850 Bordeaux Drive

Northbrook, IL 60062 USA1.847.291.7396

[email protected]

Welcome

Terry Farmer

as the new

GE Energy

Corporate

Sponsor

WPCA Corporate Sponsors

Airflow Sciences Corp.Robert G. Mudry, P.E.12190 Hubbard Street Livonia, MI 48150 Phone: +1.734.525.0300 Fax: +1.734.525.0303Email: [email protected]: www.airflowsciences.com

Alstom Environmental Control Systems Philip Rader1409 Centerpoint Blvd. Knoxville, TN 37932Phone: +1.865-694-5233 Fax: +1.865-694-5213Email: [email protected]: www.environment.power.alstom.com

The Babcock & Wilcox Power Generation Group, IncGreg Bielawski20 S. Van Buren Ave. Barberton, OH 44203 Phone: +1.330.860.1591 Fax: +1.330.860.9901Email: [email protected] Website: www.babcock.com

Babcock Power Environmental, Inc.Tony Licata5 Neponset Street Worcester, MA 01606 Phone: +1.508.854.3853 Fax: +1.508.854.3800Email: [email protected]: www.babcockpower.com

Buell APC, Fisher-KlostermanThomas Lugar200 North Seventh Street, Suite 2 Lebanon, PA 17046 Phone: +1.717.274.7110 Fax: +1.717.274.7342Email: [email protected]: www.buellapc.com

CleanAir EngineeringAllen Kephart1601 Parkway View Drive Pittsburgh, PA 15205 Phone: +1.412.787.9130 Fax: +1.412.787.9138Email: [email protected] Website: www.cleanair.com

E.ON Engineering Corp.Peter Struckmann4001 Bixby Road Groveport, OH43125Phone: +1.614.830.0817 Fax: +1.614.830.0816Email: [email protected]

Evonik Energy Services LLCMarilynn Martin304 Linwood Rd., Suite 102, Kings Mountain, NC 28086Phone: +1.704.734.0688 Fax: +1.704.734.1088Email: [email protected]: www.evonik-energyservices.us

GEA Process Engineering A/S Niels JacobsenGladsaxevej 305, Soeborg, Denmark DK-2860Phone: +45.3954.5432 Fax: +45.3954.5871Email: [email protected] Website: www.niro.com

GE EnergyTerry Farmer8800 East 63rd. Street Kansas City, MO 64133 Phone: +1.816.356.8400 Fax: +1.816.353.1873Email: [email protected]: www.gepower.com/airquality

Haldor TopsoeNathan White5510 Morris Hunt Drive Fort Mill, SC 29708Phone: +1.803.835.0571 Fax: +1.281.228.5129Email: [email protected] Website: www.topsoe.com

Johnson Matthey Catalysts LLC Cindy Khalaf5895 Shiloh Road Suite 101 Alpharetta, GA 30005Phone: +1.678-341-7520 Fax: +1.678-341-7509Email: [email protected]: www.jmcatalysts.com

KC Cottrell Co., Ltd.Tae Young Lee160-1 Dongkyo-dong, Mapo-gu, Seoul, Korea 121-817Phone: +82-2-3206-103 Fax: +82-2-3206-100Email: [email protected]: www.kc-cottrell.com

Marsulex Environmental TechnologiesRichard Staehle3737 Embassy Parkway, Suite 260 Fairlawn, OH 44333 Phone: +1.360.668.6202 Fax: +1.360.664.0983Email: [email protected]: www.marsulex.com

Redkoh IndustriesPaul Ford300 Valley Road Hillsborough NJ. 08844 Phone: +1.908.369.1590 Fax: +1.908.369-1594Email: [email protected]: www.redkoh.com

Reinhold Environmental Ltd.Susan Reinhold3850 Bordeaux Dr. Northbrook, IL 60062Phone: +1.847.291.7396 Fax: +1.847.498.1512Email: [email protected]: www.reinholdenvironmental.com

Siemens Environmental Systems & ServicesBuzz Reynolds501 Grant St., 4th Floor Pittsburgh, PA 15219 Phone: +1.908.578.0693 Fax: +1.973.215.2557Email: [email protected]: www.wapc.com

Southern Environmental, Inc.John Caine6690 West Nine Mile Road Pensacola, FL 32526Phone: +1.850.944.4475 Fax: +1.850.944.8270Email: [email protected]: www.sei-group.com

Stock Equipment Co.Royce Warnick16490 Chillicothe Rd. Chagrin Falls, OH 44023Phone: +1.301.334.1882 Fax: +1.301.334.1883Email: [email protected]: www.stockequipment.com

URS CorporationGordon Maller9400 Amberglen Blvd. Austin, TX 78729Phone: +1.512.419.5045 Fax: +1.512.454.8807Email: [email protected]: www.urscorp.com

For more information

on the WPCA,

please visit our

website at

www.wpca.infoWahlco, Inc.Bill Hankins

2722 S. Fairview St. Santa Ana, CA 92704 Phone: +1.714.979.7300 Fax: +1.714.979.0603

Email: [email protected]