The prediction of flue gas emissions from the combustion in the industrial tubular heaters



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Ovidius University Annals of Chemistry Volume, Number 1, pp.137-11, 9 The prediction of flue gas emissions from the combustion in the industrial tubular heaters Mirela VELICU a, Claudia-Irina KONCSAG b and Anisoara NEAGU b a Rompetrol Quality Control, DJ, Km.3, 957, Navodari, Constanta b Ovidius University of Constanta, Department of Chemical Engineering and Technology, 1 Mamaia Blvd, 957 RO Constanta, Romania Abstract. The monitoring of gaseous emissions in a refinery is complex and difficult task requiring special equipment and operators in good physical shape. Some of these emissions could be calculated from other measured data from fixed analysis points. This shall decrease the number of determinations in hazardous circumstances. The authors of this study worked out some equations for the correlation of the main combustion emissions (CO, NO x ) with the oxygen content of flue gas and the temperature at the stack. Even though the CO emissions could be predicted by stoechiometric calculations, a model based on statistical processing of hundreds of data is easier to apply; this is why, the authors searched for simple and exact equations. The prediction of CO and NO x was made versus the the oxygen content of flue gas and the temperature at the stack, which can be measured with fixed sensors. Finally, the prediction of flue gas emissions can be performed by replacing the costly and dangerous sampling, using accurate mathematical model. Keywords: NO x emissions, modeling, flue gas monitoring 1. Introduction The main pollutants in the air proceeding from industrial activities are: CO, CO, NO x, SO x and particulates. Following the Directive in Europe and the Environmental Protection Act 199 in USA, the monitoring of these emissions and their balance are compulsory for any industrial actor. The prediction of the emissions is desirable for industry since the monitoring process requires a large number of analytical determinations in hazardous circumstances and expensive equipment. The modeling of different emissions was more interesting for the cement industry and for coal combustors by now [1-], but it could be done for the oil processing industry too, taking into account the large amount of emissions in this sector. The most important source of CO, CO, SO and NO x emissions in an oil refinery is the combustion in the industrial heaters. Since the emissions of sulfur oxides and CO depend only on the combustible s composition, the emissions of CO depend on the excess air for combustion and those of NOx on a few factors: the temperature of the burning process, the air excess, the geometry of the burners [5]. Taking into account these facts, the present study was designed to find correlations for the prediction of some pollutants, thus reducing the equipment and the number of determinations.. Experimental The experiment took place in a refinery were data from the monitoring program were acquired. The study was limited to vertical tubular parallelepiped heaters. Data from other type of heaters (boilers, heat economizers, Claus ovens) were far from the precedent because of very different combustion parameters and geometry. The monitoring program consists on sampling the flue gases from each combustor and determinate the concentration of CO, CO, NO x, SO and the temperature at the stack. Also, determination of these pollutants in six points around the refinery is done, in order to quantify the imissions. The ISSN-13-71 9 Ovidius University Press

13 The prediction of flue gas emissions... / Ovidius University Annals of Chemistry (1), 137-11 (9 frequency of these determinations is set at twice a month, and a portable analyzer is used. The gas analyzer MSI Compact 5 is a portable apparatus for multiple measurements the in the analysis of flue gas emissions. It is endowed with a standard proof stick for sampling. The sample point is located at two third from the baseline of the heater s stack. The list of parameters, measurement principle and precision are presented in Table 1. The measurements are instantaneous but they can be correlated among them and also with the fuel List of parameters composition. By consequence, the CO is calculated from the fuel composition alone, since the air excess is calculated from the fuel composition and oxygen in flue gas, in stoechiometric calculations. The data during a year long were acquired and 1 sets of complete data were available. The average minimum and maximum of the measured values are presented in Table. The NO x values correspond to the actual concentrations of O. In order to be compared they have to be normalized at 15% vol O [5]. Table 1. The main characteristics of the gas analyzer MSI Compact 5 Measurement principle Measurement range Precision Air temperature PTC resistor -1 o C 1 o C Gas temperature NiCr-Ni thermocouple -1 o C 1 o C Oxigen,O Electrochemical sensor -,9% vol..1% Carbon monoxide,co Electrochemical sensor - ppm vol. 1 ppm Carbon dioxide,co Calculated From the fuel composition.1% Nitrogen oxides,nox Electrochemical sensor - ppm vol. 1 ppm SO Electrochemical sensor - ppm vol 1 ppm Air excess Calculated 1-99.1 Table. The experimental data Parameter U.M. Average Minimum value Maximum value Oxygen in flue gas % vol 7. 1.5 15. CO in flue gas % vol 7.3.. NO x in flue gas ppm vol 3 3 39 Temperature at the stack K 9 37 91 Fuel gas composition: %vol C 1.7 7.7. C. 1.7 5.19 C 3. 1.95 17.11 C.5 1. 11.99 + C 5 3.37.3 1.3 H 15.19 5.7 3. CO,CO, O, N..5 1.1 Kcal/m 3 11133 7 157 Calorific power of flue gas at 15 o C/15 o C

M.Velicu et al., Ovidius University Annals of Chemistry (1), 137-11 (9) 139 The formula for this conversion is the Eq.(1): 5.9 NOx _ 15% = ( NOx NOxa ) n (1).9 O where: NO x measured during test; NO xa - the ambient concentration of nitrogen oxides; n- the ambient correction factor The Eq.(1) can be simplified by considering the ambient concentration of NO x as negligible, and the factor n equal to 1 for this application. The data were processed in Matlab and Excel using plotting and curve fitting facilities. 3. Results and discussion Some observations were made concerning the correlation between the at combustion α and the O content in flue gas on the one hand and between α and the CO content in flue gas on the other hand. In the first case, the O content increases with α following a logarithmic function, in the second case the CO decreases with α, following a power function, because of diluting the CO in flue gas with α increasing. The graphical correlations are given in Fig. 1 and Fig.. O in flue gas,%vol 1 1 1 1 1 y = 11,157Ln(x) +,351 R =,9 1 3 Fig 1. The variation of O content in flue gas with the α By processing the data, the equations () and (3) resulted: = 11.157 ln x +.351 () y r =.9.931 y = 11.7x r =.95 (3) The Eq.()describes the O content vs. the air coefficient α correlation and the Eq.(3)describes the variation of CO content with the α. Co in flue gas,%vol 1 1 Fig. The variation of CO content in flue gas with the α These correlations are interesting but only the first is important because it allows the calculation of the and of the excess air for combustion only by using the data acquired with the O sensor, without knowing the fuel composition. The second correlation is useful but indirectly since first the would be calculated with the Eq.(). This is why, the direct correlation of the CO content with the concentration of the O in flue gas (which can be measured with a fixed sensor for oxygen) is considered to be more useful. The correlation is presented in Fig. 3 and the Eq.() describes it. =.551x + 11.79 y = r y = 11,7x -,931 R =,95 1 3.9 () The Eq.() is as good as the Eq.(3) speaking on the correlation coefficient r.

1 The prediction of flue gas emissions... / Ovidius University Annals of Chemistry (1), 137-11 (9 CO, %vol 1 1 CO vs. O y = -,551x + 11,79 R =,9 literature [5], at 15% vol O, with the Eq.(1). Then, separate correlations were tried: NO x _ 15% vs.o in flue gas and NO x_15% vs. temperature at stack [K]. As seen in Fig. 5 and Fig., these correlations have poor coefficients (r =.7 and r =. respectively), mainly because of the fluctuations of the NO x measured with the portable equipment. 5 1 15 O, %vol Fig. 3. The variation of CO content in flue gas with O concentration Trying to correlate the NO x concentration in flue gas with other measured parameters, we observed that NO x content increases with the temperature at stack and with the excess air so that a 3 D plot was done as seen in the Fig.. NOX_15%, ppm y = 13,x +,171 3 R =,7 5 15 1 5 5 1 15 O,%vol Fig.5. The variation of NO x _ 15% with O in flue gas 3 NOX,ppm 35 3 5 15 1 3 temperature,oc 1 Fig.. 3D-plot of α- temperature at the stack -NO x in flue gas From Fig., one can see that experimental points can barely be correlated and this is due to the fact that NO x concentrations are measured in different conditions. It was necessary to normalize the concentrations by expressing them in the same conditions, as recommended in 1 3 NOX_15%,ppm Fig. The variation of NO x _ 15% with temperature at stack The flow of flue gas at the stack is inconstant and NO x values can vary by dozens in a second. However, one can combine these separate equations, in order to obtain an improved model, the Eq.(5): NO 5 15 1 5 x _15% + 7)].5 = [(13.x +. )(.1y y =,1x - 1,95x + 7,31 R =, 1 Temperature at stack,k 1.9y + (5)

M.Velicu et al., Ovidius University Annals of Chemistry (1), 137-11 (9) 11 In the Eq. (5) x represents the concentration of O in flue gas (%vol) and y represents the temperature at the stack (K). This equation allows the prediction of the NO x _ 15% concentration (ppm vol) through two directly measurable parameters. This model proved to be reliable since the NO x _ 15% calculated with the Eq.(5) differs from the measured NO x _ 15% by.% (average) and a medium standard deviation of ppm is good. These errors are acceptable taking into account that the experimental data were affected by measurement errors due to the specific of data acquiring system.. Conclusions The equations for the prediction of NO x and CO emissions worked out in this study are simple and accurate enough for the industrial use. The model is valid only for vertical tubular parallelepiped heaters, since for other geometries, the model for NO x is strongly affected. It was checked on industrial tubular heaters, of various capacity and size. The measured data were acquired twice a month, during a year long. The furnaces ran with fuel gas containing: C 1 (methane): 7.7-.% vol, C : 1.7-5.19% vol, C 3 :1.95-17.11%vol, C : 1.-11.99%vol, C + 5 :.3-1.3%vol, H : 5.7-3.%vol. The O concentration in flue gas varied between: 1.5-15.%vol, the temperature at the stack was: 37-91 K, and the measured values for CO were.-.% and NOx concentration varied between 3-39 ppm at the stack conditions. The prediction of CO concentration is based only on the measured O concentration in flue gas and not on the combustible composition, as at present. Also, the prediction of NO x is based on the same measured O concentration in flue gas plus the temperature at the stack. This is an important achievement since the expensive equipment for the measurement is avoided. The CO concentration wasn t interesting for this study since the was over 1.3 and the temperature at the stack was moderate most of time, so the concentration of CO is usually zero, rarely reaching a few ppm. One could give up the monitoring of CO at the stack of tubular vertical heater. So, instead of measuring the emissions at altitude with portable equipment twice a month, the stack of the heater should be equipped with fixed sensors for oxygen and temperature, and the CO and NO x emissions could be predicted with the equations worked out in this paper. The monitoring would be more effective since it would be continuous and unaffected by momentum measurements, as now. Also, the SO emissions can be found easy by stoechiometric calculations. 5. References *E-mail address: ckoncsag@univ-ovidius.ro [1]. J. Cojbasic, L. Cojbasic, V. Nikolic, N. Radojkovic and M. Vukic, Facta Universitas Series, Mechanical Engineering, 1(9), 13-17 () []. G.G. Szego, B.B. Dally and G.J. Nathan, Combustion and Flame, 15(1-), 1-5 () [3]. H.Tsuji, A.K. Gupta, T.Hasegawa, M. Katsuki, K. Kishimoto and M. Morita, High temperature air combustion, Ed. WARKS, U.K. (199) []. R. Weber, A.L. Verlaan, S. Orsino and N. Lallemant, Journal of the Institute of Energy, 7, 77-3 (1999) [5]. Buychok, M.R., Fundamentals of Stack Gas Dispersion, New Port Beach, CA, USA, (1995)