TG1: Real-time Instrument for Diesel Exhaust Particulate Measurement
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1 TG1: Real-time Instrument for Diesel Exhaust Particulate Measurement Sreenath B. Gupta USA Fig. 1 Panoramic view of prototype TG1 Slide 2: gives the terminology used in the presentation. Slide 3: A survey of available instrumentation in the US market shows that real-time quantitative measurements of particulate emissions to be elusive. The most promising instrument appeared to be the Tapered Element Oscillating Microbalance (TEOM). Slide 4: In comparison, Laser Induced Incandescence (LII), a rather new and simple technique can measure mass concentrations in vehicle exhausts in real-time. Furthermore, in combination with Rayleigh scattering can yield mean particle size, D (nm) and Number density, N (#/cc). Slide 5: In LII, soot particles are heated up to their sublimation temperature ( 4000 K) and the ensuing thermal radiation when collected in a certain manner provides a signal directly proportional to the local mass concentration. Slide 6: 2-D images of the soot fields measured in a laminar diffusion flame are shown. These images represent the capabilities of the LII + Rayleigh Scattering technique. Slide 7: At the initial stages of the program, computer modeling was used to investigate the effects of various parameters on LII signal. Such a study showed that the LII signal could vary with the engine exhaust temperature (SAE ). In a typical diesel, the exhaust temperatures could vary between o C. To reduce the effect of temperature variations, it was decided to dilute the engine exhaust before measurement. Slide 8, 9, 10: Initially experiments were performed in the exhaust of a sooting laminar diffusion flame. Varying the airflow rate in the burner varied the concentrations. Validation experiments were performed using a TEOM instrument. The signals measured are shown in slide 10. In such a setup, by performing a parametric study, it was determined that the required laser fluences are approx. 1.6 times those previously reported through inflame studies. The following measurements showed LII to be a very promising technique. Slide 11: Subsequently, it was decided to reduce this technique into an instrument. Our initial sketches are shown in the left figure. However, to confirm to our objectives of (1) Low-cost (2) Portable (3) Independent of engine size (4)
2 real-time and (5) modular in design, the final instrument resembled a 19 inch rack mount version as shown in the right figure. We will refer to this instrument as TG-1 henceforth. Slide 12: The prototype TG-1 was used to measure in the exhaust of a Mercedes Benz 1.7 L engine coupled to a low-inertia dynamometer. An SMPS provided the validation measurements. The agreement is shown in the graph on the right. Slide 13: To investigate the real-time measurement capabilities, the instrument was tested by switching the engine between three steady-state modes in a step like manner. While TG-1 proved far superior the TEOM-1100 showed negative values in certain regions. Rupprecht and Patashnick Co. which manufactures the TEOM when contacted mentioned that most of the problems were addressed in their current version of the instrument, i.e., TEOM Slide 14: Subsequently, a TEOM 1105 was procured and validation tests were performed. As the manufacturer had mentioned many of the problems were corrected in TEOM However, as shown in slide 9, one ought to realize that a TEOM measures the mass concentration by performing a derivative. A parametric study performed by varying the two time constants T MC and T TM in the TEOM software showed that both the time constants to be set to a minimum of 5 secs in order to obtain reasonable measurements. As a result, the minimum window for moving average is 5 secs for a TEOM TG-1 on the other hand provided comparable measurements with as little as 0.3 sec moving average. Slide 15: The comparative performances of TG-1 and TEOM 1105 while step changing the engine through three steady-state modes is shown. Slide 16: Similar comparative performances while operating the engine through a portion of the urban driving cycle is shown. Slide 17, 18, 19: Self-explanatory. Patents pending. For industrial partnership contact ragland@anl.gov Tel: (630)
3 TG-1: Instrument to Measure Diesel Exhaust Particulate Emissions in Real-time S. Gupta Engine and Emissions Research ETH Conference Zurich, 08/19/02
4 Diesel Exhaust Particulate Aerosol Soot Volatile Organics Sulfates Terminology Water vapor Mass Concentration MC (gms/cc) Number Density N (Number of Particles/cc) Mean Particle Diameter D (nm) Soluble Organic Fraction SOF (gms/cc)
5 Real-time Quantitative Measurements Difficult With Current Instrumentation Smoke Meters (Bosch, Hartridge) Filter Paper Collection (Sierra, Horiba, etc.) TEOM (Rupprecht & Patashnick Co, NY) ELPI (TSI, Inc.) SMPS (TSI, Inc.) - quantitative measurements difficult - steady state - overall measurement time 36 hrs typical - measurement every 5secs - could result in negative values - transients possible - extremely low size resolution - scan times typically 60 sec
6 Laser Induced Incandescence (LII) Primarily measures volume fraction, f v f v x ρ = MC (grams/cc) Can measure in real time; 10 Hz typical In combination with Rayleigh scattering yields Mean particle size (nm) D = Qvv K1 MC 1 3 Number density (#/cc) N = K 2 MC D
7 LII Phenomenon + Soot Particle Laser Pulse 4000 K Time
8 f v (ppm) D 63 (nm) x N (#/cc) Soot Volume Fraction Particle Diameter Number Density
9 LII Computer Modeling was Used to Gain Insight Into the LII Phenomenon e e e e e+12 laspow (W/m2) Particle Radius (nm) temerature(k) LII Signal (a.u.) e-11 Temperature (K) Laser Power (W/m 2 ) 1.6e e e e e e e e Particle Radius (nm) 4e-11 3e-11 2e-11 1e-11 LII Signal (a.u.) Time (ns) LII signal strongly varies with initial particle temperature; for typical diesel exhausts ( o C) dilution is necessary 0
10 Bench scale LII Experimental Setup
11 Tapered Element Oscillating Microbalance (TEOM) Tapered Element Oscillating Microbalance Measures Mass Concentration, M (g/cc) in Diesel Exhausts M = k f o 2 MC = 1 V dm dt = 1 V 2k f 3 o df dt f as well as accurately. df need to be measured dt
12 Critical Operational Parameters were Determined Through Experiments LII (a.u.) laspulse 30 slpm 40 slpm 50 slpm 60 slpm 70 slpm 80 slpm 90 slpm Start of Laser Pulse Time (ns) Parametric study shows optimal laser fluence ~ 1.6 times that previously recommended through in-flame studies
13 A Portable Prototype Instrument has Been Developed Detector Exhaust Signal Conditioning/ Display Laser Power Supply Prototype Low-cost Portable Cross-platform Real-time Modular design
14 TG-1 Shows Excellent Performance Over Typical Diesel Engine Operation 3 TG1 on MB 1.7 L Engine MC_SMPS (g/cc) LII Signal (V) 2 1 6e-8 5e-8 4e-8 3e-8 2e-8 1e Torque (Nm) 1000 rpm 1900 rpm 3100 rpm 3900 rpm 1000 rpm 1900 rpm 3100 rpm 3900 rpm TG1_MC (g/cc) 7e-8 6e-8 5e-8 4e-8 3e-8 2e-8 1e e-8 2e-8 3e-8 4e-8 5e-8 6e-8 7e-8 SMPS_MC (g/cc) Torque (Nm)
15 Transient response of TG1 Proved Superior Over That of TEOM 1100 MB 1.7 L engine coupled to a low-inertia dynamometer TG1 TEOM 1100
16 TG-1 has Faster Time Response Than a TEOM sig/mean sig/mean T_TM T_MC T_TM (s) T_MR/MC (s) σ / mean case # Averaging Time (s) TEOM-1105 TG-1
17 TG-1 has Faster Time Response Than a TEOM second moving average 3e-7 3e rpm 10 Nm 3500 rpm 120 Nm 1500 rpm 10 Nm 3e-7 3e-7 1.2e-7 1.0e rpm 10 Nm 5 sec moving average 3500 rpm 120 Nm 1500 rpm 10 Nm 1.2e-7 1.0e-7 TEOM MC (g/cc) 2e-7 2e-7 1e-7 TEOM 5s mvg avg TG1 0.3 s mvg avg 2e-7 2e-7 1e-7 TG1 MC (g/cc) TEOM MC (g/cc) 8.0e-8 6.0e-8 4.0e-8 TEOM TG1 8.0e-8 6.0e-8 4.0e-8 TG1 MC (g/cc) 5e-8 5e-8 2.0e-8 2.0e Time (secs) Time (secs) Transient measurements performed on a Mercedes Benz 1.7 L engine coupled to a low-inertia dynamometer
18 TG-1 Performance Over the Urban Driving Cycle 1.4e-7 1.2e-7 case 8; SA_Trans e-7 5 sec moving average 1.2e-7 TEOM MC (g/cc) 1.0e-7 8.0e-8 6.0e-8 4.0e-8 TEOM TG1 1.0e-7 8.0e-8 6.0e-8 4.0e-8 TG1 MC (g/cc) 2.0e-8 2.0e-8 Speed (rpm) Torqe & speed Time (secs) Torque (Nm)
19 Specifications for Prototype TG1 Size: (24 x 15 x 8.5 ) for TG1 + (19 x 8.6 x 15 ) for laser power supply Weight: Approx. 40 lbs. for TG lbs for laser power supply. Accuracy/ variability: SMPS measurements. Repeatability: Cost: Compatibility: ± 12% Full scale as compared to (not yet determined) To be determined Independent of engine size
20 Known Problems... Diluter needs constant cleaning Sample cell windows need cleaning every 1-3 days of operation Needs zero and span calibration almost everyday
21 Future Plans Install capabilities to measure N and D in real-time Decrease the size and weight; 19 in. rack mount version Market introduction through Sierra Instruments Inc., CA. Acknowledgements Primary financial support through Argonne s LDRD funding is gratefully acknowledged
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