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- 2009 Annual Meeting
- Catalysis and Reaction Engineering Division
- Applied Environmental Catalysis II
- (547g) “Fast” NOx Storage On Pt/BaO/Al2O3 with NO+O2 Vs. NO2+O2
We studied a set of seven monolithic samples containing combination of 0.6, 2 and 6 wt. % Pt with 4, 8 and 20 wt. % Ba/ γ-Al2O3 using a flow reactor setup capable of simulating the NSR operation. After several short NOx capture ? regeneration cycles to condition the trap to the desired feed conditions, long capture phases (1.5 hr for feed containing NO2 + O2 and 1 hr for NO + O2) were run on them with the same feed, and NO and NO2 breakthrough curves were recorded. All the experiments were performed at 300°C and 30000/hr space velocity in presence and absence of 7% CO2, 8% H2O. *Total NOx Storage Capacity (t-NSC) and **Fast NOx Storage Capacity (f-NSC) of these traps was measured.
In absence of CO2 and H2O, the t-NSC on three samples loaded with 0.6, 2 and 6 wt. % Pt/20 wt. % Ba dropped by 35 (±5)% with NO+O2 as compared to NO2 +O2 in feed; whereas the f-NSC decreased by only 10 (±2)%. On samples containing 2 wt. % Pt/8 wt. % Ba and 0.6, 2 and 6 wt. % Pt/4 wt. % Ba, the t-NSC and f-NSC remained the same irrespective of NO or NO2 in feed with O2.
In presence of 7% CO2 and 8% H2O, the t-NSC on three samples with 0.6, 2 and 6 wt. % Pt/20 wt. % Ba dropped by 55 (±5)% with NO+O2 as compared to NO2 +O2 in feed; whereas the f-NSC also dropped by 45 (±5)%. On samples containing 2 wt. % Pt/8 wt. % Ba the t-NSC dropped by 25% but the f-NSC remained unchanged with NO+O2 and NO2+O2. Lastly on the samples loaded with 0.6, 2 and 6 wt. % Pt/4 wt. % Ba, the t-NSC and f-NSC remained the same irrespective of NO or NO2 in feed with O2.
We observed a clear trend in f-NSC/Ba (in mol NOx/mol Ba) with exposed Pt/Ba (mol exposed Pt/mol Ba), on the samples with same Ba loading. Hence we conclude that Pt plays a significant role in ?fast? NOx storage with NO2+O2 as well as with NO+O2. These results clearly indicate that in addition to NO oxidation, Pt also assists the sorption of NO2. It can be envisaged that O2 is the source of O* spilled over from Pt, which is used as an oxidant during the fast NOx storage. Thus, Pt on samples with higher exposed Pt/Ba can cater to a larger fraction of the available Ba by increasing the source number of O* available per Ba, giving rise to higher f-NSC on those traps. Our DRIFTS spectra show that, at 300°C, most of the NOx is stored in the form of Ba(NO3)2 on these traps. Formation of barium nitrate from BaO and two NO molecules requires 3O* compared to 1O* if NO2 is used instead of NO. Direct storage of NO on Ba also contributes to fast NSC in addition to storage of NO2. Lower fast NOx storage/Ba (mol/mol) on traps containing higher Ba loadings might be due to this direct storage since reduces the amount of Ba that can be reached by O* spilled over from Pt by consuming more O* per barium nitrate formed. Furthermore, in presence of CO2 and H2O in the gaseous lean phase feed, a fraction of the fast NOx storing Ba to which Pt can provide O* might be blocked due to formation Ba-cabonate, carboxylate and hydroxide, resulting in lower f-NSC. Our DRIFTS studies show that the stability of these species depends on the gas phase feed composition. On traps with lower Ba loading, f-NSC is unaffected for feed containing NO2+O2 and NO+O2 simply because the amount of Pt present is sufficient to produce the required O*. This mechanism can also explain our results for experiments with 50 to 600 ppm NO +320 ppm NO2 + 10% O2 in lean feed for which a small drop in f-NSC is seen on traps with 20 wt. % Ba and negligible change on traps containing 8 and 4 wt. % Ba. The trend in f-NSC/Ba with exposed Pt/Ba under these conditions remained the same as expected.
We also observed that the time to breakthrough (1% of the inlet NOx) changed proportionally when 100 to 450 ppm NO2 + 10 % O2 + 7% CO2 +8% H2O + Ar (balance) was fed; keeping the f-NSC constant. Using this fact and fitting parameters for a power law fit of the ratio of ^ideal fast NSC /measured fast NSC (y) and exposed Pt on the trap (x), a simple empirical correlation was developed for time to breakthrough and PNO2 in the exhaust for a trap with known Pt dispersion and Ba loading. This correlation is specific to our samples, but it highlights a simple approach which can be applied to any set of traps to yield required parameters to predict their f-NSCs. The correlation is simple enough to be used in real time with real time measurements of PNO2 and temperature of the vehicle exhaust.
* total NSC = integrated area above the NOx breakthrough curve and under the inlet [NOx] level
** fast NSC = time for 1% of the inlet NOx (NO + NO2) breakthrough x inlet [NOx]
^ ideal fast NSC - assuming that all the Ba on the trap identically contributes to the fast NSC