2.1. Conversion Variation in a Commercial Vacuum Residue Hydrocracker Investigated by Intercriteria, Regression Analyses, ANN, and Pilot Plant Tests
Considering that the feedstock quality is the single variable that most affects oil refining unit performance [
8,
9,
10,
32], one may expect a performance change following the composition of the crude blend processed. Indeed, that was reported with the replacement of the Urals crude oil used by design with other petroleum crudes at the LUKOIL Neftohim Burgas (LNB) refinery (see its processing scheme in
Figure S1) in late 2023 and early 2024 [
33]. As a result of the lessons learned, the LNB refinery started to select crude oils that are expected to be processed without creating problems, such as increased fouling rate, corrosion rate, and poor performance of the most profitable conversion processes, ebullated bed vacuum residue H-Oil hydrocracking (see its flow diagram in
Figure S2) and fluid catalytic cracking (see the FCC process diagram in
Figure S3). In the initial process of replacing of Urals crude oil with other crude oils in December 2023, the H-Oil hydrocracker registered a drop in the vacuum residue conversion from 81 down to 72 wt.% with simultaneous increase of sediment content in the atmospheric tower bottom product (ATB). from 0.13 to 0.40 wt.% [
33]. This was also associated with an enhanced fouling rate at the bottom of the atmospheric tower. Then, by excluding the identified problematic crude oils, the H-Oil conversion level was enhanced up to 83 wt.% with a reduction in the ATB sediment content down to 0.03 wt.% in July 2024. However, along with the improvement of H-Oil performance, it was observed that the net vacuum residue conversion deviated from the predicted value based on the plug flow reactor model. The parameters of this model established in [
34] are as follows: an activation energy of 215 kJ/mol, a reaction order (
n) of 1.59, and a collision factor of
. This model was found to predict H-Oil conversion with the highest accuracy in comparison with the CSTR model (
;
kJ/mol;
n = 1.82) and the regression model as communicated in [
34]. This model had been developed using data from the H-Oil unit while processing vacuum residues derived from crude oil blends of 70% Urals/30% Middle East.
Figure 1 indicates a graph of variation of observed H-Oil net conversion and was calculated using the plug flow reactor model.
The discrepancy between the observed net H-Oil conversion and that calculated from the plug flow reactor model may come as a result from the treatment of different feedstocks. In order to verify this hypothesis, laboratory hydrocracking experiments with six distinct vacuum residues were carried out, and a regression model that predicts conversion at the same operating conditions from feed properties was developed. Then, this empirical correlation we called “feed reactivity”, along with commercial H-Oil data, which were evaluated by intercriteria analysis, resulted in a new regression model that predicts H-Oil conversion. Additionally, an artificial neural network (ANN) model was developed to compare its ability to predict H-Oil conversion with the regression model. Both models revealed that the composition of crude oil blends processed in the refinery affects substantially the level of H-Oil conversion.
2.1.1. Determination of the Feed Reactivity in the Ebullated Bed Vacuum Residue Hydrocracking
The conversion in the vacuum residue hydrocracking was found to be thermally driven [
35,
36], where the catalyst supplies hydrogen to the vacuum residue and prevents its carbonization [
36,
37], while at the same time removing the impurities (sulfur, nitrogen, and metals) [
23,
38,
39,
40]. For that reason, in most cases of vacuum residue hydrocracking, the catalyst has no impact on the conversion level [
24], although there are few reports announcing some effect of catalyst type on the conversion [
41,
42]. Thus, in order to increase the conversion, the vacuum residue hydrocracker operator augments reactor temperature. However, investigations have shown that some components in the vacuum residue can affect the thermal conversion level, for example, sulfur, which increases conversion [
43,
44,
45], and asphaltenes, which retard the vacuum residue conversion [
22,
46]. In order to find a quantitative relation of the vacuum residue properties with respect to the conversion level obtained at the same operating conditions, a multiple regression analysis of the data reported in [
8] was performed in order to define the hydrocracking feed reactivity. The conversion predicted by the multiple regression model developed (Equation (1)) was contrasted against the experimentally measured conversion, and as shown in
Figure 2, a good agreement was obtained.
where
VR hydrocracking reactivity = vacuum residue conversion, obtained during hydrocracking at the same operating conditions, wt.%;
Sulfur = vacuum residue sulfur content, wt.%;
Nitrogen = vacuum residue nitrogen content, wt.%;
Asphaltenes = vacuum residue C7 asphaltene content, wt.%;
Concarbon = vacuum residue Conradson carbon content, wt.%;
SG = specific gravity.
The double standard deviation of Equation (1) of 2.2 wt.%, used as an indicator for the uncertainty of prediction [
47], is very close to the uncertainty of the laboratory vacuum residue hydrocracking reported by Fortain [
48] of 1.7 wt.%.
For confidentiality reasons, the explicit form of Equation (1) cannot be revealed. The essence of Equation (1) reveals that vacuum residues, which have higher sulfur and lower nitrogen contents and are at the same time more aromatic (have a higher density and Conradson carbon content [
49]), and also have a lower ratio of asphaltenes to total aromatic carbon fractions (aromatics + resins + asphaltenes), exhibit higher conversion during hydrocracking at the same operating conditions.
Figure 3 shows the difference in the conversion, estimated by Equation (1) relative to the conversion of the base case, which is Urals vacuum residue, for all studied vacuum residues whose properties are shown in
Table 1. These vacuum residues have been hydrocracked in the commercial H-Oil hydrocracker in the LNB refinery. The Urals vacuum residue has been selected as a base case because the LNB H-Oil hydrocracker was designed to process this vacuum residue. The data in
Figure 3 exhibits the presence of significant variation (up to 16.4 wt.% difference in the estimated conversion) in the reactivity of the processed vacuum residual oils in the LNB H-Oil hydrocracker within the scope of this study. This reactivity difference could be the reason for the observed deviation between observed and estimated conversion with the activation energy of 215 kJ/mol and the reaction order of 1.59, and the collision factor of
established for the vacuum residue blend 75% Urals/25% Light Siberian [
34] (see
Figure 1).
2.1.2. Ebullated Bed Vacuum Residue Commercial and Pilot Plant Results at Different Operating Conditions
In order to search for relations between the operating conditions (reaction temperature (WABT), and reaction time
), conversion, yields, sediment content in hydrocracked residual oils, and mixed vacuum residue feed quality, an ICrA evaluation of data of 185 days of LNB commercial H-Oil unit (for the period 1 January 2024–10 July 2024) was performed. The range of variation of the LNB commercial H-Oil unit variables being analyzed by ICrA is given in
Table 2.
The dataset of 185 days of operation of the H-Oil vacuum residue hydrocracker was assessed by using ICrA.
Table 3 and
Table 4 present the μ and υ values of the ICrA evaluation of this dataset. The data in
Table 3 and
Table 4 indicate that the yields of gas, naphtha, and vacuum tower bottom (VTB) products have statistically meaningful consonances with the net conversion. The variables, which were expected to have appreciable influence on the net conversion, like the weight average bet temperature (WABT), the liquid hourly space velocity (LHSV), and the feed reactivity, were not identified by ICrA as statistically affecting the H-Oil conversion for the investigated dataset of 185 days of operation of the H-Oil vacuum residue hydrocracker. Neither did the sediment content in the hydrocracked atmospheric residue (ATB TSE) exhibit any statistically significant consonance with all variables examined in
Table 3 and
Table 4. However, when the laboratory hydrocracking experiments shown in
Figure 4 as a graph of the dependence of conversion, product yields, and hydrocracked atmospheric residue sediment content on reactor temperature are assessed by ICrA (see
Table 5 and
Table 6), one can see that the WABT has a very strong influence on the vacuum residue conversion (μ—value of 1.00 and υ—value of 0.00).
The same is evident from the data in
Table 5 and
Table 6, which show the relation of reactor temperature (WABT) against the hydrocracked atmospheric residue sediment content (ATB TSE) (μ—value of 1.00, and υ—value of 0.00), while in the commercial H-Oil unit the relation between WABT, and ATB TSE (μ and υ values are 0.29 and 0.45, respectively) evaluated by ICrA (see
Table 3 and
Table 4) suggests no effect of reactor temperature on the sediment formation rate exists. Such a discrepancy between the performance observed in the laboratory and the commercial hydrocracking units may be ascribed to the many variables acting simultaneously in the commercial unit, thus generating a strong noise, contrary to the laboratory unit, where the noise is much lower.
The employment of a regression analysis of the dataset of 185 days of operation of the H-Oil vacuum residue hydrocracker to assess the effect of reactor temperature, LHSV, H-Oil feed vacuum residue content, and feed reactivity (calculated by Equation (1)) indicated that these variables had statistically meaningful effect on the vacuum residue net conversion. The developed regression Equation (2), shown below, demonstrates a multiple correlation coefficient of 0.808 which could be considered statistically significant (R ≥ 0.75 implies the presence of a statistically meaningful relation).
where
H-Oil conv. = net conversion of vacuum residue in the commercial H-Oil hydrocracker, wt.%;
H-Oil feed VR% = content of vacuum residue (the material boiling above 540 °C) in H-Oil feed, wt.%;
Feed Reactivity = calculated by Equation (1) vacuum residue conversion obtained at the same operating conditions in the laboratory hydrocracking plant, wt.%;
WABT = weight average bed temperature of both reactors in the commercial H-Oil vacuum residue hydrocracker, °C;
LHSV = liquid hourly space velocity, h−1.
The p-values of all regression coefficients of Equation (2) are much lower than the significance level of 0.05, and therefore, they can be reckoned to have a statistically meaningful effect on the vacuum residue conversion. The results of ICrA and regression analysis evaluation of the commercial H-Oil vacuum residue hydrocracker data indicate that while ICrA detects the presence or absence of statistically meaningful relations of the individual variables, the regression analysis can discover the presence of a statistically meaningful relation of a combination of variables to the target variable, which individually have been found to have statistically meaningless relation to the target variable. The meaning of Equation (2) is that the H-Oil conversion depends not only on the operating variables WABT and LHSV but also on the reactivity of the vacuum residue mixture calculated by Equation (1) and the content of vacuum residue in the H-Oil mixed feed that can consist of vacuum residue, FCC slurry oil, FCC HCO, and vacuum gas oil.
The same variables, along with a more detailed characterization of the vacuum residue blend, including the contents of Conradson carbon, sulfur, nitrogen, saturates, aromatics, resins, C
5-asphaltenes, and C
7-asphaltenes, were used as input variables in an ANN model.
Figure S1,
Figure 5 and
Figure 6 present the results of ANN modeling of the commercial H-Oil vacuum residue conversion. Comparing the data in
Figure 7 with the reported multiple correlation coefficient of Equation (2) (R = 0.808), one can see the superiority of the ANN model (R = 0.942 for the test set) that predicts the H-Oil commercial hydrocracker vacuum residue conversion with a higher accuracy than the regression model (Equation (2)).
Figure S5 illustrates how the neural network training process has been accomplished to build the ANN commercial H-Oil hydrocracker vacuum residue conversion prediction model. It is evident from the data in
Figure S5 that the maximum number of epochs allocated for training was 5000, the time for the ANN training took 12 s, the desired mean squared error was set at
, as well as the achieved mean squared error was at
, and the training method used was that of Levenberg–Marquardt.
Figure 5 indicates graphs of the neural network training performance for prediction of commercial H-Oil hydrocracker vacuum residue net conversion. One can see from the data in
Figure 5 the three types of data: training, testing, and validation. The graph shows that the achieved mean squared error was 0.00028062, which occurred at epoch 5. After epoch 5, the mean squared error began to magnify for both testing and validation, meaning that no further improvement in the model accuracy could be expected.
Figure 6 is a cross-plot of predicted versus measured (target) H-Oil hydrocracker vacuum residue net conversion for the three types of data: training, testing, and validation. The correlation coefficients of the three types of data were found to be R = 0.9623 for training, R = 0.94151 for testing, R = 0.87062 for validation, and overall R = 0.946. The overall data comprised all subsets of data for training (70% of all data), testing (20% off all data), and validation (10% of all data).
2.2. Performance of Commercial Ebullated Bed Vacuum Residue H-Oil Hydrocracker during Employment of Cascade and Parallel Mode of Fresh Catalyst Addition
The effect of catalyst condition on the performance of commercial ebullated bed vacuum residue H-Oil hydrocracking during the employment of cascade mode of fresh catalyst addition is exemplified in the data shown in
Figure 7 and
Figure 8. They exhibit how the sediment content in the hydrocracked atmospheric residue suddenly went up at the beginning of the second (2018–2021) and third cycles (2021–2025) of the LNB H-Oil hydrocracker. The hydrocracked atmospheric residue sediment content at the start of the second cycle after 20 days on stream commenced enhancing and went beyond the maximum acceptable level of 0.3 wt.% (
Figure 7). On the 51st day of the second cycle, the sediment content reached the excessively high value of 1.1 wt.%.
Figure 8 shows exactly the same pattern of dynamics of the atmospheric residue hydrocracking sediment content change over time recorded at the beginning of the third cycle (2021–2025), when the fresh catalyst cascade addition system continues to be used as shown in
Figure 7. After 30 days from the start of the third cycle, the sediment level settled in increments beyond the maximum acceptable level of 0.3 wt.% and reached 0.96 wt.% on the 48th day. In both cycles, the increased sediment formation rate required a decrease in the reaction temperature, which ranged from 419 to 410 °C in the second cycle (
Figure 7) and from 428 to 415 °C in the third cycle (
Figure 8). It is interesting to note that regardless of using three different Ni–Mo-supported solid catalysts, they all exhibited the same poor sediment control at the beginning of the second and third cycles. The common in both cases was the formation of black powder in the first reactor that substituted the solid catalyst in this reactor and represented 80% of reactor inventory.
Figure 9 shows photographs of the catalyst unloaded from the first ebullated bed reactor (the left-hand side picture) and from the second ebullated bed reactor (the right-hand side picture) during 2018, and 2021 maintenance works. During the turnaround in Spring 2018 and Autumn 2021, the first reactor was loaded with fresh catalyst only, while the second reactor remained with the existing catalyst from the previous cycle.
The analysis of black powder revealed that it consists of metal sulfide particles as FeV2S4, NiV2S4, and (Ni, Fe)S and no presence of the original Ni–Mo-supported catalyst. It appeared that the catalyst inventory of the first reactor (R-1001) has been progressively replaced during the normal operation of the H-Oil unit by this material. This replacement has obviously occurred over a long period of time considering the concerned quantity. Moreover, the specific size and density of these particles have allowed them to co-exist with the equilibrium catalyst in the ebullated process. The analytical results for the size of the spent catalyst withdrawn from the first reactor over the same period showed it could not be attributed to an unusual breakage of the catalyst inside the reactor.
Figure 10 displays the results of fluorescence wave dispersion X-ray (WDXRF) spectrometry of the content of V, Ni, and Fe in three spent catalyst samples taken from the bottom of the first reactor, which represented 20% of reactor inventory, and three samples of black powder extracted from the first reactor, which was 80% of first reactor inventory during the maintenance work in Autumn 2021.
It is evident from these data that the contents of V, Ni, and Fe in the black powder are 3 times, 1.5 times, and 10 times as high as those of the spent catalyst, respectively.
Figure 11 demonstrates that the ratios
and
in the black powder are the same as those of the H-Oil feed and much different from those in the spent catalyst, suggesting that the origin of the black powder comes from the feed.
Scanning electron microscopy (SEM) (10 and 20 µm) and microprobe analysis of catalyst samples taken from the first and second reactors during the third cycle unveiled the following:
The cascade fresh addition system distinguishes with fresh catalyst addition in the second reactor, withdrawal of spent catalyst from the bottom of the second reactor and addition of the second reactor spent catalyst in the first reactor, and withdrawal from the bottom of the first reactor the spent catalyst from this reactor (see
Figure S6). The spent catalyst withdrawn from the second reactor is cooled from 420–430 °C down to 232 °C by the transport oil (heavy vacuum gas oil). Then, it is heated up again to 420–430 °C when it enters the first reactor. The catalyst undergoes a thermal shock, and the thin, not homogeneous layer of metal sulfides forms on the catalyst surface in the second reactor, which seems to be broken in the first reactor, releasing these metal sulfides while forming this way a black powder. All these findings suggest that the black powder originates from the not homogeneous metal-containing layer, formed on the outer surface of the catalyst in the second reactor. Considering that the parallel fresh catalyst addition system independently introduces catalyst in both reactors without using the spent catalyst from the second reactor as a catalyst for the first reactor, this system was chosen instead of the cascade one. Moreover, the parallel system enables the control of the activity of the catalytic system in both reactors independently, which, as detailed in [
50], allows better sediment control. Now the LNB H-Oil hydrocracker has been employing the parallel fresh catalyst addition system for two years.
The formation of black powder and the related loading of fresh catalyst in the first reactor during the maintenance works in Spring 2018 and Autumn 2021 were associated with poor sediment control and were far from the optimal performance of the commercial H-Oil hydrocracker, and restoring optimal sediment control took 130 days in both the second and third cycles (
Figure 7 and
Figure 8).
2.3. Conversion Variation in a Commercial Fluid Catalytic Cracking Investigated by Intercriteria, Regression Analyses, and ANN
Seventeen crude oils and two imported atmospheric residues were processed in the LNB refinery under study. The properties of these crude oils are presented in
Table S1. The vacuum gas oils derived from these 19 refinery feed oils were cracked in the LNB FCC unit, and their properties are summarized in
Table 7. Availing the correlations developed by Navarro et al. [
7] to predict FCC conversion at maximum gasoline yield (so-called crackability) from feed hydrogen content and that of Stratiev et al. [
51] relating FCC feed density to the hydrogen content, the following expression was established:
where
Crackability = FCC conversion at maximum gasoline yield, observed in laboratory ACE FCC unit wt.%;
d15 = density at 15 °C of FCC feed, g/cm3.
By using Equation (3) and the data from
Table 7, the crackability of the 19 vacuum gas oils converted in the commercial FCC unit was obtained and shown in
Figure 14.
The data in
Figure 14 display that the various vacuum gas oils (VGOs) have quite a different crackability, ranging from 69.5 to 77.7 wt.%. These vacuum gas oils, however, were cracked in the commercial FCC unit as blends and not individual VGOs. They were cracked on seven diverse FCC catalysts, whose characteristics are epitomized in
Table 8.
Table 9 witnesses the range of variation of variables, which affect FCC unit performance, registered during 194 days of LNB FCC unit operation, when the above-mentioned catalysts and VGOs were employed.
In order to investigate which variables from
Table 9 are statistically meaningful related to the FCC conversion, ICrA evaluation was used.
Table 10 and
Table 11 present μ and υ values obtained from the ICrA assessment. From all investigated variables, five were identified by ICrA to have a statistically meaningful relation to the FCC conversion. These variables are as follows: ΔCoke (μ = 0.18; υ = 0.75), FCC feed density (μ = 0.17; υ = 0.74), H-Oil VGO density (μ = 0.22; υ = 0.70), regenerator dense phase temperature (μ = 0.20; υ = 0.74), and regenerator dilute phase temperature (μ = 0.20; υ = 0.73). All of them are in negative consonance, implying that their magnification will be associated with a reduction in the FCC conversion. The variables FCC feed density and H-Oil VGO density concern the effect of feed quality on FCC conversion, as exemplified in Equation (3). Whereas the variable ΔCoke is a function of both feed quality and catalyst coke selectivity [
52,
53,
54]. The regression analysis of the data for 194 days of LNB FCC unit operation confirmed that ΔCoke depends on two variables related to FCC feed quality—density, and to catalyst characteristics—micro-activity, of the equilibrium catalyst. Equation (4) displays the developed ΔCoke correlation.
where
ΔCoke = the difference between coke on spent catalyst and coke on the regenerated catalyst in the commercial FCC unit, wt.%;
FCC feed d15 = density at 15 °C of the combined FCC unit feed, g/cm3;
ECAT Micro-activity = Micro-activity of equilibrium catalyst from the FCC unit, wt.%. (This is the conversion of a standard feed, measured in a laboratory ACE FCC unit on an equilibrium catalyst sample at a catalyst-to-oil ratio of 4.0 wt./wt., and reaction temperature of 527 °C)
The regenerator temperatures are dependent on the ΔCoke (μ = 0.84; υ = 0.12) and therefore their influence on the FCC conversion is accounted by the ΔCoke.
Regression of FCC feed crackability data, estimated by density and Equation (3), along with ΔCoke, against the FCC conversion led to the development of Equation (5).
where
FCC conversion = conversion of material boiling above 210 °C in FCC unit, wt.%;
Crackability = estimated by Equation (3) conversion of FCC feed at the maximum gasoline yield observed in laboratory ACE FCC unit, wt.%.
For this dataset, the riser outlet temperature had no statistically meaningful effect on the FCC conversion. Laboratory cracking experiments in an ACE FCC unit with a feed consisting of 75% straight run VGO and 25% H-Oil VGO, having 73.0% crackability, and using catalyst F in the reactor, a temperature range of 526–550 °C, were used to elucidate the reason for not detecting any effect of reactor temperature on conversion in the commercial FCC unit.
Figure 15 witnesses the variation of FCC feed conversion with catalyst to oil ratio changing for two reaction temperatures (526 and 550 °C). One can calculate from the data in
Figure 15 that at each 10 °C reaction temperature alteration, the FCC conversion fluctuates with about 1.3 wt.%.
Having in mind that the fluctuation of reaction temperature for most of the FCC data presented in this work ranges between 540 and 550 °C, the effect of reactor temperature seems to be suppressed by the wider ambit of VGO feed crackability variation. The FCC feed crackability was mainly controlled by the percent of H-Oil VGO in the FCC feed and by the content of FCC slurry oil in the H-Oil feed, since the blended straight-run VGO crackability for the studied data varied in the narrow range of between 72.0 and 75.6 wt.%. A regression of these two variables against the FCC conversion led to the development of Equation (6).
where
%HOilVGO in FCC feed = the content of H-Oil VGO in FCC feed, wt.%;
%FCCSLO in H-Oil feed = the content of FCC slurry oil in H-Oil feed, wt.%.
It deserves mentioning here that the increase of equilibrium catalyst activity from 69.0 to 77.1 wt.% (see
Table 9) does not give a positive effect on the commercial FCC unit conversion. Instead, it increases ΔCoke (see Equation (4)) that eventually leads to a reduction of the FCC conversion by 2.4 wt.% (see Equation (5)).
The 194 operating days of the FCC unit were employed to construct an ANN model predicting FCC conversion.
Figure S7 exemplifies how the neural network training process has been accomplished to build the ANN commercial FCC vacuum gas oil feed conversion prediction model. The data in
Figure S5 shows that the maximum number of epochs allocated for training was 5000, the time for the ANN training took 68 s, the desired mean squared error was set at
, as well as the achieved mean squared error was at
, and the training method used was that of Levenberg–Marquardt.
Figure 16 indicates graphs of the neural network training performance for prediction of commercial H-Oil hydrocracker vacuum residue net conversion. One can see from the data in
Figure 17 the three types of data: training, testing, and validation. The graph shows that the achieved mean squared error was 0.0015754, which occurred at epoch 10. After epoch 10, the mean squared error did not keep on falling for validation, meaning that no further improvement in the model accuracy could be expected.
Figure 17 is a parity graph of predicted versus measured (target) FCC VGO feed conversion for the three types of data: training, testing, and validation. The correlation coefficients of the three types of data were found to be R = 0.99182 for training, R = 0.95393 for testing, R = 0.74011 for validation, and overall R = 0.89046. The overall data comprised all subsets of data for training (70% of all data), testing (20% off all data), and validation (10% of all data). The lower accuracy of the FCC conversion fit for the validation data is a result of quite inaccurate prediction of conversion of 100% H-Oil VGO (65% predicted versus 48.2 wt.% observed). There was only one point for 100% H-Oil VGO being a feed of the studied commercial FCC unit that was not included in the training of the ANN model. Therefore, a good FCC ANN model would require all possible variations to be present in the training and validation processes to a fairly large extent. The test set that included data not utilized in the training and validation demonstrated quite a good predictability with R = 0.9593, which is much better than the multiple correlation coefficient of regression Equation (5) (R = 0.864).