1. Introduction
Currently, renewable fuels are increasingly in demand due to the high consumption of fossil fuel resources (petroleum and natural gas), whose use produces global warming, and their reserves are limited and concentrated in some countries suffering conflicts. In this context, biofuels have attracted much attention as renewable fuels [
1], having environmental benefits and being necessary for the sustainable development of society [
2]. One remarkable example of biofuels is biodiesel consisting of fatty acid alkyl (mainly methyl) esters (FAMEs) derived from vegetable oils or animal fats [
3]. A better alternative is the production of green diesel by catalytic hydroprocessing of triglycerides or carboxylic esters to generate hydrocarbons (hydrotreatment of vegetable oils, nonedible oils or fats, HVO). Another way to obtain green diesel is Fischer–Tropsch synthesis, which produces known GTL (gas to liquids) diesel. The hydrocarbons obtained after these processes have good combustion properties but also a high cloud point, which invalidates them as hydrocarbon-based fuel (green diesel). The best way to decrease the cloud point and produce a suitable green diesel is the hydroisomerization of these lineal alkane fuels. Green diesel stands out for its high cetane number, low cloud point, absence of aromatic hydrocarbons and sulfur, and lower emissions of greenhouse gases [
4].
Hydroisomerization is the process of isomerization in the presence of hydrogen. The classical isomerization mechanism consists of dehydrogenation on the metal, protonation of olefins on the Brønsted acid sites with the formation of a secondary alkylcarbenium, rearrangement of the alkylcarbenium ion, deprotonation, and hydrogenation [
5]. Effective hydroisomerization catalysts should minimize hydrocracking and parallel side reactions that lower the liquid fuel yield [
4,
5] and achieve high isomerization selectivity for long chain hydrocarbons, resulting in a high liquid yield [
6]. In oil refineries, selective isomerization is a highly desirable reaction that is more difficult to realize in long chain hydrocarbons than in short chain alkanes [
6]. Thus, the hydroisomerization of large hydrocarbons requires optimizing the acid strength to avoid excessive cracking. Isomerization reactions usually occur over bifunctional catalysts via carbenium ions. The two functions of these catalysts are metallic sites (mostly noble metals such as platinum and palladium) for hydrogenation/dehydrogenation and acid sites for skeletal isomerization [
5,
7]. Two types of catalysts can be used for the isomerization of alkanes: solid acids loaded with a transition metal (mostly Pt) used in industrial isomerization processes (often called bifunctional catalysts) and acid catalysts (homogeneous or heterogeneous) [
5,
7]. There are several acidic supports that can be used as the acidic function in these required bifunctional catalysts for hydroisomerization, such as mesoporous materials (MCM-41, MCM-48, SBA-15), zeolites (ZSM-5, ZSM-22, Y, Beta), and silicoaluminophosphates (SAPO-11, SAPO-31, SAPO-41) [
5,
6,
8].
Tungstated zirconia (WO
x/ZrO
2) is found to be an efficient solid acid catalyst and/or catalytic support because of its remarkable properties, such as strong acidity due to WO
x, high thermal stability, slow deactivation, superior stability under both oxidizing and reducing conditions, the amphoteric character of its surface hydroxyl groups, and its ease of preparation [
9,
10]. WO
x/ZrO
2 is structurally more stable than sulfated zirconia, which is widely studied [
11], since these catalyst compounds tend to form volatile sulfur compounds under catalysis and regeneration conditions [
9]. Overall, tungstated zirconia is active for isomerization and alkylation of hydrocarbons [
12]. Several catalyzed reactions such as alkylations, dimerizations, and acylations show good WO
x/ZrO
2 activity results. The catalytic performance of WO
x/ZrO
2 varies with the activation temperature and W loading [
10].
Alumina has not been studied as well as zirconia, but some studies can be found using Pt/WO
x/Al
2O
3 for selective glycerol hydrogenolysis to 1,3-propanediol [
13,
14] and showing the relationship between the structure and activity of supported Pt-WO
3 catalysts for hydrogenolysis [
2] or using alumina- and silica alumina-supported WO
3 catalysts for the esterification reaction of acetic acid with
n-butanol [
15]. Another example is the introduction of a metal function (0.3 wt % Pt) on WO
x–Al
2O
3 (8.4 wt % W), which produces bifunctional alkane conversion reactions where acid sites catalyze the isomerization and β-scission reactions of alkenes and metal sites catalyze alkane dehydrogenation because WO
x species appear to interact strongly with sites on the surface of γ-Al
2O
3 [
16].
We chose zirconia and alumina as supports and introduced acidity with the incorporation of tungsten oxide. Catalyst properties such as metal dispersion, macro/mesopore distribution, and strength and density of acid sites influence the selectivity and the hydroisomerization rate and, for this reason, have been studied carefully.
The hydroisomerization catalysts that we tested require a reduction step before the reaction to obtain WO3 oxide, which interacts with alumina and zirconia, favoring the reaction. Temperature reduction has a decisive influence on the conversion results because it affects catalyst properties and has not been widely studied. Considering the results published in the literature for hydroisomerization, the aim of this work is to study the influence of the reduction temperature and the support nature in the hydroisomerization (catalytic behavior, acidity and dispersion) of n-dodecane to improve the lineal alkane fuels mentioned before and produce a suitable green diesel.
Thus, in this study, the hydroisomerization of
n-dodecane is discussed over three bifunctional catalysts to improve the lineal alkane fuels obtained through Fischer–Tropsch, HVO, or any other process. Pt-supported (0.3 wt % Pt) on W-modified alumina or zirconia were used as catalysts. These catalysts were characterized by different techniques indicated in the
Section 2. Correlations between activity and characterization results were established to determine which properties identify the optimum reduction temperature and the best support.
2. Results and Discussion
The chemical analysis of catalysts confirms the loading of W and Pt with a content very close to the nominal 14.7–15.2 wt % W and 0.27–0.28 wt % Pt.
Textural properties were determined by N
2 adsorption–desorption. The BET surface area, mean pore volume, and mean pore diameter of alumina and zirconia supports and catalysts are reported in
Table 1.
When the active phase is impregnated onto the support, the surface areas and pore volumes decrease due to the incorporation of tungsten oxide partially covering the support surface, partly blocking the support pores and reducing nitrogen accessibility [
17]. Pore volume does not vary in PtW/ZrC with respect to its support, W-ZrO
2C support, because this support already has WO
3 in it, and the small amount of platinum added is not enough to block the pores. Only a decrease in the BET surface area is observed in this case. Comparing the three supports, the surface area shows the following variation: PtW/Al > PtW/ZrC > PtW/Zr with values of 244 m
2/g for alumina, 117 m
2/g for commercial tungstated zirconia, and 97 m
2/g for zirconia.
To characterize the porosity of this sample, N
2 adsorption–desorption isotherms of the supports and catalysts were obtained and are depicted in the
supplementary information (Figure S1). All the isotherms belong to type IV (a) according to the IUPAC 2015 classification or type IV according to the BDDT (Brunauer, Deming, Deming, and Teller) classification, given by mesoporous materials [
12,
15]. According to the IUPAC system, the hysteresis loops obtained in the isotherms can be classified as the H3 type for ZrO
2 support, PtW/Zr catalyst (
Figure S1A), Al
2O
3 support and PtW/Al catalyst (
Figure S1C), and H2 type for W-ZrO
2C support and PtW/ZrC catalyst (
Figure S1B). In addition, the type of pore can be deduced from the isotherm hysteresis loop. Zirconia and alumina isotherm hysteresis loops are close to slit-shaped pores (H3 hysteresis type). Hysteresis loops for commercial tungstated zirconia isotherms indicate the existence of bottleneck type pores (H2 type) [
15,
18,
19]. Comparing the support and catalyst isotherms in the three cases, both isotherms are very similar visibly, which means a high dispersion of the WO
3 and Pt active phases on the support. The pore size distribution curves of the support and the catalysts are compared in the
supplementary information, Figure S2. All the supports and catalysts show pore size distributions in the mesopore range from 2 to 50 nm.
The ZrO
2 support (
Figure S2A) presents three components: one wide peak with a relative maximum at 7.4 nm, another sharper peak at a higher diameter (9.6 nm), and the broadest and least defined peak at 12 nm. The second component is not visible on the PtW/Zr catalyst, modifying the original pore size distribution profile of the support and suggesting a partial blocking of the zirconium pore structure when adding the Pt and W active phases. Thus, the PtW/Zr catalyst shows a bimodal pore size distribution profile with two components: one at 7.1 nm and the other at 11.7 nm. In contrast, the W-ZrO
2C support and PtW/ZrC catalyst (
Figure S2B) show both a unimodal pore size distribution with a maximum at 4.3 nm. Both distributions show a visible small shoulder at 3.4 nm. The Al
2O
3 support (
Figure S2C) shows two main components, one at 7.9 nm and the other at 9.0 nm, which are converted into the only component in the catalyst PtW/Al at 8.0 nm, which also suggests a partial blocking of the alumina pore structure after the addition of the active phases. A broad shoulder is seen in the support at 10.2 nm, less defined in the catalyst but also included. The samples supported on alumina and zirconia present a wider range of pore sizes, while the samples supported on commercial tungstated zirconia (ZrO
2 com support and PtW/ZrC catalyst) show a narrower pore size distribution, mainly between 2 and 5 nm.
The crystalline phases present in the samples were studied by X-ray diffraction. The X-ray patterns obtained are shown in
Figure 1 and the crystalline phases found are reported in
Table 2. In general, the X-ray diffractograms of the catalysts do not show many different lines compared with the supports.
For the PtW/Zr catalyst (
Figure 1A), the most intense diffraction lines are located at 28.1 and 31.4°, and these lines are associated with the (111) and (−111) planes, respectively, of monoclinic ZrO
2. The diffraction lines at 2θ = 17.5, 24.0, 28.1, 34.1, 34.3, 35.0, 38.6, 40.6, 44.8, 49.2, 50.4, 54.2, 55.4, 60.1, 61.5, 62.7, 71.2, and 75.2° were attributed to the monoclinic phase of the ZrO
2 support. There are also some minor peaks associated with the tetragonal phase of ZrO
2.
In addition, no obvious sharp diffraction peaks of WO
3 were found, meaning either a homogeneous dispersion of WO
3 on the support surface [
20] or a very small crystallite size of WO
3 [
15]. Most WO
3 peaks overlapped with monoclinic ZrO
2 peaks. The most intense diffraction line for WO
3 is the one at 24.0°, corresponding to the (110) plane of WO
3, but it overlaps with the diffraction line of the support. The absence of platinum diffraction peaks also revealed the high dispersion of this metal on the catalyst, which was expected due to the low Pt loading.
For the PtW/ZrC catalyst (
Figure 1B), the most intense diffraction line is placed at 30.2° associated with the (101) plane of tetragonal ZrO
2. In this catalyst, no obvious diffraction peaks of WO
3 were found, meaning even a better dispersion of WO
3 than in the PtW/Zr catalyst because fewer WO
3 peaks were found. The peaks observed at 2θ = 30.2, 35.3, 50.2, 60.2, 62.8, 74.5, 82.5, and 84.9° were assigned to the tetragonal phase of zirconia. There are also some minor peaks overlapping with those diffraction lines corresponding to tetragonal ZrO
2 associated with the monoclinic phase of the W-ZrO
2C support, but, in this case, most peaks correspond to the tetragonal phase. The ZrO
2 supports are both crystalline, showing sharp peaks.
For the alumina support and PtW/Al catalyst (
Figure 1C), the XRD spectra present three main peaks placed at 36.9, 47.6, and 67.4°, corresponding to the (111), (006), and (215) planes of γ-Al
2O
3, respectively. The lower intensity of the diffraction lines for the catalyst is explained by the smaller amount of sample placed in the sample holder. Again, few obvious sharp diffraction peaks were found for WO
3 or W
3O
8, indicating a high dispersion of tungsten oxide in the support.
The Scherrer equation was applied to the most intense and non-overlapping diffraction line to determine the average crystalline domain. These values are also given in
Table 2.
The average crystalline domain sizes of the corresponding zirconia crystallites are similar comparing each support and catalyst, showing sizes of approximately 10 nm. In the case of alumina and alumina-supported catalysts, this determination has not been calculated since the alumina phase (gamma) is poorly crystallized (pseudocrystalline state), and pseudocrystals form its structure.
Molecular structure was studied by Raman spectroscopy.
Figure 2A shows the Raman spectra of the ZrO
2 support and the PtW/Zr catalyst with a profile corresponding to the monoclinic zirconia phase. The ZrO
2 support exhibits Raman bands at 180, 333 (with a shoulder at 306), 380, 473, 539, and 620 cm
−1 corresponding to the monoclinic phase [
21,
22,
23]. In the PtW/Zr catalyst, the same bands are observed at 180, 330, 378, 473, 540, and 630 cm
−1. These bands are consistent with the main zirconia phase observed by XRD.
PtW/Zr also shows bands at ~800 and ~700 cm
−1, which are characteristic of stretching and bending vibrations of W-O-W, respectively. These bands are also characteristic of crystalline WO
3 [
17]. The band at approximately 270 cm
−1 is assigned to the W-O-W deformation mode [
22]. In addition, a broad band with two components at 955 and 995 cm
−1 is attributed to asymmetric and symmetric vibrations of W=O, respectively [
9]. More bands of monoclinic zirconia were found at higher frequencies, with Raman modes at 1340, 1515, 1579, and 1670 cm
−1 assigned to the ZrO
2 support and Raman modes at 1333, 1517, 1578, and 1680 cm
−1 assigned to the PtW/Zr catalyst.
Figure 2B shows the Raman spectra of the W-ZrO
2C support compared to the spectra of the PtW/ZrC catalyst. These profiles correspond to the tetragonal zirconia phase [
24]. Almost the same Raman profile was obtained for this catalyst and its corresponding support, as in all techniques because the only difference between them (0.3 wt % platinum) is not remarkable. These spectra are characterized by two very intense Raman bands [
25] at 1340 and 1535 (with a small shoulder at 1670) cm
−1 in the support and 1350 and 1540 (with a small shoulder also at 1670) cm
−1 in the catalyst.
The W-ZrO
2C support also exhibits small Raman bands at 150, 180, 317 (with a shoulder at 278), 420 (with a shoulder at 468), 636, 2223, and 2320 cm
−1 that come from the tetragonal phase. In the PtW/ZrC catalyst, the same bands are observed at 170, 318, 429, and 624 and 2310 cm
−1 frequencies [
21,
22]. A broad and small band at 840 cm
−1 in the support and catalyst originates from the W-O-W stretching vibration mode [
17]. The ZrO
2 com support also shows a band at 962 cm
−1 in the support, which appears at 995 cm
−1 in the catalyst and is attributed to the stretch asymmetric vibration mode of mono-oxo W=O, corresponding to highly dispersed WO
x species, in agreement with the XRD results. This small shift might be attributed to the interaction between Pt and external tungsten oxides. Due to this interaction, electrons from Pt to WO
3 formed in the catalysts are transferred, and the distortion of oxo-tungsted species is affected, resulting in an enhancement of the W=O bond strength [
20].
Figure 2C shows the Raman spectra of the Al
2O
3 support compared to the PtW/Al catalyst. γ-Al
2O
3 (calcined at 500 °C) only exhibits two Raman bands at 1315 and 1518 cm
−1 for the support and catalyst, indicating the pseudoamorphous alumina state, in accordance with the XRD diagrams obtained for this support and catalyst. In addition, for low calcination temperatures (500–800 °C), below monolayer coverages less than ~25–30% WO
3 on Al
2O
3, tungsten oxide has been proven to be in a highly dispersed and amorphous state on the alumina surface [
26], and no WO
3 Raman peaks appear in the spectrum of the PtW/Al catalyst, which is also in line with the higher surface area of this support compared to the zirconia counterparts.
The dispersion of the catalysts (reduced at 250 °C, in order to avoid a partial reduction of tungsten oxide that could be produced at 300 °C and above) was determined by CO pulse chemisorption. The results obtained, reported in
Table 3, indicate that the highest dispersion is achieved in the PtW/ZrC catalyst, followed by PtW/Zr and PtW/Al. Dispersion could not be measured at the same reduction temperature used in the reaction (350 °C) because, in the zirconia catalysts, WO
3 was reduced by approximately 400 °C [
27,
28], and dispersion measures would include adsorption on WO
3-δ, not only Pt.
The catalyst acidity was investigated by TPD of ammonia. This technique usually measures the strength of acid sites present on the catalyst surface as well as the total acidity [
9]. The desorption profiles of the catalysts are depicted in
Figure 3.
Figure 3 shows the ammonia TPD profiles for all three catalysts, with three different desorption peaks that correspond to the following three acid strengths: low strength (desorption peaks <250 °C), medium acid strength (desorption between 250 and 400 °C), and strong acid sites (desorption temperature >400 °C) [
29,
30]. The desorption profile of PtW/Zr shows complex desorption peaks with several components. The most intense peak, located at approximately 200 °C, is attributed to weak strength acidity, a second less intense peak, centered at approximately 375 °C, is attributed to moderate strength acidity, and, finally, a low intensity contribution at high temperature (500 °C), is attributed to strong strength acidity. The TPD profile for PtW/ZrC is quite similar but with a higher relative intensity and a higher number of acid sites. The ammonia TPD profile of PtW/Al is clearly different from the ammonia TPD profile of its zirconia counterparts showing an intense peak due to ammonia desorption from weak acid sites at 200 °C, a small component of the desorption of intermediate strength at 300 °C and a more intense desorption peak from strong acid sites at 530 °C. The proportion of strong acid sites in alumina-based catalysts is clearly higher than the proportion of strong acid sites in both zirconia-based catalysts. These results can be related to a stronger interaction of WO
x species with alumina by a smaller size of WO
x particles and at the same time related to the higher surface area of alumina support (
Table 1). This result agrees with the absence of Raman peaks for WO
x in this catalyst (
Figure 2). As reported in
Table 3, the total acidity amount was measured and follows the order PtW/Al > PtW/ZrC > PtW/Zr, which agrees with the conversion results.
The nature of the surface acidity is the adsorption of pyridine as a base on the surface of solid acids. The use of IR spectroscopy to detect the adsorbed pyridine facilitates the distinction of different acid sites [
9]. The FTIR pyridine (DRIFT) absorption spectra of the PtW/Zr, PtW/ZrC and PtW/Al catalysts were measured at room temperature at different reduction temperatures: 250, 300, 350, and 400 °C (
Figure 4).
The FTIR spectra of pyridine adsorbed on samples show the presence of adsorption bands centered at 1607–1617, 1573, and 1442–1450 cm
−1, which are assigned to the vibrational modes of pyridine adsorbed on Lewis (L) acid sites. A wide band at 1540 cm
−1 is assigned to pyridinium ions absorbed due to Brønsted (B) acidity. The absorption band at 1488 cm
−1 is influenced by both Lewis and Brønsted acid sites [
9,
10,
20,
31]. The presence of Lewis acid sites can be attributed to the presence of coordinately unsaturated Zr
4+ cations, while the B sites are likely hydroxyl groups (W–O–W–OH or Zr–O–W–OH) associated with W
6+ and W
5+ atoms [
10].
The reduction temperature clearly affects the intensity of the bands of adsorbed pyridine. In general, the intensity of the bands increases when increasing the reduction temperature [
32]. The acid character (relative Brønsted versus Lewis acid) can be estimated from the intensity ratio of the bands at 1540 cm
−1 and 1450 cm
−1 [
32] from DRIFT spectra. A slightly higher relative acidity is achieved from the PtW/Al catalyst at a reduction temperature of 350 °C, which can be related to the higher i-C
12 yield obtained for this catalyst at a reduction temperature of 350 °C.
The acidity of ZrO
2 is ascribed mainly to Lewis acid sites, principally because of the greater ionic character of the Zr-O bond [
33]. Thus, although Zr-OH contributes to Brønsted acid sites of weak basicity, the main contribution to acidity comes from anion vacancies on the surface of ZrO
2, exposing CUS (coordinatively unsaturated) Zr
4+ cations that present strong Lewis acidity [
34]. As observed in
Figure 3, the appearance of a peak at approximately 500 °C is an indication that the addition of WO
3 to zirconia introduces additional strong Brønsted acid sites, evidencing the presence of both Lewis and Brønsted acid sites on WO
3/ZrO
2 samples [
35,
36]. The fact that WO
x species are well dispersed seems crucial to maximize the surface acidity by the formation of Zr-containing polytungstates (by coalescence of isolated WO
x clusters) [
32]. If these WO
x species agglomerate, forming WO
3 bulk crystallites, a loss of surface Brønsted acidity is produced.
Surface chemical analyses of the catalysts were carried out by XPS. XPS spectra for the PtW/Zr, PtW/ZrC, and PtW/Al catalysts are shown in
Figure 5, and the binding energies (eV) (Al2p, Zr3d, W4f
7/2, Pt4f
7/2 core levels) and surface atomic ratios are listed in
Table 4.
The binding energy found for the Al 2p or Zr 3d core level corresponds to Al
2O
3 or ZrO
2, respectively. The W 4f signal presents a typical doublet corresponding to spin orbital splitting. PtW/Zr and PtW/ZrC catalysts show a single component with BE for W4f
7/2 at approximately 35.4 eV attributed to WO
3 (nanocrystals) species, while the PtW/Al catalyst presents two components, one attributed to WO
3 species (35.3 eV) and a second attributed to aluminum tungstate at approximately 36.5 eV [
37]. Therefore, W supported on ZrO
2 forms one unique species, WO
3, but W supported on Al
2O
3 forms two species, WO
3 and aluminum tungstate.
Pt was detected and measured in ZrO2 catalysts, showing two peaks centered at 71.6 eV in PtW/Zr and 71.7 eV in PtW/ZrC (for Pt0) and 73.3 in PtW/Zr and 73.8 in PtW/ZrC (for Ptδ+). However, the strong overlap of the Pt4f signal with the Al 2p signal of the support makes it impossible to measure the platinum signal on alumina-based catalysts. Platinum species are reduced, but the strong interaction with oxygen of supports shows the presence of oxidized species.
The surface atomic ratio W/(Al or Zr) shows the following trend: PtW/ZrC > PtW/Zr > PtW/Al. Despite the higher specific surface of alumina and the absence of tridimensional crystalline species in XRD profiles, the W/Al is very low. This low value can be explained by the presence of aluminum tungstate species; the formation of this kind of species usually forces the migration of surface tungsten to the interior of the alumina, reducing the W signal observed by XPS.
Summarizing the characterization techniques used (N2 adsorption–desorption isotherms at −196 °C, X-ray diffraction, Raman spectroscopy, FTIR, NH3-TPD, CO pulse chemisorption, and XPS), we can conclude that the alumina catalyst achieves a higher surface acidity than zirconia catalysts, which is related to a stronger interaction of WOx species with alumina by a smaller size of WOx particles and at the same time related to the higher surface area of alumina support. The absence of WO3 diffraction peaks in XRD for all catalysts revealed the homogeneous dispersion of this oxide on the catalytic support, in agreement with the Raman analyses. XRD diagrams and Raman spectra also indicate that ZrO2 exists mainly in the monoclinic system, whereas W-ZrO2C exists mainly in the tetragonal system.
To study the influence of the reduction temperature on the activity and selectivity, PtW/Zr PtW/ZrC and PtW/Al catalysts were investigated for the hydroisomerization of
n-dodecane using four different pretreatment reduction temperatures: 250, 300, 350, and 400 °C (
Figure 6). Having the best reduction temperature, 350 °C, PtW/Zr, PtW/ZrC, and PtW/Al catalysts were studied in the hydrosiomerization of
n-dodecane with the same reaction conditions (Tr = 350 °C, P = 2.0 MPa, liquid flow = 0.1 mL·min
−1 and H
2 flow = 340 mL
N·min
−1) in a trickled bed-mode reactor (
Figure 7).
Pretreatment with different reduction temperatures prior to the reaction affects the catalytic behavior. The increases in the reduction temperature produce an increase in the conversion of
n-dodecane and a slight increase in the selectivity to isomerization. However, at higher reduction temperatures, the effect is not clear. The combination of both effects is clearly shown in the i-C
12 yield; the yield increases reach a maximum (i-C
12 yield = 58% for PtW/Al, 30% for PtW/ZrC and 26% for PtW/Zr) for a reduction temperature of 350 °C and decreases for the highest reduction temperature (
Figure 6).
This behavior can be related to the reduction in WO
3 species. Pt/WOx/ZrO
2 properties were previously studied, and the peaks observed above 300 °C in H
2-TPR were shown to correspond to the reduction of tungsten oxide species [
28]. Another group indicated that, in the reduction profiles (H
2-TPR) of WO
3 species, three different reduction peaks can be identified, with the first peak at 300–500 °C corresponding to WO
3 → WO
2.
9 [
27]. This result likely occurred because the loss of acidity creates a loss in the activity, and, for this reason, the best reduction temperature is below 400 °C. Consequently, this partial reduction slightly reduces the acidity of the catalyst and then the activity.
All catalysts are active in the hydroisomerization of
n-dodecane. The conversion of
n-dodecane presents the following trend: PtW/Al > PtW/ZrC > PtW/Zr, with high differences among the average conversions obtained of 67%, 37%, and 34% (
Figure 7), respectively. The selectivity to isomers (
Figure 7) is high and similar for the three catalysts (selectivity to C
12 ~ 80%, selectivity to C
11 ~ 10–13% and selectivity to C
7−10 ~2–7%).
The clearly higher catalytic activity of alumina-supported catalysts can be related to their higher surface area and acidity, which are higher than those of zirconia-supported catalysts [
17]. In addition, catalysts based on commercial tungstated zirconia, which also have a higher surface area than zirconia catalysts, show a higher conversion than other zirconia-based catalysts [
38]. This higher surface area for PtW/ZrC catalyst also causes a higher surface density of polytungstic species responsible for proton generation from H
2, acting as active sites in isomerization [
38].
The higher catalytic activity for alumina-based materials can be related also to the higher acidity observed by TPD (
Figure 3) in the PtW/Al catalyst, especially in high-strength acid sites. The presence of strong Lewis sites (finely dispersed WO
3 particles) facilitates the formation of these protonic sites from H
2 [
39,
40]. The comparison of zirconia-based samples reveals a higher isomerization selectivity found for the catalyst PtW/ZrC, which has a higher proportion of tetragonal zirconia in this catalyst and is generally considered to be active phase for isomerization reaction [
41].