Cuixian
Yang
a,
Andrew R.
Teixeira
a,
Yanxiang
Shi
a,
Stephen C.
Born
a,
Hongkun
Lin
a,
Yunfei
Li Song
b,
Benjamin
Martin
c,
Berthold
Schenkel
c,
Maryam
Peer Lachegurabi
a and
Klavs F.
Jensen
*a
aDepartment of Chemical Engineering, Massachusetts Institute of Technology, Cambridge, MA 02139, USA. E-mail: kfjensen@mit.edu
bDepartment of Chemical Engineering and Biotechnology, University of Cambridge, Cambridge, UK
cNovartis Pharma AG, Chemical and Analytical Development, 4002, Basel, Switzerland
First published on 19th January 2018
Recent advancements in micro-flow technologies and a drive toward more efficient, greener and safer processes have led to a renaissance in flow-chemistry for pharmaceutical production. In this work, we demonstrate the use of a stabilized Pd nanoparticle-organic-silica catalyst to selectively catalyze the hydrogenation of N-4-nitrophenyl nicotinamide, a functionalized active pharmaceutical ingredient (API) surrogate. Extensive catalyst and reactor characterization is provided to establish an in-depth understanding of the unique multiphase dynamics within the micro-packed bed reactor, including the identification of a large liquid holdup (74–84%), rapid multiphase mass transfer (kma > 1 s−1), and liquid residence time distributions. A kinetic analysis has revealed that the surface catalyzed hydrogenation progresses through a condensation mechanism whereby an azo dimer intermediate is formed and rapidly consumed. Finally, a parametric study was performed at various pressures, temperatures, residence times and flow regimes to achieve quantitative chemoselective conversion of the nitroarene to the corresponding primary amine.
Hydrogenation reactions constitute the second most prominent reaction during pharmaceutical industrial API syntheses, representing about 14% of all chemical transformations.13 In comparison to the usage of other costly sacrificial reducing agents such as hydrides (LiAlH4, NaBH4) or borane reagents,14,15 direct hydrogenation of pharmaceutical precursors with hydrogen gas has been identified as “the most atom efficient process”.13 This assertion is owing to commercial and/or on-demand generation availability of H2 gas,16 efficient and low cost downstream separation or recycle by simple gas/liquid phase separation, strong applicability as a green reagent, and minimized formation of undesired by-products.
However, a major challenge for H2 gas-based hydrogenation is the poor solubility of H2 in liquid phase solvents coupled with slow gas–liquid mass transfer limitation.17,18 Packed-bed reactors (PBR) are a viable option for overcoming this barrier with their good gas–liquid–solid mass transfer,19 capability of in situ catalyst regeneration/recyclability, and relatively low catalyst/substrate charge ratio. By moving to micro-packed bed reactors (μPBRs), characterized by the 10–100 micron scale interstitial channels, the risks associated with pressurized gas/solvent mixtures are further mitigated by localizing the pressurization region.20 Additionally, by achieving high mass transfer between the two phases, hydrogen flow is restricted to nearly stoichiometric amounts and result in the rapid dissolution with little excess volume of pressurized gas. Dominant surface tension effects (capillary forces) at small scales transition the hydrodynamics of gas–liquid–solid multiphase micro-system from classical trickle-bed reactors to high liquid holdup systems.21
In this study, a micro-packed bed flow system is developed for hydrogenation of N-4-nitrophenyl nicotinamide to form primary amine directly using hydrogen gas as a reductant (Scheme 1). Similar nitro reductions are typically performed over precious metal catalysts in slurry reactors22 where transport limitations are often circumvented by simply operating with excess reducing agent for long periods of time. Such batch-wise operations are sub-optimal for the catalytic hydrogenation, and presents key targets for flow chemistry. This study demonstrates the application of direct hydrogenation of a pharmaceutically relevant substrate at high yields over many catalytic cycles, while providing insight into key chemical pathways and physical phenomena in micro-packed catalytic beds.
Hydrogen (HY UHP35) and nitrogen (NI UHP35) gases were supplied at ultra-high purity (>99.999%) by Airgas (Salem, NH, USA). Dimethyl acetamide (DMAc) (HPLC grade, ≥99.9%) was provided by Sigma Aldrich (St Louis, MO, USA).
Organosilica network supported palladium nanoparticles (Prod. #R815-100) were generously provided by SiliCycle® Inc. (Quebec City, G1P 4S6, Canada). The catalyst powder is a sol–gel-entrapped Pd nanocatalyst with highly dispersed Pd nanoparticles. The raw powdered catalyst was sequentially dry- and wet-sieved to a size range of 150–212 μm to ensure uniform packing and reduced pressure drop due to clogging. The Pd loading was measured by dissolution in Aqua regia (HCl:HNO3 = 3:1) followed by Atomic Absorption Spectroscopy (AAS) (Agilent 200 Series AA). Transmission electron microscopy (TEM) and contrast adjusted particle counting were used to quantify palladium nanoparticle size distributions and dispersion. The specific surface area was determined from 40 point nitrogen isotherms obtained with a Quantachrome Autosorb iQ and fitting the standard Brunauer, Emmett and Teller (BET) model (ESI, Fig. S-3†). The Pd active sites for hydrogenation were first reduced with H2 at 100 °C for 2 hours, then titrated with CO at 100 °C using a Quantachrome Autosorb-iQ. The chemisorption method followed the protocol described in the ESI (section S2.3†).
The fixed catalytic bed was contained within a tubular stainless steel reactor vessel comprised of a 1/4 inch diameter stainless steel tube with an inner diameter of 4.6 mm (Fig. 1). To enhance gas–liquid dispersion at the reactor inlet, the gas and liquid streams were combined immediately prior to the bed and fed into a minimal dead volume fitting with integrated 20 μm stainless steel frit. The packed bed was comprised of two sections: a calming chamber (bottom) and an active catalyst bed (upper). The calming chamber was introduced to ensure sufficient gas/liquid mixing, well-developed flow and isothermal heating prior to entrance into the catalytic zone. This region was packed with inert spherical glass beads (75 μm, SigmaAldrich 59200-U) to a depth of about 2 cm with a measured void fraction of 36.3%. The catalyst bed was packed above the calming chamber to the top of the reactor vessel (6 cm), resulting in a bed porosity of 73.2%. Exact μPBR characteristics are provided in Table 1.
Calming Chamber | |
Packing | Glass beads |
Particle size | D p = 75 μm |
Bed weight | 0.522 g |
Bed height | 2 cm |
Bed volume | 0.33 ml |
Void fraction | 36.3% |
Catalyst Bed | |
Catalyst | Pd/silica (Silicycle) |
Particle size | 150 μm < Dp < 212 μm |
Catalyst weight | 0.431 g |
Catalyst bed height | 6 cm |
Empty volume | 0.98 mL |
Catalyst volume | 0.26 mL |
Void fraction | 73.2% |
First, external mass transfer of hydrogen molecules from the gas to liquid to solid is considered. To characterize the transport timescale in the system, the catalytic hydrogenation of α-methylstyrene to cumene was investigated, as described in similar systems.25 This reaction was considered due to the well-known and fast intrinsic reaction kinetics enabling the study of H2 mass transfer inside the reactor. To most closely match experimental conditions, the α-methyl styrene hydrogenation was performed in DMAc solvent at 100 °C under 150 psi pressure with various flow conditions to mimic reaction conditions. Steady state profiles were fitted to standard reaction-transport models (section S3.2, ESI†), and overall mass transfer coefficient of H2 are reported to be between 1.0–5.4 s−1, as summarized in Table 2. This range falls within the expected regime reported for similar systems.26
Liquid [mL min−1] | Gas [sccm] | (kma)GLS [s−1] |
---|---|---|
0.4 | 12 | 1.0 |
0.4 | 36 | 2.3 |
0.4 | 60 | 2.5 |
0.8 | 24 | 2.1 |
1.2 | 36 | 3.2 |
1.6 | 48 | 4.3 |
2.0 | 60 | 5.4 |
Potential diffusion limitations within the porous media were evaluated by calculating the Weisz modulus (Mw), which ratios the effective reaction time and the diffusion time within the catalyst particle. The modulus was determined for both hydrogen and the starting material from the apparent reaction rate (experimental) and effective diffusivity (calculation by Wilke–Chang correlation27), as shown in Table S-1 in ESI.† The values for the Weisz modulus were determined to be 0.125 and 0.689, for H2 and N-4-nitrophenyl-nicotinamide, respectively, indicating only minor contributions from intraparticle diffusion.28
Linear calibration curves for determining the concentration of reactant (A) and product (P) (Scheme 1), were constructed by plotting the peak area versus the concentration of all standard compounds. Reactant A was characterized at maximum absorbance peak position of 330 nm, while product P was analyzed at 265 nm. The solutions were diluted 20 times to be within the linear detection range. The conversion and product yields at steady-state under each flow condition were calculated referenced to the original concentration of the starting material (0.1 mol L−1). Yield was determined as the concentration ratio of the final product concentration to the initial starting material.
Reaction intermediates observed by HPLC-MS were further separated by preparative thin layer chromatography (TLC) using a mixture of dichloromethane/methanol (4:1) as the mobile phase. Component fractions were extracted, dissolved in dichloromethane/methanol (4:1) and analyzed with NMR (Bruker AVANCE III HD b400) for identification. The sample mixture was also confirmed by TLC interface (CAMAG) with MS (Advion, expression CMS). See section S5 of the ESI† for detailed characterization methods.
Fig. 2 Catalyst characterization. (a) TEM of 6 nm Pd nanoparticles on silica support, (b) 300 μm single particle micrograph. |
Characterization | Value | Units | Method |
---|---|---|---|
Surface area | 640 | m2 g−1 | BET |
Pd loading | 0.55 | wt% | AAS |
Pd surface area | 0.25 | m2 g−1 | CO chemisorption |
Pd nanoparticle diameter | 6 | nm | TEM |
Catalyst density | 0.463 | g mL−1 | SiliCycle analysis |
Pore volume | 0.88 | mL g−1 | BJH model |
Pore diameter | 5.4 | nm | BJH model |
The Pd–silica catalysts life is extremely important for the practical use of packed bed reactors. The Pd–silica catlaysts in packed bed reactors can be readily regenerated in situ by flowing air to burn off the accumulated coke and then by hydrogen to reduce Pd for the next reaction cycles. (ESI, section S6†).
As shown in Fig. 3(a) and (b), increasing gas-to-liquid flow rate ratios results in improved conversion and selectivity under all four pressure conditions studied. Lower ratios of gas to liquid velocities α did not provide sufficient gas flow to obtain the desired catalytic performance. At pressure of 75 and 100 psi, ratios of α = 3.8 were required to achieve this optimal operating criteria, while at high pressure (150 psi), this criteria was nearly met even at α = 1.9. This high conversion at elevated pressure is directly attributed to the enhanced solubility of H2 in DMAc under higher pressures in accordance with Henry's law.29 At lower pressure, higher gas flow rates are required to overcome the interfacial mass transfer limitations.
Additionally, the complex three-phase hydrodynamics and interfacial mass transfer within micro-packed beds are known to be highly dependent on the flow and pressure conditions.21 Specifically, transition away from the classical trickle-bed regimes is observed with large liquid hold-up and preferential gas-channelling in the small systems. In our study, by tuning the ratio of superficial gas velocity to superficial liquid velocity (α = uG/uL), however, it is possible to decrease liquid holdup, and enhance gas–liquid mass transfer. Evidence of regime changes from stable (mostly liquid) to chaotic flow (more pulsation) is observed in substantial deviations in pressure drop characteristics under varied flow conditions (section S7, ESI†).
Over precious metal catalysts, the mechanism for small molecule nitroarene hydrogenation has been discussed in detail by Corma et al. and shown to potentially progress through several competitive pathways.30,31 In the first mechanism (direct), two consecutive fast hydrogenations of the nitro group to the nitroso and hydroxyl-amine compounds occur before undergoing the slow final reduction to the primary amine. In contrast, the second mechanism (condensation) circumvents the slow step by condensing the two hydrogenation products into an azoxy compound which can be more easily deoxygenated and reduced before undergoing a final cleavage to form two monomeric primary aromatic amines. A similar mechanism is proposed here (Scheme 2), whereby the starting material (A) undergoes either three consecutive direct hydrogenations (top pathway) or proceeds by dimerization and consecutive hydrogenation (bottom pathway).
A single dominant, stable intermediate was observed to accumulate, especially at low conversion with low yield to the desired primary amine product. The molecule was identified by mass spectrometry to have a parent peak with m/z = 438 and confirmed to be the dimeric azoxy compound (D) by isolation by TLC and subsequent NMR (ESI section S5†). This is consistent with established mechanisms observed with nitroarene hydrogenation.30,32,33
The reaction in the micro-packed bed reactor was operated under flow conditions giving rise to operation with several residence times while maintaining constant gas-to-liquid ratio, pressure and temperature. Concentrations of the unreacted starting material (A), azo intermediate (D) and primary amine product (P) were quantified using HPLC with total mass balance closures >93% for all residence times examined. Notably, no appreciable amounts of species (B) and (C) were detected, as is consistent with the expected fast kinetic steps.30 Concentration profiles of each species are plotted versus mean liquid residence time in Fig. 4. It is observed that as the residence time is increased there is a drop in the reactant concentration with a simultaneous increase in the concentrations of the intermediate dimer and product at steady state. The dimer that accumulates at short residence times, however reacts to completion to form product (P) at higher residence times. Such profiles are typical for irreversible reactions progressing through a stable intermediate, indicating that the reaction mechanism at least in part progresses through the lower reaction pathway.
To quantify the relative contributions of the two kinetic pathways to the overall production rate of product P, a simplified version of Scheme 2 (kinetic model, inset Fig. 4) describing the reactant (A), azo intermediate (D) and primary amine product (P) was developed and applied to a dispersion-reaction packed bed reactor model. The full derivation is shown in the ESI (section S8†).
The resulting molar fluxes indicate that the relative reaction flux to the product predominately passes through the reaction intermediate D (88%). The lumped kinetic rate constants from kinetic flux analysis are determined to be k1 = 0.31 min−1, k2 = 2.25 min−1, k3 = 11.07 min−1. This result indicates that the dominant reaction pathway for liquid-phase hydrogenation of the nitro group in N-4-nitrophenyl nicotinamide progresses through an azo-dimer formation before cleaving to two reduced primary amines. However, this pathway alone cannot describe the experimentally observed kinetics, indicating that competitive progression through the direct catalytic pathway is likely.
To achieve more rapid catalytic turnover with high product yields, it is desirable to operate hydrogenation reactions at high temperatures (>200 °C). However, reactors operating at such temperatures may demonstrate relatively slower mass transfer limitations, or diminished product selectivity due to the increased rate of secondary hydrogenations. Although both reaction conversion and transport rates benefit from the increase of temperature, reaction kinetics are known to be strongly activated, increasing exponentially with temperature in accordance with the Arrhenius relationship:
krxn ∝ exp (−Ea/RT) |
Reactions were performed at temperatures from 25–100 °C at constant superficial gas to liquid ratios of 2.9 and pressure of 150 psig. At each temperature, apparent rates were calculated according to eqn (S15)† and apparent rate constants were extracted and plotted for the various temperatures (Fig. 5(b)). The data showed strong agreement with the Arrhenius relationship, demonstrating a constant activation energy of Ea = 48.4 ± 3.0 kJ mol−1. This value represents a single rate limiting activated reaction step, with a magnitude typical of bulk supported and network stabilized Pd (Ea = 43–45 kJ mol−1).34–36 Additionally, values for apparent rate constants are substantially slower than the fast mass transfer (Table 2 and ESI section S3†). Furthermore, activation energies are substantially higher, again affirming that our observed rate limitation is not due to transport limitations, but rather a reaction limitation.
By carefully tuning pressure, residence time and temperature, quantitative conversion and selectivity are realized for the hydrogenation of N-4-nitrophenyl nicotinamide to N-4-aminophenyl nicotinamide, as demonstrated at elevated temperatures in Fig. 5(c).
Footnote |
† Electronic supplementary information (ESI) available: Synthesis, characterization and experimental methods, supporting experiments and model derivations. See DOI: 10.1039/c7gc03469e |
This journal is © The Royal Society of Chemistry 2018 |