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	<title>catalyst deactivation &#8211; Science</title>
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	<title>catalyst deactivation &#8211; Science</title>
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		<title>Methanol Catalyst Defies Textbook Rules as Its Crystals Grow Faster Than Theory Predicts</title>
		<link>https://scienmag.com/methanol-catalyst-defies-textbook-rules-as-its-crystals-grow-faster-than-theory-predicts/</link>
		
		<dc:creator><![CDATA[Bethany Barker]]></dc:creator>
		<pubDate>Wed, 07 Oct 2026 08:46:33 +0000</pubDate>
				<category><![CDATA[Chemistry]]></category>
		<category><![CDATA[catalyst aging prediction models]]></category>
		<category><![CDATA[catalyst deactivation]]></category>
		<category><![CDATA[catalyst deactivation under high temperature]]></category>
		<category><![CDATA[challenges to classical crystal growth laws]]></category>
		<category><![CDATA[co-precipitation]]></category>
		<category><![CDATA[copper crystallites]]></category>
		<category><![CDATA[copper-zinc oxide-alumina catalyst behavior]]></category>
		<category><![CDATA[crystal growth kinetics in catalysis]]></category>
		<category><![CDATA[crystallite growth]]></category>
		<category><![CDATA[Cu/ZnO/Al2O3 catalyst]]></category>
		<category><![CDATA[Cu/ZnO/Al2O3 catalyst deactivation]]></category>
		<category><![CDATA[growth kinetics]]></category>
		<category><![CDATA[heterogeneous catalysis in methanol production]]></category>
		<category><![CDATA[impact of catalyst structure on activity]]></category>
		<category><![CDATA[industrial catalysts lifespan]]></category>
		<category><![CDATA[Methanol catalyst crystal growth]]></category>
		<category><![CDATA[methanol synthesis]]></category>
		<category><![CDATA[nanometer-scale catalyst preparation]]></category>
		<category><![CDATA[nanostructure stability of catalysts]]></category>
		<category><![CDATA[parabolic growth law]]></category>
		<category><![CDATA[sintering]]></category>
		<category><![CDATA[thermal aging]]></category>
		<category><![CDATA[X-ray diffraction]]></category>
		<category><![CDATA[zinc oxide]]></category>
		<guid isPermaLink="false">https://scienmag.com/?p=243849</guid>

					<description><![CDATA[Researchers in China have shown that copper and zinc oxide crystallites in the industrial methanol synthesis catalyst Cu/ZnO/Al2O3 grow with exponents that deviate significantly from the classical parabolic law, and they built validated kinetic equations to predict the catalyst's long-term structural aging.]]></description>
										<content:encoded><![CDATA[<p>One of the most important industrial catalysts on the planet has just revealed that it does not age the way textbooks say it should. The copper-zinc oxide-alumina catalyst, better known in the trade as Cu/ZnO/Al2O3, converts synthesis gas into methanol in chemical plants around the world, and its gradual deactivation under high-temperature operation has puzzled and frustrated engineers for decades. Now a team of researchers in China has systematically tracked how the tiny crystallites that make up this catalyst grow over time, and their findings challenge a century-old law of crystal growth. The work, published in Catalysis Letters, provides the first quantitative kinetic framework tailored specifically to this iconic catalyst system, and it could change how the industry predicts and manages catalyst lifetime.</p>
<p>The story begins with a fundamental problem in heterogeneous catalysis. The Cu/ZnO/Al2O3 catalyst is prepared by co-precipitation, a method that produces an intimate mixture of copper, zinc oxide, and aluminum oxide phases at the nanometer scale. This intimacy is the secret of its activity: copper sites, stabilized and modulated by neighboring zinc oxide, catalyze the hydrogenation of carbon monoxide and carbon dioxide to methanol. But the same nanoscale structure that makes the catalyst active also makes it fragile. At the elevated temperatures of industrial operation, small crystallites tend to coarsen into larger ones, a process called sintering, which reduces the interfacial area between copper and zinc oxide and drains away the active sites. Deactivation by crystallite growth is one of the principal reasons methanol plants must periodically replace their catalyst loads.</p>
<p>Classical materials science describes this coarsening with a deceptively simple relationship known as the parabolic growth law. In its generalized form, the crystallite size raised to a power n grows linearly with time, where n equals 2 for the ideal parabolic case. That value corresponds to a specific physical picture: growth driven purely by capillary forces, with atoms diffusing across a matrix at a rate that scales in a particular way with particle size. Generations of metallurgists and ceramicists have used the parabolic law as a baseline, and deviations from n = 2 are usually taken as signatures of more complex mechanisms, such as grain-boundary pinning by impurities, pore drag, or coalescence events. The classical value is therefore not just a number but a benchmark against which real materials are judged.</p>
<p>The research team, led by Zhenxiang Li and Haodong Tang of Zhejiang University of Technology together with colleagues from Ningbo Fareasttech Catalyst Engineering and Baima Lake Laboratory, decided to test whether the benchmark holds for a real, industrially relevant catalyst. They prepared a co-precipitated Cu/ZnO/Al2O3 catalyst and subjected it to a systematic program of thermal treatments, varying both the temperature and the duration of isothermal aging. Rather than relying on a single characterization snapshot, they measured how the apparent crystallite sizes of two key diffraction planes evolved: the Cu(111) reflection, which tracks the copper metal phase, and the ZnO(101) reflection, which tracks the zinc oxide component. X-ray diffraction, the workhorse technique of crystallite analysis, provided the apparent sizes from the broadening of these diffraction peaks.</p>
<p>What they found was striking. When they fitted their data to a generalized parabolic growth law, the growth exponents for both copper and zinc oxide came out significantly larger than the classical value of 2. In other words, the crystallites in this catalyst do not simply double their size according to the textbook schedule; they grow in a manner that clearly deviates from classical parabolic behavior. This is not a minor correction to an established equation but a qualitative departure, suggesting that the microscopic processes governing coarsening in the co-precipitated catalyst are more complicated than the idealized picture of diffusion-controlled growth. The intimate contact between copper, zinc oxide, and alumina phases, along with the defect-rich structure inherited from the precipitation chemistry, likely creates pathways and barriers that the classical law does not account for.</p>
<p>From these measurements, the team derived apparent kinetic equations for the growth of Cu(111) and ZnO(101) crystallites, each capturing how size evolves with temperature and aging time. These equations are more than descriptive curve fits; they are predictive tools. To test their predictive power, the researchers applied the kinetic models to a scenario of genuine practical importance: long-term operation of the catalyst. They used the equations to forecast how the crystallite sizes would evolve over extended periods and then compared the predictions against X-ray diffraction measurements taken after 50 and 200 hours of operation. The agreement fell within the experimental uncertainty of the measurements, a result that validates the kinetic framework as a quantitative instrument for extrapolating catalyst aging beyond the laboratory timescale.</p>
<p>The implications for the methanol industry are considerable. Catalyst replacement is expensive, and being able to predict structural degradation quantitatively allows plant operators to plan maintenance, optimize operating temperatures, and evaluate new catalyst formulations on a rational basis. The kinetic equations developed here offer a common language for comparing the thermal stability of different Cu/ZnO/Al2O3 preparations, whether modified with structural promoters or synthesized by alternative routes. Recent efforts to double the life of Cu/ZnO catalysts through additives that inhibit sintering, for example, could be benchmarked using precisely this kind of growth-exponent analysis, turning what has often been an empirical trial-and-error exercise into a quantitative science.</p>
<p>The study is also notable for its methodological honesty. The authors are careful to point out that their kinetic analysis rests on X-ray diffraction-derived apparent crystallite sizes, and that the resulting kinetic parameters should be interpreted within the investigated catalyst system and its operating conditions. Apparent crystallite size from XRD is a domain-averaged quantity, and while it is highly practical and reproducible, it may not capture every nuance of microstructural evolution, such as changes in particle morphology or the formation of interfaces invisible to diffraction. By stating these limits explicitly, the team frames their equations as a robust kinetic basis for this system rather than a universal law, an approach that strengthens rather than weakens the work&#8217;s credibility.</p>
<p>The broader scientific context makes the finding even more compelling. Methanol synthesis over Cu/ZnO/Al2O3 remains one of the most intensively studied reactions in catalysis, yet the exact nature of its active sites continues to be debated in the literature, and the catalyst has been called an enigma in comprehensive reviews. As the world pivots toward green methanol produced from carbon dioxide and renewable hydrogen, the demand for durable, well-understood copper-zinc catalysts is only going to grow. Deactivation by sintering is a central obstacle to long-term operation, particularly under the fluctuating conditions that renewable-powered plants may experience. A kinetic model that can quantitatively characterize crystallite coarsening gives researchers a new lever for designing catalysts that resist it.</p>
<p>For now, the message of this study is both simple and profound: even the most familiar industrial materials can defy the classical rules when examined closely enough. By systematically measuring how copper and zinc oxide crystallites grow in a co-precipitated methanol catalyst, and by showing that their growth exponents break decisively from the parabolic ideal, the researchers have opened a quantitative window onto a degradation process that has long been treated qualitatively. The kinetic equations they established, validated against long-duration measurements, promise to help engineers predict catalyst lifetimes and chemists design more stable formulations. In the race to make methanol a cornerstone of a sustainable energy economy, understanding how a catalyst ages may prove just as important as understanding how it works.</p>
<p><strong>Subject of Research:</strong> Crystallite growth kinetics and deactivation of co-precipitated Cu/ZnO/Al2O3 methanol synthesis catalysts</p>
<p><strong>Article Title:</strong> Non-classical Crystallite-Growth Kinetics in a Co-precipitated Cu/ZnO/Al2O3 Catalyst for Methanol Synthesis</p>
<p><strong>Article References:</strong> Li, Z., He, X., Li, Y., Zhao, H., Lv, D., Liu, Z., Li, Y., Peng, B., &amp; Tang, H. (2026). Non-classical Crystallite-Growth Kinetics in a Co-precipitated Cu/ZnO/Al2O3 Catalyst for Methanol Synthesis. <em>Catalysis Letters, 156</em>(11), Article 296. <a href="https://doi.org/10.1007/s10562-026-05542-x" rel="noopener noreferrer">https://doi.org/10.1007/s10562-026-05542-x</a></p>
<p><strong>Image Credits:</strong> AI Generated</p>
<p><strong>DOI:</strong> <a href="https://doi.org/10.1007/s10562-026-05542-x" rel="noopener noreferrer">10.1007/s10562-026-05542-x</a></p>
<p><strong>Keywords:</strong> Cu/ZnO/Al2O3 catalyst, methanol synthesis, crystallite growth, sintering, catalyst deactivation, growth kinetics, X-ray diffraction, parabolic growth law, co-precipitation, thermal aging, copper crystallites, zinc oxide</p>
]]></content:encoded>
					
		
		
		<post-id xmlns="com-wordpress:feed-additions:1">243849</post-id>	</item>
		<item>
		<title>Fe–Ni–Ce Catalysts Tune Carbon Structure in Methane Decomposition</title>
		<link>https://scienmag.com/fe-ni-ce-catalysts-tune-carbon-structure-in-methane-decomposition/</link>
		
		<dc:creator><![CDATA[Bethany Barker]]></dc:creator>
		<pubDate>Sat, 05 Sep 2026 04:02:45 +0000</pubDate>
				<category><![CDATA[Chemistry]]></category>
		<category><![CDATA[carbon nanomaterials]]></category>
		<category><![CDATA[carbon nanomaterials synthesis]]></category>
		<category><![CDATA[carbon structure tuning]]></category>
		<category><![CDATA[catalyst deactivation]]></category>
		<category><![CDATA[catalyst deactivation due to carbon accumulation]]></category>
		<category><![CDATA[catalyst longevity]]></category>
		<category><![CDATA[Catalytic methane decomposition]]></category>
		<category><![CDATA[cerium-promoted catalysts]]></category>
		<category><![CDATA[effects of molybdenum and cerium in methane decomposition catalysts]]></category>
		<category><![CDATA[Fe–Ni–Ce catalyst optimization]]></category>
		<category><![CDATA[Fe–Ni–Ce catalysts]]></category>
		<category><![CDATA[graphitized carbon formation control]]></category>
		<category><![CDATA[graphitized carbon synthesis]]></category>
		<category><![CDATA[high-temperature methane cracking]]></category>
		<category><![CDATA[Hydrogen Production]]></category>
		<category><![CDATA[hydrogen production without CO2 emissions]]></category>
		<category><![CDATA[long-lasting catalysts for hydrogen generation]]></category>
		<category><![CDATA[mixed TiO₂–Al₂O₃ support in methane decomposition]]></category>
		<category><![CDATA[role of cerium as catalyst promoter]]></category>
		<category><![CDATA[solid carbon formation]]></category>
		<category><![CDATA[support materials (TiO₂–Al₂O₃)]]></category>
		<category><![CDATA[tailoring carbon structure via catalyst composition]]></category>
		<guid isPermaLink="false">https://scienmag.com/fe-ni-ce-catalysts-tune-carbon-structure-in-methane-decomposition/</guid>

					<description><![CDATA[In the global race to produce clean hydrogen without pumping carbon dioxide into the atmosphere, one of the most elegant solutions has long remained stubbornly impractical. Catalytic methane decomposition, the process of splitting natural gas into hydrogen and solid carbon at high temperature, promises COx-free hydrogen while simultaneously yielding carbon nanomaterials that can be sold [&#8230;]]]></description>
										<content:encoded><![CDATA[<p>In the global race to produce clean hydrogen without pumping carbon dioxide into the atmosphere, one of the most elegant solutions has long remained stubbornly impractical. Catalytic methane decomposition, the process of splitting natural gas into hydrogen and solid carbon at high temperature, promises COx-free hydrogen while simultaneously yielding carbon nanomaterials that can be sold to offset production costs. The catch has always been the catalyst itself: the carbon it produces eventually chokes the very metal particles that drive the reaction, deactivating the catalyst within hours. Now, researchers Nursaya Makayeva and Gaukhar Yergaziyeva of the Institute of Combustion Problems and Al-Farabi Kazakh National University in Almaty, Kazakhstan, report in Catalysis Letters that the fate of a methane decomposition catalyst can be deliberately steered by the choice of a single chemical promoter, opening a path to catalysts that either run longer for hydrogen production or deliberately manufacture highly graphitized carbon.</p>
<p>The team studied three catalyst formulations built on a mixed TiO₂–Al₂O₃ support: a baseline iron-nickel catalyst (Fe–Ni/TiO₂–Al₂O₃), a cerium-promoted version (Fe–Ni–Ce/TiO₂–Al₂O₃), and a molybdenum- and cerium-containing variant (Fe–Mo–Ce/TiO₂–Al₂O₃). Each catalyst was tested in catalytic methane decomposition reactions at temperatures between 600 and 850 degrees Celsius, both under dry conditions and in the presence of steam, a variable that industrial reactors often cannot avoid. The comparison revealed a striking divergence in behavior. The Fe–Ni–Ce formulation achieved the highest methane conversion of the series, reaching 96 percent at 850 degrees Celsius, and sustained its performance over extended time on stream. The Fe–Mo–Ce catalyst, by contrast, started out highly active but deactivated more rapidly, a decline the researchers traced to the accumulation of heavily graphitized coke on its active surface.</p>
<p>The reason for this divergence lies in the distinct chemistry that cerium and molybdenum introduce to the iron-nickel active phase. Through an extensive characterization campaign combining X-ray diffraction, temperature-programmed reduction by hydrogen (H₂-TPR), temperature-programmed oxidation (TPO), Raman spectroscopy, and thermogravimetric analysis (TGA), the team showed that cerium dioxide acts as an oxygen reservoir within the catalyst. CeO₂ enhances the reducibility of the Fe-Ni phases and boosts the mobility of oxygen species through the material, a property long prized in ceria-based catalysis. Molybdenum behaves differently: it exists as highly dispersed MoOₓ species and substantially alters the redox properties of the system, shifting the way the catalyst exchanges oxygen during the reaction. These changes at the atomic scale cascade upward into macroscopic behavior, determining not just how fast methane is split, but what kind of carbon is left behind.</p>
<p>That last point is the heart of the study. When methane decomposes on a transition metal surface, the carbon it deposits is not a uniform nuisance; it comes in structurally distinct forms ranging from disordered, defective amorphous carbon to well-ordered sp² graphitic phases. Raman spectroscopy, which distinguishes these forms by the relative intensity of the disorder-induced D band and the graphitic G band, together with TGA, which measures how readily the deposited carbon burns off in oxygen, allowed the researchers to correlate carbon structure with catalytic performance. The correlations were unambiguous. Cerium promotes the formation of predominantly ordered sp² carbon structures and, crucially, facilitates the gasification of the defective carbon species that would otherwise encapsulate and poison the active metal particles. Molybdenum does the opposite, favoring the growth of more thermally stable, highly graphitized phases that resist removal.</p>
<p>This insight resolves a long-standing puzzle in the methane decomposition literature. Iron- and nickel-based catalysts have been known for decades to produce filamentous carbon, carbon nanofibers, and carbon nanotubes, and atomic-scale imaging studies have shown how carbon dissolves into the metal particle, diffuses through it, and precipitates as a filament, often lifting the nanoparticle off its support and keeping it alive. But the balance between the &#8220;good&#8221; carbon that grows as filaments and the &#8220;bad&#8221; encapsulating coke that kills the catalyst has been difficult to control. The Kazakh team&#8217;s work suggests that the redox chemistry of the promoter, and the presence or absence of steam, together govern which carbon morphology wins. Oxygen delivered from the ceria lattice can oxidize and remove defective carbon before it matures into pore-blocking coke, while MoOₓ species steer deposition toward graphitized deposits that, once established, are thermally stable and effectively permanent.</p>
<p>Steam proved to be a second, independent lever. In gasification chemistry, water is the classic reagent for burning carbon off metal surfaces, converting solid deposits to CO and CO₂. The researchers tested the catalysts both dry and in the presence of steam and found that steam influences both the type and stability of the carbon deposits, interacting with the redox properties of the promoters in ways their mechanistic model now captures. In a proposed coke formation mechanism, the authors argue that the structure of the carbon deposit is set by the interplay between the oxygen-delivery capacity of the promoter system and the availability of gas-phase oxidants such as steam. Where oxygen transfer is vigorous and defective carbon is rapidly gasified, the catalyst stays clean and functional; where carbon is allowed to graphitize undisturbed, the deposit consolidates and deactivation follows.</p>
<p>The practical implications run in two directions, and the authors are explicit that neither is inherently better. For operators whose goal is maximum, sustained hydrogen output, the Fe–Ni–Ce/TiO₂–Al₂O₃ catalyst is the clear choice: it pairs the highest conversion measured in the study, 96 percent at 850 degrees Celsius, with superior stability over time on stream, precisely because its ceria component keeps the carbon deposit from hardening into a fatal overlayer. For a laboratory or industrial partner seeking to co-produce graphitic carbon materials, whether for battery anodes, conductive additives, or other applications where ordered graphitic carbon commands a premium, the Fe–Mo–Ce formulation is attractive despite its faster deactivation, because it manufactures exactly the kind of thermally stable, graphitized carbon that commands value. The same chemistry, in other words, can be tuned toward either product simply by choosing the promoter and adjusting the atmosphere.</p>
<p>This tunability matters because hydrogen economics are brutal. Conventional steam methane reforming, the dominant hydrogen production route today, emits carbon dioxide as an unavoidable byproduct, roughly 9 to 12 kilograms of CO₂ per kilogram of hydrogen in unmitigated plants, and requires extensive downstream gas separation to purify the hydrogen. Catalytic methane decomposition sidesteps both problems: the reaction CH₄ → C + 2H₂ is mildly endothermic, yields a hydrogen stream that needs no CO₂ scrubbing, and locks the methane&#8217;s carbon into a solid. If that solid is a high-quality nanostructure rather than a worthless soot, the economics shift further, since carbon nanotubes and graphitic carbons can sell for orders of magnitude more per kilogram than the hydrogen itself. The Kazakh results feed directly into this &#8220;two products from one molecule&#8221; strategy by showing how to make the carbon saleable on demand.</p>
<p>The work also carries technical lessons for catalyst design beyond the specific Fe–Ni system. The TiO₂–Al₂O₃ mixed support provides both mechanical stability and electronic interaction with the active metal phases, and the characterization data show that the promoters do not act in isolation. XRD revealed the crystalline phases present in the fresh and spent catalysts, while H₂-TPR quantified how easily the metal oxides were reduced, a proxy for the catalyst&#8217;s readiness to activate methane. TPO profiles of the spent catalysts, showing at what temperature the deposited carbon oxidizes, provided a direct read on carbon reactivity that matched the Raman evidence: cerium-containing spent catalysts burned off carbon at lower temperatures, consistent with a higher fraction of defective, gasifiable species, while the Mo-containing samples required more aggressive conditions, consistent with graphitized deposits. The methodological point, that Raman and TGA data taken together can predict catalyst deactivation behavior, is itself a contribution that other groups can adopt.</p>
<p>The research was carried out with support from the Ministry of Science and Higher Education of the Republic of Kazakhstan under scientific project AP25793961, which is devoted to developing inexpensive, highly efficient composite materials for hydrogen and nanocarbon production from methane. It reflects a broader push among methane-rich nations to convert a fossil feedstock into a low-carbon energy carrier without waiting for expensive carbon capture infrastructure. The Almaty team&#8217;s contribution is a design principle rather than a single recipe: the redox character of the promoter, cerium for oxygen mobility, molybdenum for graphite-favoring conditions, and steam as a modulating agent, is the control knob that determines whether a methane decomposition catalyst lives long or produces graphite.</p>
<p>Whether the approach survives scale-up remains to be seen. Industrial methane pyrolysis demands catalysts that survive thousands of hours, tolerate sulfur impurities in natural gas, and allow continuous removal of accumulating carbon, and no laboratory result yet guarantees that. But the demonstration that a 96 percent methane conversion can be sustained on a ceria-promoted iron-nickel catalyst, and that the same platform can be redirected toward graphitic carbon synthesis by swapping in molybdenum, gives process engineers something they have largely lacked: a rational, mechanistically grounded way to choose their catalyst based on which product they want more. In a field where the hydrogen and the carbon have always pulled in opposite directions, that may be the most valuable result of all.</p>
<p>The study appears in Catalysis Letters as volume 156, article 271.</p>
<div class="scienmag-article-metadata"><strong>Subject of Research:</strong> Catalytic methane decomposition over Fe–Ni–Ce and Fe–Mo–Ce/TiO₂–Al₂O₃ catalysts, examining how cerium and molybdenum promoters tune carbon deposit structure, coke formation, and catalyst stability for COx-free hydrogen production and carbon nanomaterial synthesis.</p>
<p><strong>Article Title:</strong> Methane Decomposition Over Fe–Ni–Ce and Fe–Mo–Ce/TiO₂–Al₂O₃ Catalysts: Tuning Carbon Structure and Catalyst Stability</p>
<p><strong>Article References:</strong> Makayeva, N., &amp; Yergaziyeva, G. (2026). Methane Decomposition Over Fe–Ni–Ce and Fe–Mo–Ce/TiO₂–Al₂O₃ Catalysts: Tuning Carbon Structure and Catalyst Stability. <em>Catalysis Letters, 156</em>(10), Article 271. <a href="https://doi.org/10.1007/s10562-026-05508-z" target="_blank" rel="noopener noreferrer">https://doi.org/10.1007/s10562-026-05508-z</a></p>
<p><strong>Image Credits:</strong> AI Generated</p>
<p><strong>DOI:</strong> <a href="https://doi.org/10.1007/s10562-026-05508-z" target="_blank" rel="noopener noreferrer">10.1007/s10562-026-05508-z</a></p>
<p><strong>Keywords:</strong> catalytic methane decomposition, COx-free hydrogen production, Fe–Ni catalysts, cerium oxide promoter, molybdenum promoter, coke formation, graphitized carbon, Raman spectroscopy, thermogravimetric analysis, TiO₂–Al₂O₃ support, catalyst deactivation, carbon nanostructures</p>
</div>
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