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In this work, we have studied the superhydrophobicity and buoyancy of two types of nanostructured surfaces: the cabbage leaf and a vertically aligned carbon nanotubes (VACNTs) carpet. The wettability of these surfaces were characterized by contact angle, tilting angle, sliding volume and sliding speed measurements. The results were correlated to the related surface topologies, which were investigated by scanning electron microscopy. Buoyancy of different surfaces has been investigated through measurements of the forces acting on the surface. Finally, we demonstrate that cabbage leaves and VACNT carpets have some common features with the water strider’s leg, better understanding the mechanisms of buoyancy related to the structural shape and size of natural or artificial nanostructures.
Patterned porous films prepared by the breath figure method have received considerable interests because of the potential applications. This paper reports a top–down method to fabricate functional patterned films. Cross-linked polystyrene microspheres were synthesized by a two-stage dispersion polymerization using divinylbenzene (DVB) and ethylene glycol dimethacrylate (EGDMA) as cross-linkers, which provide free vinyl groups on the microspheres surface. The amounts of residual vinyl groups were determined by potentiometric titration. Glucose was then bound to the microspheres via thiol–ene reaction, which was confirmed by x-ray photoelectron spectroscopy and water contact angle measurements. Results indicate that vinyl groups of EGDMA show relatively higher reactivity than that of DVB. Microspheres with glucose were assembled into the pores of honeycomb films prepared by the breath figure method, forming functional arrays for recognizing a lectin, Con A. This top–down method is useful in preparing patterned films with various functional moieties, which may act as a platform, such as, for investigating carbohydrate–lectin interactions and for sensing.
The paper established a model to investigate the interaction between the special rotational deformation and a semielliptical blunt crack in deformed nanocrystalline materials. By using the complex variable method, the effect of a disclination quadrupole produced by the special rotational deformation on the emission of lattice dislocation from a semielliptical blunt crack tip was explored theoretically. The complex form expression of the dislocation force was derived, and the critical stress intensity factors (SIFs) for the first edge dislocation emission were calculated. Then, the influence of the disclination strength, the disclination location and orientation, the special rotational deformation orientation, the grain size, and the curvature radius of blunt crack tip on the critical SIFs were discussed in detail, and a comparison with the sharp crack behavior was presented. The results show that the special rotational deformation and the curvature radius of blunt crack have great effects on the lattice dislocation emission form blunt crack tip. Some influence laws are also different with those of the edge dislocation emission from a sharp crack tip.
We present results of a molecular dynamics study using adaptive intermolecular reactive empirical bond order interatomic potential to analyze thermal transport in three-dimensional pillared single-walled carbon nanotube (SWCNT)–graphene superstructures comprised of unit cells with graphene floors and SWCNT pillars. The results indicate that in-plane as well as out-of-plane thermal conductivity in these superstructures can be tuned by varying the interpillar distance and/or the pillar height. The simulations also provide information on thermal interfacial resistance at the graphene–SWCNT junctions in both the in-plane and out-of-plane directions. Among the superstructures analyzed, the highest effective (based on the unit cell cross-sectional area) in-plane thermal conductivity was 40 W/(m K) with an out-of-plane thermal conductivity of 1.0 W/(m K) for unit cells with an interpillar distance Dx = 3.3 nm and pillar height Dz = 1.2 nm, while the highest out-of-plane thermal conductivity was 6.8 W/(m K) with an in-plane thermal conductivity of 6.4 W/(m K) with Dx = 2.1 nm and Dz= 4.2 nm.
The topic of catalysis recurs throughout fuel chemistry. A catalyst increases the rate of a chemical reaction without itself being permanently altered by the reaction, or appearing among the products. The key word is rate. Catalysts affect reaction kinetics. A catalyst affects reaction rate by providing a different mechanism for the reaction, usually one that has a markedly lower activation energy than that of the non-catalyzed reaction. Catalysts do not change reaction thermodynamics; they do not alter the position of equilibrium [A], but they can help reach equilibrium much more quickly. And, they cannot cause a thermodynamically unfavorable reaction to occur.
Catalysts can be classified as homogeneous, in the same phase as the reactants and products, and heterogeneous, in a separate phase. Homogeneous catalysts mix intimately with the reactants. This good mixing often leads to enormous rate enhancements, in some cases by more than eight orders of magnitude. But, because they are in the same phase as the reactants and products, industrial use would require a separation operation for catalyst recovery downstream of the reaction, unless one were willing to throw away the catalyst (possibly allowing it to contaminate the products) as it passes through the reactor. For many catalytic processes, the catalyst costs much more than the reactants do, so loss of the catalyst would result in a significant economic penalty. Usually, heterogeneous catalysts have no major separation problems, thanks to their being in a separate phase from reactants and products. However, because of their being in a separate phase, mass-transfer limitations can hold up access of the reactants to the catalyst, or hold up departure of products. Heterogeneous catalysis can also be affected by various problems at the catalyst surface (discussed in Chapter 13). Large-scale industrial processing almost always favors use of heterogeneous catalysts, to avoid possibly difficult downstream separation issues. Nevertheless, steady progress is being made in finding ways to overcome separation problems with homogeneous catalysts, including, as examples, membrane separation, selective crystallization, and use of supercritical solvents.
Evidence that Earth is heating is incontrovertible. Glaciers and permafrost are melting. Sea level is rising. Deserts are spreading. Growing seasons are getting longer in far northern latitudes. Migratory species arrive at their summer breeding grounds earlier and remain later. Animals, including some of the less-pleasant snakes and disease-carrying insects, are increasing their ranges. Meteorological records show that the past decade has been the warmest on record. So many independent observations from different areas of science make an exceptionally strong case that a real effect is occurring.
Like any other system, temperatures on Earth are governed by a simple heat balance:
(Heat in)–(Heat out) = (Heat retained in system).
Several sources provide heat. These include incoming solar radiation, heat generated by human activity, and heat from decay of radioactive species in the Earth’s interior. Of these, solar radiation dominates, by far. It is estimated that the entire yearly energy needs of all of humankind could be met by capturing and converting all of the solar energy falling on Earth for about 45 minutes. Heat is lost primarily by radiative heat transfer back into space, much in the infrared. The balance between heat coming in, mainly solar energy, and heat going out, mainly infrared radiation to space, maintains the average global temperature. Any change in either term necessarily results in a change in the amount of heat retained, which in turn eventuates in a change in average global temperature. Because temperature has a major role in affecting climate, the net effect is a change in global climate.
To explore the relationships between microstructure and growth direction, metallic A-type antiferromagnetic and anisotropic magnetoresistant Nd0.45Sr0.55MnO3 (NSMO) thin films were grown on SrTiO3(110) by pulsed laser deposition method and characterized by (scanning) transmission electron microscopy. The interface between NSMO and SrTiO3 (110) is flat and sharp. The NSMO thin films exhibit a two-layered structure: a continuous perovskite layer epitaxially grown on the substrate followed by an epitaxially grown columnar nanostructure [Fig. 1(a)]. High-density stacking faults were found in the nanostructured layer with an in-plane translational displacement of 1/2a<111>, accompanied by 1/2a[001] partial dislocations or (110) antiphase boundaries (APBs). These stacking faults terminate either at pores or in the grain matrix to eliminate (1$\bar 1$0) APBs. The formation mechanisms of the nanostructured NSMO films and the relevant stacking faults are discussed from the viewpoint of both film growth and specific substrate direction.
Among the fossil fuels, the progression from natural gas to petroleum to coal is one of increasing complexity. Even a wet, sour gas has only a small number of possible components. Once the gas has been treated and purified for distribution to consumers, it typically contains >90% of a single compound, methane. Gas contains no inorganic impurities that might leave an ash residue on combustion. Petroleum usually is a homogeneous liquid with a narrow range of elemental composition – about 82–87% carbon, 12–15% hydrogen and the balance nitrogen, sulfur, and oxygen – with atomic H/C ratio of ≈1.5–1.8. On a molecular level, petroleum contains thousands of individual compounds, every one of which could be separated, at least in principle, using common techniques of the organic chemistry laboratory, and identified [A]. Inorganic ash-forming constituents are commonly less than 0.1%. In contrast, coals have an extremely wide range of composition, some 65–95% carbon, 2–6% hydrogen, up to about 30% oxygen, and possibly several percent each of sulfur and nitrogen. The H/C ratio is less than 1. Coals are opaque, heterogeneous solids. Coals cannot be distilled reversibly. Coals are not completely soluble in any solvent, and even the partial solubility in various solvents is an extraction of components rather than a true, reversible dissolution process. Coals have a macromolecular structure that varies from one coal to another and that has never been completely elucidated for any coal. Coals contain a variable, but appreciable, amount of inorganic material, so that burning a particular coal leaves an ash residue that represents anywhere from a few percent to over 25% of the original weight of the coal. Coals also contain some variable amount of water as they are mined from the Earth, from several percent to about 70%.
Despite the complexity of coals and the difficulties encountered in studying them, systems for classifying and describing coals are nevertheless needed. Such systems can provide a conceptual framework for organizing knowledge of coal composition and properties. In a very practical sense such systems provide the descriptions needed for legally binding buying and selling of coals.
Virtually all substances of interest in fuel chemistry consist of covalently bonded molecules. Many are hydrocarbons in the literal sense of the word – compounds containing only hydrogen and carbon atoms. Others contain one or more heteroatoms, i.e. atoms of oxygen, nitrogen, or sulfur. Physical properties of fuels have numerous important roles in fuel technology and utilization, e.g. boiling point, because distillation is commonly used for separations; density, because the amount of fuel that can be carried on vehicles or aircraft is limited by volume and not by mass; and viscosity, because we need fluids to flow, or to be pumped, from place to place. An understanding of how chemical composition and molecular structure influence physical properties shows that the properties of substances do not come about by some haphazard chance but rather because of fundamental links between composition, structure, and properties. Further, such links provide useful guidelines or rules of thumb for estimating expected properties from composition, or vice versa.
The most noticeable property of most substances is their physical state: solid, liquid, or gaseous. The first point of inquiry becomes that of why molecules form solids or liquids at all. Why isn't everything a gas? To exist in a condensed phase, i.e. as a liquid or solid, there must be attractive forces among molecules strong enough to hold them in proximity.
Hydrogen and carbon monoxide are readily combustible with high calorific values (–286 and –283 kJ/mol, respectively). Although the name synthesis gas reflects its intended use in subsequent operations for production of other fuels or chemicals, no technical issues prevent use of products of gasification (or partial oxidation or steam reforming) directly as fuels. Such products can be used for domestic heating and cooking, for process heat, or for raising steam in industry. Many countries had, at one time, significant infrastructure for making and distributing fuel gases from coal. Indeed, until the development of syntheses based on CO and H2, in the early decades of the last century, the whole purpose of converting coal to gas was for domestic or industrial heating and illumination. Current interest focuses on use of synthesis gas as fuel in IGCC plants.
Water gas, town gas, illuminating gas, and related fuels made from early coal conversion processes, as well as the products of oxygen-blown gasifiers, have calorific values in the range 11–19 GJ/m3. Table 21.1 compares calorific values of some gases produced from coal with hydrogen, methane, and LPG.
A problem with some of these products is the high toxicity of carbon monoxide. Many gas-fired domestic appliances, such as water heaters or stoves, were equipped with pilot lights, in which a small quantity of gas was always being burned. Then, when the gas was turned on to the main burner or heater, it would be ignited by the pilot light, without a need to find matches. This bit of convenience for the householder, however, meant that if anything should cause the pilot light to go out, a small quantity of gas was now being emitted directly into the home.
In practical industrial processing, reactions must take place on time scales reasonably short from a human perspective – ideally in units of hours, at the most. Compared to natural geological processes, reaction times need to be reduced by up to ten orders of magnitude. Two approaches can do this. One is to increase reaction severity, usually increasing temperature. As a rough rule, reaction rate doubles for every 10 K increase in temperature. The highest temperature encountered in fuel formation is ≈225 °C, the closing of the gas window or the fourth coalification jump. Temperatures of fuel processing are often much higher, and reaction rates are correspondingly higher. The second approach is to use a catalyst to enhance reaction rate. Of course, in many situations both strategies are used together.
A catalyst changes the rate, outcome, or both, of a reaction without appearing in the net equation for the reaction (i.e. without being consumed in the reaction, or being permanently altered by the reaction). Although catalysts often find use to enhance rate, sometimes they are used to arrive at a different set of products. This is very important in, e.g., the production of high-quality gasoline (Chapter 14). As materials, catalysts are of extreme importance. Virtually all biochemical processes in living organisms are catalyzed by enzymes. About 90% of the fuels, synthetic chemicals, and plastics produced by the chemical industry have benefited from a catalyst in at least one of their processing steps.
Chapter 2 introduced the concept of catalysis, and focused on homogeneous catalysis. For large-scale production of commodities such as fuels, a homogeneous catalyst requires separation and recovery steps downstream of the reactor, unless the catalyst either is thrown away or is allowed to dilute or contaminate the product. This adds to the complexity and expense of a process. Heterogeneous catalysts are favored by industry, especially for production of commodities. In part, this derives from a very easy, even non-existent, separation from the process stream. Many heterogeneous catalysts can withstand more severe conditions of temperature and pressure than homogeneous catalysts, especially enzymes. Heterogeneous catalysts work well for gas-phase reactions, where it might be difficult to select a homogeneous catalyst [A].
Natural gas is a mixture of hydrocarbons with various quantities of non-hydrocarbons, which exists either in the gas phase or in solution with petroleum in natural underground reservoirs. The principal hydrocarbon component is methane. In most parts of the world, by the time the gas has been treated and distributed to consumers, it consists almost entirely of methane.
Gas produced during catagenesis usually migrates through porous rocks in the Earth's crust until it encounters a formation of non-porous rock. This non-porous rock prevents further migration of the gas, effectively trapping it in the porous rock below. The porous rock becomes a reservoir for the gas. The gas can be classified according to how it is found. Associated gas is found in conjunction with accumulated oil, either dissolved in the oil, called dissolved gas, or as a separate gaseous phase above the oil, gas-cap gas. Non-associated gas is found without accompanying oil. A reservoir of non-associated gas could arise from gas migrating to a different location than that to which oil migrated, or from formation of gas in the gas window, i.e. without oil. About 60% of the world's natural gas is non-associated.
Other sources of methane-rich gases occur in nature. Biogenic gas, produced during diagenesis, comes from the action of anaerobic bacteria on accumulated organic matter. Landfill gas is produced in the same way, but differs in that the feedstock is the organic residues of civilization, accumulated as solid waste in landfills. Excrement from humans or other animals also reacts in the same way, providing a useful source of fuel for farms or even domestic use [A]. Methane forms and accumulates in coal seams; its deliberate removal prior to mining provides another source, coalbed methane.
Gasification or partial oxidation is likely to be practiced with one of two purposes: to supply gaseous feed for an IGCC plant, or to use the carbon monoxide/hydrogen mixture as synthesis gas. Neither application uses raw gas with no downstream treatment. The desirable components of the product gas are carbon monoxide, hydrogen, methane, and other light hydrocarbons. If the gas were to be used in combustion applications on site, carbon dioxide and water vapor would be considered neutral, i.e. having neither a positive nor negative effect, except for their effect as diluents of the combustible gases. If the gas is to be upgraded, further processed, or shipped by pipeline, then both of these components are undesirable. Processing units would have to be larger to handle these “extra” components that make no contribution to the calorific value of the gas. Some heat and compression work would be wasted on diluents of the desired components of the gas. Components of the raw gas that are always undesirable include particulate matter, droplets of tar, hydrogen chloride, ammonia, and hydrogen sulfide and other sulfur-containing compounds.
A first treatment step involves removal of particulate matter, which may consist of fine particles of ash or of partially reacted feedstock. This can be accomplished using a cyclone separator. Cyclones can be designed to operate at temperatures to 1000 °C, and pressures to about 50 MPa. They work well for particle sizes above 5 µm. If it is necessary to remove finer particles, baghouses with fabric filters or electrostatic precipitators can be used.
In the progression through the oil window, thermally driven reactions break kerogen and larger hydrocarbon molecules into smaller ones. In a refinery, analogous processes take some of the heavier products and break them into smaller molecules. This shifts the molecular weight downward, increasing the amounts of relatively small molecules boiling in the gasoline range. To operate on a human rather than a geologic time scale requires running at much higher temperatures than are encountered in the oil window. Processes that rely entirely on heat for breaking down large petroleum molecules into smaller ones are called thermal cracking.
With the steady increase in use of automobiles and trucks in the early decades of the past century, market demand for gasoline exceeded what could be supplied by straight-run gasoline, even augmented with natural gasoline. Cracking processes can increase the relative proportion of molecules in the C5–C10 range, at the expense of larger molecules in products having a lower value than gasoline.
Refinery cracking processes are of two types, thermal (that rely entirely on temperature to drive the cracking reactions) or catalytic. Chapter 14 included a discussion of catalytic cracking reactions and processes. Thermal processes were developed starting around 1913. Numerous thermal cracking processes were developed in the early decades of the twentieth century. They helped meet the increasing demand for gasoline in the 1920s and 30s. The process developed by C.P. Dubbs [A] provides an example (see Figure 16.1).