Big Chemical Encyclopedia

Chemical substances, components, reactions, process design ...

Articles Figures Tables About

Gas to Liquid

Qatar is now aggressively building capadty to use its stranded natural gas reserves to produce a very high-quality diesel produd. Two of the largest projects are with Shell and Exxon Mobil. The Shell project, under construction in 2006, is a 6 billion seaside projed on a site approximately 1.4 by 1.6km. Approximately 60000 construction workers are involved - in a country with a population of just 800000. Exxon Mobil s plant is even larger, and will produce about 154 000 barrels per day. It also represents Exxon Mobil s largest single project investment to date (Romero 2006). [Pg.61]

The synthetic crude product is inherently cleaner than its oil-based diesel competitor, which often is high in sulfur. Shell plans to market this cleaner fuel as a means of reducing smog in the world s 27 largest cities (megacities) and the Southern California Air District. [Pg.61]


It must be remembered that, in general, the constants a and b of the van der Waals equation depend on volume and on temperature. Thus a number of variants are possible, and some of these and the corresponding adsorption isotherms are given in Table XVII-2. All of them lead to rather complex adsorption equations, but the general appearance of the family of isotherms from any one of them is as illustrated in Fig. XVII-11. The dotted line in the figure represents the presumed actual course of that particular isotherm and corresponds to a two-dimensional condensation from gas to liquid. Notice the general similarity to the plots of the Langmuir plus the lateral interaction equation shown in Fig. XVII-4. [Pg.624]

As it has appeared in recent years that many hmdamental aspects of elementary chemical reactions in solution can be understood on the basis of the dependence of reaction rate coefficients on solvent density [2, 3, 4 and 5], increasing attention is paid to reaction kinetics in the gas-to-liquid transition range and supercritical fluids under varying pressure. In this way, the essential differences between the regime of binary collisions in the low-pressure gas phase and tliat of a dense enviromnent with typical many-body interactions become apparent. An extremely useful approach in this respect is the investigation of rate coefficients, reaction yields and concentration-time profiles of some typical model reactions over as wide a pressure range as possible, which pemiits the continuous and well controlled variation of the physical properties of the solvent. Among these the most important are density, polarity and viscosity in a contimiiim description or collision frequency. [Pg.831]

Zawadski A G and Hynes J T 1989 Radical recombination rate constants from gas to liquid phase J. Phys. Chem. 93 7031-6... [Pg.869]

For stripping one begins by using the design specification to locate the point Xi, y. Then the iutersecfiou of the vertical huex = X9 with the equilibrium curve y° = F x) defines the theoretical minimum gas-to-liquid ratio. The actual value of is chosen to be about 20 to 50... [Pg.1353]

As shown by Table 14-12, empirical correlations for two-fluid atomization show dependence on high gas velocity to supply atomizing energy, usually to a power dependence close to that for turbulent breakup. In addition, the correlations show a dependence on the ratio of gas to liquid and system dimension. [Pg.1412]

Stripping Air stripping is applied for the removal of volatile substances from water. Henry s law is the key relationship for use in design of stripping systems. The minimum gas-to-liquid ratio required for stripping is given by ... [Pg.2227]

Fischer-Tropsch Synthesis The best-known technology for producing hydrocarbons from synthesis gas is the Fischer-Tropsch synthesis. This technology was first demonstrated in Germany in 1902 by Sabatier and Senderens when they hydrogenated carbon monoxide (CO) to methane, using a nickel catalyst. In 1926 Fischer and Tropsch were awarded a patent for the discovery of a catalytic technique to convert synthesis gas to liquid hydrocarbons similar to petroleum. [Pg.2376]

In one sueeessful offshore installation, the turboexpander reeeives rieh natural gas at 80 bar and produees an 80/20 gas-to-liquid mass ratio at the diseharge. The integral eompressor reeompresses expander diseharge gases from 25-37 bar after the liquid is removed. The magnetie bearings operate in envu onments where namral gas is at 25 bar. [Pg.481]

The type of reaetor is seleeted in the light of numerous faetors sueh as volume ratio of gas to liquid, pressure drop, heat transfer and mixing intensity. [Pg.235]

While several other processes have been developed to convert natural gas to liquid fuels (GTL), these technologies are generally uneconomical composed to using the crude oil feedstocks. About one-third of the energy in natural gas is lost in converting it into liquid fuels, so highly distressed gas prices or government subsidies are needed for GTL to be competitive. [Pg.833]

Natural gas is an underutilized resource worldwide relative to oil but will play an increased role in the twenty-first century. New technologies such as gas-to-liquids and large-scale liquefied natural gas projects will also dramatically alter the fossil fuel landscape. [Pg.1010]

As our first approach to the model, we considered the controlling step to be the mass transfer from gas to liquid, the mass transfer from liquid to catalyst, or the catalytic surface reaction step. The other steps were eliminated since convective transport with small catalyst particles and high local mixing should offer virtually no resistance to the overall reaction scheme. Mathematical models were constructed for each of these three steps. [Pg.162]

One possibility for this was demonstrated in Chapter 3. If impact theory is still valid in a moderately dense fluid where non-model stochastic perturbation theory has been already found applicable, then evidently the continuation of the theory to liquid densities is justified. This simplest opportunity of unified description of nitrogen isotropic Q-branch from rarefied gas to liquid is validated due to the small enough frequency scale of rotation-vibration interaction. The frequency scales corresponding to IR and anisotropic Raman spectra are much larger. So the common applicability region for perturbation and impact theories hardly exists. The analysis of numerous experimental data proves that in simple (non-associated) systems there are three different scenarios of linear rotator spectral transformation. The IR spectrum in rarefied gas is a P-R doublet with either resolved or unresolved rotational structure. In the process of condensation the following may happen. [Pg.224]

Compact GTL (UK) Offshore gas-to-liquids facilities. Developing steam reforming and Eischer—Tropsch reactor technologies [6]... [Pg.240]

Battelle - Oxford Catalysts Offshore gas-to-liquids, biofuels, 50—50000 tons per year... [Pg.240]

The physical properties of a SCF are intermediate between those of a typical gas or liquid. For example, the diffusivity of a SCF is intermediate between a liquid and a gas and the viscosity is similar to a gas. The density of a SCF can be changed by varying the applied pressure on the fluid and can range between that exhibited by a gas to liquid-like values when the fluid is compressed... [Pg.82]

Consider an extreme case in which there is no resistance to reaction and all of the resistance is due to mass transfer. The rate of mass transfer is proportional to the interfacial area and the concentration of the driving force. An expression can be written for the rate of transfer of Component i from gas to liquid through the gas film per unit volume of reaction mixture ... [Pg.124]

This involves simultaneous decomposition and polymerization processes and phase changes from gas to liquid to solid. A detailed mechanism of the final transformations to carbon is rather complex and is not well understood. [Pg.75]


See other pages where Gas to Liquid is mentioned: [Pg.84]    [Pg.610]    [Pg.86]    [Pg.97]    [Pg.1415]    [Pg.2227]    [Pg.256]    [Pg.206]    [Pg.507]    [Pg.826]    [Pg.915]    [Pg.680]    [Pg.455]    [Pg.132]    [Pg.240]    [Pg.246]    [Pg.131]    [Pg.40]    [Pg.288]    [Pg.288]    [Pg.399]    [Pg.24]    [Pg.24]    [Pg.81]    [Pg.1]    [Pg.190]    [Pg.190]    [Pg.23]    [Pg.58]    [Pg.29]   
See also in sourсe #XX -- [ Pg.238 ]

See also in sourсe #XX -- [ Pg.31 , Pg.319 , Pg.320 ]




SEARCH



An Introduction to Bioreactor Hydrodynamics and Gas-Liquid Mass Transfer, First Edition

Base Stocks from Fischer-Tropsch Wax and the Gas to Liquids Process

Classifying Matter According to Its State Solid, Liquid, and Gas

Extension of EMMS modeling to gas-liquid flow

From liquid to gas

Gas to liquids process

Gas-liquid chromatography, to determine

Gas-to-liquid mass transfer

Gas-to-liquid shifts

Gas-to-liquids production

Gas-to-liquids technology

Liquid to gas ratio

Liquid to gas, expansion

Liquid-to-gas density ratio

Liquid-to-gas phase transition

Permeability to liquids and gases

Why is burning hydrogen gas in air (to form liquid water) a spontaneous reaction

© 2024 chempedia.info