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Manifolds

Another characteristic similar to A/ 100 is the Distribution Octane Number (DON) proposed by Mobil Corporation and described in ASTM 2886. The idea is to measure the heaviest fractions of the fuel at the inlet manifold to the CFR engine. For this method the CFR has a cooled separation chamber placed between the carburetor and the inlet manifold. Some of the less volatile components are separated and collected in the chamber. This procedure is probably the most realistic but less discriminating than that of the AJ 100 likewise, it is now only of historical interest. [Pg.200]

Gasoline engine equipment such as carburetors, injectors, intake manifolds, valve systems and combustion chambers, are subject to fouling by the fuel itself, the gases recycled from the crankcase, or even dust and particulates arriving with poorly filtered air. Three types of problems then result ... [Pg.243]

As the first well is being drilled the template is connected to the host facility with flowlines, umbilicals and risers. A Chemical Injection Umbilical will also typically be laid to the template or subsea facility and connected to a distribution manifold. [Pg.269]

If one or more clusters of single wells are required then an Underwater Manifold System can be deployed and used as a subsea focal point to connect each well. The subsea trees sit on the seabed around the main manifold (compared to the template). [Pg.270]

Only one set of pipelines and umbilicals (as with the template) are required from the manifold back to the host facility, saving unnecessary expense. Underwater manifolds are becoming very popular as they offer a great deal of flexibility in field development and can be very cost effective. [Pg.270]

The manifold is typically a tubular steel structure (similar to a template) which is host to a series of remotely operated valves and chokes. It is common for subsea tree control systems to be mounted on the manifold and not on the individual trees. A complex manifold will generally have its own set of dedicated subsea control modules (for controlling manifold valves and monitoring flowline sensors). [Pg.270]

Modern subsea trees, manifolds, (EH), etc., are commonly controlled via a complex Electro-Hydraulic System. Electricity is used to power the control system and to allow for communication or command signalling between surface and subsea. Signals sent back to surface will include, for example, subsea valve status and pressure/ temperature sensor outputs. Hydraulics are used to operate valves on the subsea facilities (e.g. subsea tree and manifold valves). The majority of the subsea valves are operated by hydraulically powered actuator units mounted on the valve bodies. [Pg.270]

The master control station allows the operator to open and close all the systems remotely operated valves, including tree and manifold valves and downhole safety valve. [Pg.271]

Subsea facilities are easily decommissioned as they are relatively small and easy to lift. However, subsea manifolds and templates can weigh in excess of 1,000 tons and will require heavy lift barges for removal. [Pg.371]

COLOURED PRODUCTS BOX MANIFOLD NOTCH SPECIMEN 1 NOTCH SPECIMEN 2... [Pg.624]

Maas U and Pope S B 1992 Simplifying chemical kinetics intrinsic low-dimensional manifolds in composition space Comb. Flame 88 239... [Pg.796]

Mbelonging to the complementary manifold = M, In a second time interval the superposition... [Pg.1059]

IVR in tlie example of the CH clnomophore in CHF is thus at the origin of a redistribution process which is, despite its coherent nature, of a statistical character. In CHD, the dynamics after excitation of the stretching manifold reveals a less complete redistribution process in the same time interval [97]. The reason for this is a smaller effective coupling constant between the Fenni modes of CHD (by a factor of four) when... [Pg.1072]

Figure Bl.3.4. The two fully resonant doorway stages for resonanee Raman seattering (RRS), in wlheh the manifold of vibrational sublevels for eaeh eleetronie state is indieated. (a) Doorway stage iii... Figure Bl.3.4. The two fully resonant doorway stages for resonanee Raman seattering (RRS), in wlheh the manifold of vibrational sublevels for eaeh eleetronie state is indieated. (a) Doorway stage iii...
Wliatever the deteetion teehnique, the window stage of the 4WM event must eonvert these evolved vibrational wavepaekets into the third order polarization field that oseillates at an ensemble distribution of optieal frequeneies. One must be alert to the possibility that the window event after doorway ehaimel B may involve resonanees from eleetronie state manifold e to some higher manifold, say r. Thus ehaimel B followed by an e (ket) or a (bra) event might be enlianeed by an e-to-r resonanee. However, it is nonnal to eonfine the... [Pg.1202]

Figure Bl.4.9. Top rotation-tunnelling hyperfine structure in one of the flipping inodes of (020)3 near 3 THz. The small splittings seen in the Q-branch transitions are induced by the bound-free hydrogen atom tiiimelling by the water monomers. Bottom the low-frequency torsional mode structure of the water duner spectrum, includmg a detailed comparison of theoretical calculations of the dynamics with those observed experimentally [ ]. The symbols next to the arrows depict the parallel (A k= 0) versus perpendicular (A = 1) nature of the selection rules in the pseudorotation manifold. Figure Bl.4.9. Top rotation-tunnelling hyperfine structure in one of the flipping inodes of (020)3 near 3 THz. The small splittings seen in the Q-branch transitions are induced by the bound-free hydrogen atom tiiimelling by the water monomers. Bottom the low-frequency torsional mode structure of the water duner spectrum, includmg a detailed comparison of theoretical calculations of the dynamics with those observed experimentally [ ]. The symbols next to the arrows depict the parallel (A k= 0) versus perpendicular (A = 1) nature of the selection rules in the pseudorotation manifold.
Figure Bl.12.13. MAS NMR spectra from kyanite (a) at 17.55 T along with the complete simulation and the individual components, (b) simulation of centreband lineshapes of kyanite as a fiinction of applied magnetic field, and tire satellite transitions showing (c) the complete spiimmg sideband manifold and (d) an expansion of individual sidebands and their simulation. Figure Bl.12.13. MAS NMR spectra from kyanite (a) at 17.55 T along with the complete simulation and the individual components, (b) simulation of centreband lineshapes of kyanite as a fiinction of applied magnetic field, and tire satellite transitions showing (c) the complete spiimmg sideband manifold and (d) an expansion of individual sidebands and their simulation.

See other pages where Manifolds is mentioned: [Pg.267]    [Pg.268]    [Pg.281]    [Pg.282]    [Pg.340]    [Pg.265]    [Pg.1057]    [Pg.1058]    [Pg.1058]    [Pg.1059]    [Pg.1062]    [Pg.1063]    [Pg.1063]    [Pg.1065]    [Pg.1065]    [Pg.1065]    [Pg.1067]    [Pg.1069]    [Pg.1071]    [Pg.1072]    [Pg.1073]    [Pg.1073]    [Pg.1073]    [Pg.1073]    [Pg.1075]    [Pg.1076]    [Pg.1201]    [Pg.1202]    [Pg.1256]    [Pg.1555]    [Pg.1578]    [Pg.2110]   
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Manifolding

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