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Slumping

Another application of laser-based profilometry is the inspection of rocket and missile components. The U.S. Air Force has funded work to develop a non-contact laser-based profilometer for the inside surface of solid rocket motors. Over time, these devices are subject to slumping and cracking, which could potentially render the rocket motor ineffective and hazardous. When fully implemented, this system will provide a meaningful screening method for evaluating the condition of aging rocket motors. [Pg.1066]

The average polymer Enjoys a glassy state, but cools, forgets To slump, and clouds in closely patterned minuets. [Pg.199]

Increases in U.S. demand for caustic soda have been unpredictably high in the last few years. Between 1987 and 1989, the annual increase in demand was about 3% (6). However, the caustic soda market is mature and new areas of significant growth have not surfaced in recent years. The unexpected recent demand is generally related to two factors the pick-up in the U.S. economy after the slump of 1986 and pulp mills operating at fiiU capacity, leading to less efficient caustic use. [Pg.517]

To estimate the slumping motion of the kiln bed which periodically exposes a fresh, vapor saturated surface at the bed—freeboard interface must be considered. Based on Pick s second law in a bed of porosity, S, and for an effective diffusion coefficient, the mass-transfer coefficient on the bed side is... [Pg.51]

Ball and roUer bearings represent the largest business segment with worldwide production estimated at 14 biUion in 1988 (1). U.S. production, forecast for 3.6 biUion in 1991, has fallen 5% aimuaHy for several years (2). This decrease is attributed largely to the slump in the automotive industry which represents 31% of the market for rolling-element bearings (3). [Pg.1]

Impression plasters are formulated to produce a thin, fluid slurry when mixed with the proper amount of water. A satisfactory impression plaster should have a setting time of 4 1.5 min fineness, ie, 98% should pass a number 100 sieve (ca 0.15 mm), and 90% pass a number 200 sieve (ca 0.07 mm) setting expansion at 2 h should be <0.15% the compressive strength at one hour should be 5.9 2 MPa (855.5 290 psi) and testing consistency as determined by the diameter of the slump in the consistence test should be 90 3 mm. [Pg.476]

Model Plasters. Model plaster should have a setting time of approximately 10 minutes. The fineness of the powder should be such that 98% passes a number 100 sieve (ca 0.15 mm) and 90% passes a number 200 sieve (ca 0.07 mm). Setting expansion should be less than 0.30%, compressive strength at the end of one h should be a minimum of 8.8 MPa (1276 psi), and the consistency should form a disk during the slump test of 30 2 mm diameter. [Pg.476]

Mixes of improved dental stone (type IV) using 22 parts of water to 100 parts of powder produce a mass that is not fluid and pourable but can be easily vibrated into place. The physical properties of the improved dental stone include a setting time 10 3 min, fineness of powder such that 98% passes a 100 sieve (ca 0.15 mm) and 90% passes a 200 sieve (ca 0.07 mm) setting expansion at 2 h limited to a max of 0.10% compressive strength at 1 h of at least 34.3 MPa (4974 psi) and a disk formed in the slump test for consistency of a 30 2 mm diameter. [Pg.477]

Figure 26-53 shows the affect of initial momentum and buoyancy of the release. If the material is released as a jet, then the effective height of the release is increased. Furthermore, if the material released is heavier than air (which is the usual case for the release of most hydrocarbons), the plume initially slumps toward the ground until subsequent dilution by air results in a neutrally buoyant cloud. [Pg.2341]

Dense gases behave considerably differently from neutrally buoyant gases. When they are initially released, these gases slump toward the ground and move both upwind and downwind. Furthermore, the mechanisms for mixing with air are completely different from neutrally buoyant releases. [Pg.2344]

This section was written for the fourth edition published in 1982 at a time when there had just been a further sharp increase in the price of petroleum. At the time I was optimistic about the future for plastics, although I did not anticipate the slump in oil prices that has taken place since then. Oil remains a finite resource and sooner or later prices wilt rise again. Apart from changing one word and inserting one other for technical reasons, I see no reason to otherwise change what I wrote then. [Pg.15]

In 1942 the Japanese overran Malaya and the then Dutch East Indies to cut off the main sources of natural rubber for the United States and the British Commonwealth. Because of this the US Government initiated a crash programme for the installation of plants for the manufacture of a rubber from butadiene and styrene. This product, then known as GR-S (Government Rubber-Styrene), provided at that time an inferior substitute for natural rubber but, with a renewed availability of natural rubber at the end of the war, the demand for GR-S slumped considerably. (Today the demand for SBR (as GR-S is now known) has increased with the great improvements in quality that have been made and SBR is today the principal synthetic rubber). [Pg.425]

On release, vapours heavier than air tend to spread (i.e. to slump ) at low level and will aeeumulate in pits, sumps, depressions in ground, ete. This may promote a fire/explosion hazard, or a toxie hazard, or eause an oxygen-defieient atmosphere to form, depending on the ehemieal. [Pg.48]

The density of a vapour or gas at eonstant pressure is proportional to its relative moleeular mass and inversely proportional to temperature. Sinee most gases and vapours have relative moleeular masses greater than air (exeeptions inelude hydrogen, methane and ammonia), the vapours slump and spread or aeeumulate at low levels. The greater the vapour density, the greater the tendeney for this to oeeur. Gases or vapours whieh are less dense than air ean, however, spread at low level when eold (e.g. release of ammonia refrigerant). Table 6.1 ineludes vapour density values. [Pg.180]

Provide a high level of general ventilation taking note of density and volume of gas likely to develop initially gases will slump, while those less dense than air (e.g. hydrogen, helium) will eventually rise. [Pg.260]

The gas generated by vaporization is eold and therefore denser than air, i.e. it tends to slump. [Pg.264]

Preeautions also have to be instituted to proteet against the inherent properties of the eylinder eontents, e.g. toxie, eorrosive, flammable (refer to Table 9.1). Most gases are denser than air eommon exeeptions inelude aeetylene, ammonia, helium, hydrogen and methane. Even these may on eseape be mueh eooler than ambient air and therefore slump initially. Eventually the gas will rise and aeeumulate at high levels unless ventilated. Hydrogen and aeetylene, whieh both have very wide flammable limits (Table 6.1), ean form explosive atmospheres in this way. [Pg.265]

Reinforcing fillers (active) Fumed Silica (Si02) precipitated calcium carbonate (CaCOi) carbon black Thixotropic reinforcing agents (non-slump), adjustment of mechanical properties (cohesion) provide toughness to the elastomer as opposed to brittle materials. [Pg.701]

The lift pipe design was tapered to a larger diameter at the top. This minimized the effects of erosion and catalyst attrition, and also prevented the instantaneous total collapse of circulations when the saltation concentration, or velocity, of solids is experienced (i.e. the slump veloeity-that velocity helow which particles drop out of the flowing gas stream). In a typical operation, 2 % to 4 % eoke can he deposited on the catalyst in the reactor and burned in the regenerator. Catalyst circulation is generally not sufficient to remove all the heat of eombustion. This facilitated the need for steam or pressurized water coils to be located in the regeneration zone to remove exeess heat. [Pg.208]

Melting and slumping of the fuel onto the lower core support structures and into the vessel bottom head. [Pg.317]

It a bottom node (i.j) is tally nwiten, it and ail moiton nodes above ii slump from core to 1 si support grid... [Pg.318]


See other pages where Slumping is mentioned: [Pg.48]    [Pg.48]    [Pg.48]    [Pg.52]    [Pg.248]    [Pg.237]    [Pg.31]    [Pg.51]    [Pg.104]    [Pg.406]    [Pg.418]    [Pg.323]    [Pg.503]    [Pg.504]    [Pg.290]    [Pg.300]    [Pg.222]    [Pg.175]    [Pg.292]    [Pg.187]    [Pg.313]    [Pg.318]    [Pg.432]    [Pg.49]    [Pg.189]    [Pg.369]    [Pg.353]   
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See also in sourсe #XX -- [ Pg.65 ]

See also in sourсe #XX -- [ Pg.289 ]

See also in sourсe #XX -- [ Pg.22 ]

See also in sourсe #XX -- [ Pg.273 ]




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Concrete slump

Equations for Slump Predictions

Inverted slump cone test

Slump

Slump

Slump characteristics

Slump control factor

Slump loss

Slump loss effect

Slump prediction

Slump retention

Slump test

Slump velocity

Slumping bed

Slumping technique

Spread and Slump

Vapour slumping

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