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Flash pocket

Generally, the blow mold is a cavity representing the outside of a blow-molded part The basic structure of a blow mold consists of a cast or machined block with a cavity, cooling system, venting system, pinchoffs, flash pockets, and mounting plate. The selection of material for the construction of a blow mold is based on the consideration of such factors as thermal conductivity, durabrhty, cost of the material, the resin being processed, and the desired quality of the finished parts. Commonly used mold materials are berylHum, copper, aluminum, ampcoloy, A-2 steel, and 17-4 and 420 stainless steels. [Pg.191]

I) Conventional pinch-off edge (II) coextrusion pinch-off edge (III) pinch-off edge for Selar RB (1) Flash pocket (2) cavity... [Pg.151]

In order to keep the inserts a constant size, the overall dimensions will not be changed. The Laser Mike and pillow mold will be used to set the parison thickness at 0.3048mm. The thickness of the compression region of the flash pocket will be modified four times, keeping the length of the pocket constant. The optimum thickness is determined and three more inserts will be machined with the optimum depth as a constant dimension and vaiying the length of the first pocket. The HDPE parts will then... [Pg.3001]

One cmrent rule is the depth of the pocket is determined by multiple factors. These factors are plastic density, weight of part and parison, parison diameter, parison orientation, and pre-blow pressme. When the flash pocket is shallow, it causes extreme pressme at the parting line and machine pressure section and it causes difficulties in trimming off the flash. When the flash pocket is deep, it causes poor cooling. The poor cooling can cause a hot flash which softens and weakens the weld line [1]. [Pg.3001]

There are multiple types of pinch-offs used. Single pinch-offs are used to make smaller bottles. Usually, these bottles are up to 19 liters [1]. The landing varies from 0.254 to 1.0 millimeter [1]. The land on the one half of the mold usually varies from the land on the other half of the mold for better cut off Another type of pinch off is the double compression pinch-off. This type is used for bigger bottles. The primary pinch-off at fre parting line level widths vary from 1.0 to 2.0 millimeters [1]. The secondary flash pocket, which is below the parting line, varies from. 254 to 1.0 millimeter. The width of this pinch-off area has a length that is equal or smaller. [Pg.3002]

A vapor poeket on the exchanger s low-pressure side can create a cushion that may greatly diminish the pressure transient s intensity. A transient analysis may not be required if sufficient low-pressure side vapor exists (although tube rupture should still be considered as a viable relief scenario). However, if the low-pressure fluid is liquid from a separator that has a small amount of vapor from flashing across a level control valve, the vapor pocket may collapse after the pressure has exceeded the fluid s bubble point. The bubble point will be at the separator pressure. Transient analysis will prediet a gradually inereasing pressure until the pressure reaches the bubble point. Then, the pressure will increase rapidly. For this ease, a transient analysis should be considered. [Pg.49]

Two-phase flow is beyond the scope of this pocket guide. One word of advice Be careful when designing low pressure and/or flashing condensate lines. These deserve special care. Ruskin10 has a quick method for condensate line sizing. [Pg.14]

When the bottom valve was opened, the pocket of water came in contact with the hot oil. Flashing steam surged upward through the tower. The steam created excessive pressures at the bottom of the tower, and all the trays dropped within the tower. In this case the pressure luckily did not exceed the vessel rupture pressure. Although no injuries were sustained, the tower was destroyed by this accident. [Pg.553]

Did I miss anything Garudin flashed a look at his gold watch, the only decoration about his person besides the pristine wedge of blue-silk handkerchief poking out of his breast pocket. [Pg.33]

Aluminium electrolytic capacitors are exploited in a range of applications and their relatively low cost makes them attractive for printed circuits for car radios, stereo equipment, pocket calculators, digital clocks, etc. Also, the very high value capacitors are used in large photo-flash equipment and for voltage smoothing. [Pg.258]

In some cases, as with pulp-mill liquors, the evaporator vapors contain constituents more volatile than water, such as methanol and sulfur compounds. Special precautions may be necessary to minimize the effects of these compounds on heat transfer, corrosion, and condensate quality. They can include removing most of the condensate countercurrent to the vapor entering an evaporator-heating element, channeling vapor and condensate flow to concentrate most of the foul constituents into the last fraction of vapor condensed (and keeping this condensate separate from the rest of the condensate), and flashing the warm evaporator feed to a lower pressure to remove much of the foul constituents in only a small amount of flash vapor. In all such cases, special care is needed to properly channel vapor flow past the heating surfaces so there is a positive flow from steam inlet to vent outlet with no pockets, where foul constituents or noncondensibles can accumulate. [Pg.970]

If rows of identical pockets are machined into the working surface and the rollers are timed such that the pocket halves exactly match, so-called briquettes are formed (Figure 224). Roller presses do not produce compacts with the same fine detail and uniformity as those made by tabletting machines or other die presses. The flashing or web, caused by the land areas around each briquette pocket, which is usually found on the edges of all briquettes from roller presses can not be removed completely and reliably and, therefore, may also be objectionable. [Pg.263]

Good briquettes discharging from the presses are surrounded by a flash which is produced on the land areas between the pockets on the rollers (see Section 4.2.2.4.7). These flashes break off during handling and are separated on the screens (17 and 20) producing so-called chips—relatively hard, compacted particles that require crushing prior to feeding back into the system. [Pg.465]

Fig. 12. Convective regions for the 1.9M0, Z = 0.008 model during the first five thermal pulses. The He-intershell extends from about 0.52Mq to 0.56Mq. The teardrop-shaped pockets correspond to the flash-driven convective region that extends over most of the He-intershell. These have the effect of homogenizing the abundances within the He-intershell. Convective regions are shaded in green and radiative zones in magenta. The n-axis is nucleosynthesis time-step number, which is a proxy for time. For this model, the duration of the convective zones are about 250 years... Fig. 12. Convective regions for the 1.9M0, Z = 0.008 model during the first five thermal pulses. The He-intershell extends from about 0.52Mq to 0.56Mq. The teardrop-shaped pockets correspond to the flash-driven convective region that extends over most of the He-intershell. These have the effect of homogenizing the abundances within the He-intershell. Convective regions are shaded in green and radiative zones in magenta. The n-axis is nucleosynthesis time-step number, which is a proxy for time. For this model, the duration of the convective zones are about 250 years...
Fig. 22. The composition of the He-intershell for a 3Mq, Z = 0.02 model. The upper panel shows the composition during a thermal pulse, where the flash-driven convective pocket is shown (at its full extent it reaches from 0.664Mq almost all the way to the H-shell at 0.679Mq). The lower panel shows the composition of the He-intershell after the thermal pulse has died down, before the next third dredge-up takes place. The location of the base of the outer convective envelope is 0.681Mq... Fig. 22. The composition of the He-intershell for a 3Mq, Z = 0.02 model. The upper panel shows the composition during a thermal pulse, where the flash-driven convective pocket is shown (at its full extent it reaches from 0.664Mq almost all the way to the H-shell at 0.679Mq). The lower panel shows the composition of the He-intershell after the thermal pulse has died down, before the next third dredge-up takes place. The location of the base of the outer convective envelope is 0.681Mq...
Fig. 20. left) Optical emission spectra from a suspension of A1 nanoparticles in nitrocellulose oxidizer (NC) after laser flash heating at the indicated fluences. Higher resolution spectra of the features indicated by i)-(iv) are shown in the insets. These features are attributed to AlO emission at surfaces or gas pockets. Reproduced from ref. [201]. [Pg.177]


See other pages where Flash pocket is mentioned: [Pg.182]    [Pg.655]    [Pg.3001]    [Pg.3001]    [Pg.182]    [Pg.655]    [Pg.3001]    [Pg.3001]    [Pg.1147]    [Pg.230]    [Pg.124]    [Pg.125]    [Pg.147]    [Pg.333]    [Pg.12]    [Pg.119]    [Pg.305]    [Pg.120]    [Pg.335]    [Pg.69]    [Pg.3785]    [Pg.2599]    [Pg.114]    [Pg.280]    [Pg.282]    [Pg.292]    [Pg.286]    [Pg.125]    [Pg.223]    [Pg.34]    [Pg.149]    [Pg.151]    [Pg.216]   
See also in sourсe #XX -- [ Pg.125 ]




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