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Clamped couplings

Muff. m, muff (Tech.) sleeve, collar, socket, socket joint, clamp, coupling box musty or moldy smell, mustinesa, moldiness,... [Pg.305]

Flanged rigid couplings, split rigid or clamp couplings... [Pg.996]

Figure 3-34 Proportional base drive circuits (a) the Baker clamp (b) transformer-coupled proportional base drive. Figure 3-34 Proportional base drive circuits (a) the Baker clamp (b) transformer-coupled proportional base drive.
Making an active clamp from a controller IC that does not support its direct drive depends upon which signals are brought out from the IC. Figure 4—8 gives a couple of ideas. [Pg.148]

On the basis of the principle of grafted TLC, reversed-phase (RP) and normal-phase (NP) stationary phases can also be coupled. The sample to be separated must be applied to the first (2.5 cm X 20 cm) reversed-phase plate (Figure 8.16(a)). After development with the appropriate (5ti 5yi) mobile phase (Figure 8.16(b)), the first plate must be dried. The second (20 cm X 20 cm) (silica gel) plate (Figure 8.16(c)) must be clamped to the first (reversed-phase) plate in such a way that by use of a strong solvent system (Sj/, SyJ the separated compounds can be transferred to the second plate (Figure 8.16(d)). Figure 8.16(e) illustrates the applied, re-concentrated... [Pg.187]

Figure 8.16 Views from above (a-c, e, and f) of coupled RP-NP cliromatographic plates (without lines, RP stationaiy phase light shading, NP stationaiy phase), and schematic diagram of a cross-section (d) tlrrough the clamped plates using a strong mobile phase (S-j-/, 5vj) for the transfer of the sample to be further separated. Figure 8.16 Views from above (a-c, e, and f) of coupled RP-NP cliromatographic plates (without lines, RP stationaiy phase light shading, NP stationaiy phase), and schematic diagram of a cross-section (d) tlrrough the clamped plates using a strong mobile phase (S-j-/, 5vj) for the transfer of the sample to be further separated.
Figure 8.17 Schematic diagram of a cross-section (a) tlvough the clamped plates, and views from above (b-d) of coupled plates serially connected to achieve multidimensional separation with stationary phases with different characteristics (hatched lines, glass plate light shading, stationary phase A dark shading, stationary phase B wavy lines, stationary phase C). Figure 8.17 Schematic diagram of a cross-section (a) tlvough the clamped plates, and views from above (b-d) of coupled plates serially connected to achieve multidimensional separation with stationary phases with different characteristics (hatched lines, glass plate light shading, stationary phase A dark shading, stationary phase B wavy lines, stationary phase C).
With the shear-type coupling, the elastomeric element may be clamped or bonded in place, or fitted securely to the hubs. The compression-type couplings may be fitted with projecting pins, bolts, or lugs to connect the components. Polyurethane, rubber, neoprene, or cloth and fiber materials are used in the manufacture of these elements. [Pg.994]

Also, if your clamp is too hot, check that the leakage inductance of the transformer is better than about 1 to 2% of the primary inductance. If not, you need to first reduce the leakage inductance. That calls for improving the coupling between the Primary and (main)... [Pg.230]

CUORICINO crystals are grouped in elementary modules of four elements (see Fig. 15.7) held between two copper frames joined by copper columns. PIPE pieces are inserted between the copper and TeOz, as a heat impedance and to clamp the crystals. There is a 6 mm gap between crystals with no material in between. The four detectors are mechanically coupled some of the PTFE blocks and springs act simultaneously on two crystals. [Pg.365]

With the triples correction added, the error relative to experiment is still as large as 15 kJ/mol. More importantly, we are now above experiment and it is reasonable to assume that the inclusion of higher-order excitations (in particular quadruples) would increase this discrepancy even further, perhaps by a few kJ/mol (judging from the differences between the doubles and triples corrections). Extending the coupled-cluster expansion to infinite order, we would eventually reach the exact solution to the nonrelativistic clamped-nuclei electronic Schrodinger equation, with an error of a little more than 15 kJ/mol. Clearly, for agreement with experiment, we must also take into account the effects of nuclear motion and relativity. [Pg.10]


See other pages where Clamped couplings is mentioned: [Pg.991]    [Pg.304]    [Pg.216]    [Pg.229]    [Pg.991]    [Pg.304]    [Pg.216]    [Pg.229]    [Pg.94]    [Pg.449]    [Pg.958]    [Pg.958]    [Pg.298]    [Pg.619]    [Pg.14]    [Pg.97]    [Pg.249]    [Pg.186]    [Pg.28]    [Pg.920]    [Pg.533]    [Pg.32]    [Pg.306]    [Pg.59]    [Pg.22]    [Pg.324]    [Pg.311]    [Pg.568]    [Pg.203]    [Pg.171]    [Pg.151]    [Pg.153]    [Pg.154]    [Pg.180]    [Pg.462]    [Pg.64]    [Pg.578]    [Pg.47]    [Pg.115]    [Pg.451]    [Pg.262]    [Pg.357]   
See also in sourсe #XX -- [ Pg.304 ]




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