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Clamping geometries

FIGURE 10.14 Diagrammatic representation of the compression clamp geometry. (Adapted from Dynamic Mechanical Analyser 2980 Operator s Manual, TA Instruments, New Castle, DE, 1996.)... [Pg.330]

Different clamping geometries are used to accommodate particular specimens (Figure 8). Single or dual cantilever bending modes are the most common for materials which can be formed into bars. Shear measurements are used for soft, thick samples. Films and fibres are usually mounted in tension with loading arranged so that the sample is... [Pg.104]

Figure 8 Common clamping geometries for dynamic mechanical analysis (cf. Figure 1)... Figure 8 Common clamping geometries for dynamic mechanical analysis (cf. Figure 1)...
In practice the clamping pressure will also depend on the geometry of the cavity. In particular the flow ratio (flow length/channel lateral dimension) is important. Fig. 4.42 illustrates typical variations in the Mean Effective Pressure in the cavity for different thicknesses and flow ratios. The data used here is typical for easy flow materials such as polyethylene, polypropylene and polystyrene. To calculate the clamp force, simply multiply the appropriate Mean Effective Pressure by the projected area of the moulding. In practice it is... [Pg.294]

In a different context, a micropipette has been applied to monitor the current through a single-ion channel in a biological membrane. The patch-clamp technique invented by Sackmann and Neher [119] led to their Nobel Prize in medicine. The variations in channel current with voltage, concentration, type of ions, and type of channels have been explored. While the functions of specific channels, in particular their ionic selectivity, have been well known, only a handful of channels have the internal geometry and charge distribution determined. The development of a theory to interpret the mass of channel data and to predict channel action is still lacking. [Pg.643]

It turns out that it is possible to develop another version of the adiabatic theory, which can be applied in many cases. Often nuclei (ions) are located near the equilibrium geometry which leads to simplifications of the theory—the clamped adiabatic approximation. Sometimes this approach is called the "crude" approximation (46,77). [Pg.145]

Tunneling junctions are most often produced in a crossed stripe geometry so that 4-terminal measurements of their current-voltage characteristics can be made. Electrical contacts are made to the films ( often with miniature brass "C" clamps ), the samples are mounted in a Dewar insert, and cooled to liquid helium temperatures ( 4.2 ° K or below ). [Pg.218]

Summary. The interplay between electrical and mechanical properties of suspended, doubly clamped carbon nanotubes in the Coulomb blockade regime is studied theoretically. In this geometry, the capacitance between the nanotube and the gate depends on the distance between them. We find that the tube position changes in discrete steps every time an electron tunnels onto it. Edges of Coulomb diamonds acquire a (small) curvature. Eigenffequencies are modified by Coulomb blockade in a discrete fashion. [Pg.47]

The terms, Enn(Q)and Hpq(Q) are introduced over the Taylor s expansion at the equilibrium geometry of fixed nuclear configuration Ro (crude level -clamped nuclei),... [Pg.88]

Since the longest flow path may exceed the radius of the projected area that causes mold separating pressures, we must also find the radius of equivalent projected area, Rp, to compute a more accurate mold clamping force. However, to perform the calculations to predict velocities and pressure fields, we assume a disc geometry of radius R and thickeness h, schematically depicted in Fig. 8.41. [Pg.428]

Sample application of the radial flow method. In this sample application, we are to determine the maximum clamping force and injection pressure required to mold an ABS suitcase shell with a filling time, tf=2.5 s. For the calculation we will use the dimensions and geometry schematically depicted in Fig. 8.49, an injection temperature of 227°C (500 K), a mold temperature of 27°C (300 K) and the material properties given in Table 8.8. [Pg.435]


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