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Helical springs

Fig. 16.3. Left Schematic picture of the damping system of MimiGRAIL. The suspension consists of seven stages, the upper four made of CuAl followed by three copper masses. The upper CuAl mass is suspended from the top flange of the cryostat by stainless steel cables hanging from helical springs. Mass number 5, the first copper mass, will be cooled by the dilution refrigerator. Right Picture of the four CuAl masses hanging from the top flange (courtesy of Leiden Cryogenics). Fig. 16.3. Left Schematic picture of the damping system of MimiGRAIL. The suspension consists of seven stages, the upper four made of CuAl followed by three copper masses. The upper CuAl mass is suspended from the top flange of the cryostat by stainless steel cables hanging from helical springs. Mass number 5, the first copper mass, will be cooled by the dilution refrigerator. Right Picture of the four CuAl masses hanging from the top flange (courtesy of Leiden Cryogenics).
In this section, we will discuss vibration isolation systems based on suspension springs with eddy-current damping. To date, it is probably the most efficient vibration isolation system. The design and choice of springs are also discussed. An elementary theory of helical springs, sufficient for all the applications in STM and AFM, is presented in Appendix F. [Pg.244]

Fig. F.7. Stiffness of a helical spring, (a) A fictitious position with a zero pitch, (b) When the pitch h of a spring increases, the twisting angle of the wire increases. The torque also increases. Using the formula for torsion, the stiffness of a helical spring is obtained. Fig. F.7. Stiffness of a helical spring, (a) A fictitious position with a zero pitch, (b) When the pitch h of a spring increases, the twisting angle of the wire increases. The torque also increases. Using the formula for torsion, the stiffness of a helical spring is obtained.
See Atomic units Helical springs 247, 373—374 allowable stres.s 374 materials 247 stiffness 247, 374 working stress 374 Herringbone pattern 329 Hertz formulas... [Pg.407]

Helical spring balances first used by McBain and Bakr have been extensively used for adsorption measurements. The spring is suspended inside a glass tube by attachment to a hook at the top. A bucket containing the adsorbent is connected to the bottom of the spring. The bottom of the tube, containing the sample, is immersed in the coolant. The upper portion of the tube is connected to a vacuum pump, source of adsorbate, and manometer. [Pg.192]

For maximum accuracy, the manifold and calibrated volumes in a volumetric apparatus should be maintained at constant temperature. Thermostating is not necessary for vacuum micro balances but in helical spring balances the spring should be maintained at constant temperature. Continuous flow apparatus need not be thermostated since the signals are immediately calibrated with known volumes at the same temperature and pressure. However, ambient temperature and pressure must be known to insure accurate calibration. [Pg.195]

The spring constant of a helical spring of a circular tvire can be calculated... [Pg.201]

In the older literature, chiral centers often are called asymmetric centers and you may be confused by the difference between asymmetric and dissymmetric. Both asymmetric and dissymmetric molecules (or objects) are chiral. An asymmetric object has no symmetry at all and looks different from all angles of view. Formulas 3 and 4 represent asymmetric molecules. A dissymmetric molecule is chiral, but looks the same from more than one angle of view. A helical spring is dissymmetric—it looks the same from each end. We will encounter dissymmetric molecules later. [Pg.116]

If you had several helical springs, how could you determine whether each spring was right- or left-handed ... [Pg.95]

The right- or left-handedness of a helix is the same as a conventional screw or bolt. When turned clockwise, a right-handed screw advances. The same is true of a helix or a helical spring. [Pg.889]

As a model for E we take a helical spring with stiffness E. The response e of such a spring to a stress cr is schematically indicated in Figure 6.1 the response is instantaneous, without any time dependency, and the recovery after release of the stress is also instantaneous and complete. [Pg.102]

For small U and C values, the discharge resistor may be permanently connected to the capacitor. In the example given above, the resulting power loss would be 10 kW. Consequently, a discharge switch shall be fitted which automatically closes the discharge circuit. For pressurized apparatus, a single-pole vacuum tube (contactor type) may be used. Its open position is achieved by a pneumatically actuated drive, the closed position should be maintained by the atmospheric air pressure, and, if necessary, by an additional helical spring. [Pg.127]

Adsorption from the gas phase can be measured by either gravimetric or volumetric techniques. In the gravimetric method, the weight of adsorbed gas is measured by observing the stretching of a helical spring from which the adsorbent is himg (see Fig. 2).f Alternatively,... [Pg.311]

Fig. 4 Typical sinker designs. (A) 3-prong sinker (B) JP basket sinker and (C) helical-spring sinker. Fig. 4 Typical sinker designs. (A) 3-prong sinker (B) JP basket sinker and (C) helical-spring sinker.
In another static method of measuring gas adsorption, the amount of gas adsorbed is measured by the increase in the weight of the adsorbent. For this, a very useful balance was developed by McBain and Bakr (Figure 13 2), the essential part of which is a helical spring... [Pg.302]

The helical spring, in which changes of mass are detected by contraction or elongation of the spring and which may be recorded by suitable transducers. [Pg.90]

Incremental or continuous application of torsional or helical spring force. [Pg.91]

Strain in the system of bonds of reactants, and the release of the strain as the transition state converts to the products (like cutting a stretched helical spring), can provide rate enhancement of chemical reactions. [Pg.157]

Fig. 13.9. The experimental apparatus used to measure the interaction between crossed mica cylinders (see inset) (after Israelachvili et ai, 1979 1980). Note that M=micrometer drive, 0=microscope objective, P=mica plates, E=piezoelectric crystal, H = helical spring, C=stiff double cantilever spring and L=ir light. Fig. 13.9. The experimental apparatus used to measure the interaction between crossed mica cylinders (see inset) (after Israelachvili et ai, 1979 1980). Note that M=micrometer drive, 0=microscope objective, P=mica plates, E=piezoelectric crystal, H = helical spring, C=stiff double cantilever spring and L=ir light.

See other pages where Helical springs is mentioned: [Pg.238]    [Pg.119]    [Pg.396]    [Pg.195]    [Pg.274]    [Pg.373]    [Pg.373]    [Pg.916]    [Pg.973]    [Pg.974]    [Pg.54]    [Pg.75]    [Pg.128]    [Pg.336]    [Pg.448]    [Pg.42]    [Pg.402]    [Pg.169]    [Pg.912]    [Pg.198]    [Pg.146]    [Pg.147]    [Pg.348]    [Pg.354]    [Pg.740]    [Pg.205]    [Pg.721]   
See also in sourсe #XX -- [ Pg.146 ]




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