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Spring element

Fig. 6. Load cell spring element. C, gauges in compression T, gauges in tension. Fig. 6. Load cell spring element. C, gauges in compression T, gauges in tension.
Load-ceU performance is limited by properties such as nonlinearity, hysteresis, and creep, which are inherent to the particular design or spring element material. [Pg.327]

These layouts are configured as shown in Figure 6-25. The cantilevered support ribs, along with die sector diey are supporting at bodi ends, form a centering spring element. The small gap between die sector and die outer ring forms die squeeze film damper clearance... [Pg.364]

That is, the stress is constant and supported by the spring element so that the predicted response is that of an elastic material, i.e. no relaxation (see Fig. 2.37)... [Pg.89]

Solution The spring element constant, i, for the Maxwell model may be obtained from the instantaneous strain, . Thus... [Pg.91]

A Standard Model for the viscoelastic behaviour of plastics consists of a spring element in scries with a Voigt model as shown in Fig. 2.86. Derive the governing equation for this model and from this obtain the expression for creep strain. Show that the Unrelaxed Modulus for this model is and the Relaxed Modulus is fi 2/(fi + 2>. [Pg.162]

Christensen Shock-Eze. See Figure 4-170 [57]. A double-action vibration and shock absorber employing Belleville spring elements are immersed in oil. [Pg.813]

Certain considerations should be given to achieve adequate results at a reasonable cost when using finite element analysts methods. One item to consider is the appropriateness and practicality of the element type. The most suitable element types from the simplest to the most complex include spring elements, line (beam) elements, piate/shell elements and solid elements. [Pg.182]

When dash pot and spring elements are connected in parallel they simulate the simplest mechanical representation of a viscoelastic solid. The element is referred to as a Voigt or Kelvin solid, and it is shown in Fig. 3.10(c). The strain as a function of time for an applied force for this element is shown in Fig. 3.11. After a force (or stress) elongates or compresses a Voigt solid, releasing the force causes a delay in the recovery due to the viscous drag represented by the dash pot. Due to this time-dependent response the Voigt model is often used to model recoverable creep in solid polymers. Creep is a constant stress phenomenon where the strain is monitored as a function of time. The function that is usually calculated is the creep compliance/(f) /(f) is the instantaneous time-dependent strain e(t) divided by the initial and constant stress o. ... [Pg.74]

The linear spring element SI will undergo an extension A rsi according to... [Pg.187]

Fig. 1. Layout of titin in the sarcomere. Center panel electron micrograph of sarcomere of stretched soleus muscle fiber, labeled with anti-titin antibodies that demarcate the tandem Ig and PEVK spring elements of titin s extensible I-band region. Superimposed are two schematic titin molecules (one for each half sarcomere). Top and bottom panels domain structure of I-band and A-band sequence of titin, respectively (from Labeit and Kolmerer, 1995). Bottom left length of tandem Ig segment (proximal + distal segment) and PEVK segment in human soleus fibers, as function of sarcomere length (based on Trombitas et al., 1998b). Fig. 1. Layout of titin in the sarcomere. Center panel electron micrograph of sarcomere of stretched soleus muscle fiber, labeled with anti-titin antibodies that demarcate the tandem Ig and PEVK spring elements of titin s extensible I-band region. Superimposed are two schematic titin molecules (one for each half sarcomere). Top and bottom panels domain structure of I-band and A-band sequence of titin, respectively (from Labeit and Kolmerer, 1995). Bottom left length of tandem Ig segment (proximal + distal segment) and PEVK segment in human soleus fibers, as function of sarcomere length (based on Trombitas et al., 1998b).
Segment contains tandem Ig repeats and PEVK repeats, both acting as molecular spring elements. This segment is extensively differentially spliced. In the shortest cardiac-specific N2B titin isoform (linked to inclusion of exon 49), exon 50 is spliced direcdy to exon 225. In more compliant cardiac and skeletal titin isoforms, exon 50 is spliced to exon 51 (linked to additional inclusion of exons in the segment 52-224). [Pg.112]

Labeit, D., Watanabe, K., and Witt, C. (2003). Calcium dependent molecular spring elements in the giant protein titin. Proc. Natl. Acad. Sci. USA Oct 30. [Pg.117]

Watanabe, K., Nair, P., and Labeit, D. (2002b). Molecular mechanics of cardiac titin s PEVKand N2B spring elements./. Biol. Chem. 277, 11549-11558. [Pg.120]

Figure 1.2 illustrates the multiple-lumped resonator apparatus and the associated electronics. A resonator consists of a stack of five cylindrical lumps joined by cylindrically shaped torsional spring elements of smaller diameters. The moment of inertia of each of the four lumps is... [Pg.7]


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See also in sourсe #XX -- [ Pg.264 , Pg.417 , Pg.421 , Pg.441 , Pg.449 , Pg.450 ]




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