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Beam formulas

Much piping is supported from structures installed for other purposes. It is common practice to use beam formulas for tubular sections to determine stress, maximum deflection, and maximum slope of piping in spans between supports. When piping is supported from structures installed for that sole purpose and those structures rest on driven piles, detailed calculations are usually made to determine maximum permissible spans. Limits imposed on maximum slope to make the contents of the line drain to the lower end require calculations made on the weight per foot of the empty line. To avoid interference with other components, maximum deflection should be limited to 25.4 mm (1 in). [Pg.123]

This issue was addressed in 1979 by McBride and Jacobs. Jacobs was from Fluor in Houston. The principle was to calculate stresses in two distinct areas, membrane and bending. Membrane stresses are based on pressure area times metal urea. Bending is based on AISC beam formulas. The neck-and-shell section (and sometimes the flange as well) is assumed as bent on the hard axis. This is not a beam-on-elastic-foundation calculation. It is more of a brute-force approach. [Pg.203]

The stiffness can be calculated from beam formulae, and expressed as a deflection in radians per Nm of torque. [Pg.62]

Beam formulas for one-, two-, and three-span conditions. (From Johnston, D.W., Design and construction of concrete formwork, in Concrete Construction Engineering Handbook, Nawy, E.G., Ed., CRC Press, Boca Raton, FL, 1998, p. 7-33.)... [Pg.275]

Simple beam equations are used to determine the stresses on specimens at different levels of cross-head displacement. Using traditional beam formulas and section properties, the following relationships can be derived where Y is the deflection at the load point (refer to Fig. 3-19) ... [Pg.146]

Figure 5 shows the geometries of file crossed beam arrangement and the laser polarization (El) and gives the definitions of the angles used in the formulae for the alignment effects [14]. For each scattering system, the velocity vectors are calculated by standard molecular beam formulae, in order to determine the expected... [Pg.249]

Side drilled holes are widely used as reference reflectors, especially when angle beam probes are used (e.g. for weld testing). However, the distance law of side drilled holes is different to that of a flat bottomed hole. In the literature [2] a conversion formula is given which allows to convert the diameter of a side drilled hole into the diameter of a flat bottomed hole and vice versa, valid in the far field only, and for diameters greater than 1.5 times the wave length. In practical application this formula can be used down to approximately one nearfield length, without making big mistakes. Fig. 2 shows curves recorded from real flat bottomed holes, and the uncorrected and corrected DGS curves. [Pg.814]

The force and moment ia a constrained system can be estimated by the cantilever formula. Leg MB is a cantilever subject to a displacement of and leg CB subject to a displacement Av. Taking leg CB, for example, the task has become the problem of a cantilever beam with length E and displacement of Av. This problem caimot be readily solved, because the end condition at is an unknown quantity. However, it can be conservatively solved by assuming there is no rotation at poiat B. This is equivalent to putting a guide at poiat B, and results ia higher estimate ia force, moment, and stress. The approach is called guided-cantilever method. [Pg.61]

You will find the formulae for the elastic deflections of plates and beams under their own weight in standard texts on mechanics or structures (one is listed under Further Reading at the end of this chapter). We need only one formula here it is that for the deflection, 8, of the centre of a horizontal disc, simply supported at its... [Pg.68]

The square-section beam of length / (determined by the design of the structure, and thus fixed) and thickness t (a variable) is held rigidly at one end while a force F (the maximum service force) is applied to the other, as shown in Fig. 7.4. The same texts that list the deflection of discs give equations for the elastic deflection of beams. The formula we want is... [Pg.71]

Why, then, are bicycles not made of wood (There was a time when they were.) That is because metals, and polymers, too, can readily be made in tubes with wood it is more difficult. The formula for the bending of a tube depends on the mass of the tube in a different way than does that of a solid beam, and the optimisation we have just performed - which is easy enough to redo - favours the tube. [Pg.72]

Flere M 4 is the couple which must be applied at the mid span of the shaft to make (di//dx) o= 0 and Mg is the couple that is needed to cause the out-of-plane deflection of the end discs. Using the standard beam-bending formula of... [Pg.301]

The interpretive difficulty has been discussed in detail by Pawel and by Mortonin papers which appeared almost simultaneously. Both authors use arguments to show that the simple formula of bending-beam theory utilised by Stoney... [Pg.288]

Electrostatic Analyzer In magnetic-sector instruments, an electrostatic sector can be incorporated either before or after the magnet to provide energy resolution and directional focusing of the ion beam. The resolution achievable in these double-focusing instruments is sufficient to separate ions having the same nominal mass (e.g., 28 Daltons) but with different chemical formula (e.g., N2 and CO). [Pg.12]

This formula results in conservative accuracy, since the core does contribute to the stress-absorbing function. It also adds a built-in safety factor to a loaded beam or plate element when safety is a concern. [Pg.367]

The following calculation for carbon illustrates the use of a grating. The values = 0.75°, d = 8333 A, and A carbon Ka = 44,4 A substituted in the grating formula, give 6.3° for the angle between the grating and the first-order diffracted beam, which corresponds to a 26 of only 7°. [Pg.319]

Stem-Gerlach experiment The demonstration of the quantization of electron spin by passing a beam of atoms through a magnetic field, stick structure See line structure. stock solution A solution stored in concentrated form, stoichiometric coefficients The numbers multiplying chemical formulas in a chemical equation. [Pg.968]

Thus, if 5 = 1mm, / = 15.8 Hz. This very simple result is quite useful for approximately evaluating the gravity driven deflections of a stmeture given its natural frequency, or visa versa. Of course this was derived for a specific and very simple system, so it does not perfectly apply to more complex systems. Still it is a very useful rule of thumb. For a mass on the end of a cantilever beam, the above formula is correct. The lowest natural frequency of a massive cantilever beam is about 1.2 x the prediction of the above formula. [Pg.56]


See other pages where Beam formulas is mentioned: [Pg.1003]    [Pg.826]    [Pg.1007]    [Pg.254]    [Pg.254]    [Pg.257]    [Pg.381]    [Pg.382]    [Pg.383]    [Pg.384]    [Pg.384]    [Pg.1003]    [Pg.826]    [Pg.1007]    [Pg.254]    [Pg.254]    [Pg.257]    [Pg.381]    [Pg.382]    [Pg.383]    [Pg.384]    [Pg.384]    [Pg.217]    [Pg.220]    [Pg.322]    [Pg.210]    [Pg.211]    [Pg.484]    [Pg.145]    [Pg.300]    [Pg.111]    [Pg.138]    [Pg.205]    [Pg.321]    [Pg.159]   
See also in sourсe #XX -- [ Pg.384 ]




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Cantilever-beam formulas

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