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Forcing functions, impulse function

An impulse function (F) is also useful in some problems where the force exerted on bounding surfaces is desired ... [Pg.280]

The forcing function of transform A is an impulse of magnitude K. The response to... [Pg.316]

Tributary area for sidesway load is equal to Vt the wall base to eave height. Use the wall blast load impulse for the forcing function. [Pg.247]

The first term on the right-hand side of eqn. (11) decays away and, after a time approximately equal to 5t, the second term alone will remain. Note that this is a sine wave of the same frequency as the forcing function, but that its amplitude is reduced and its phase is shifted. This second term is called the frequency response of the system such responses are often characterised by observing how the amplitude ratio and phase lag between the input and output sine waves vary as a function of the input frequency, k. To recover the system RTD from frequency response data is more complex tnan with step or impulse tests, but nonetheless is possible. Gibilaro et al. [22] have described a short-cut route which enables low-order system moments to be determined from frequency response tests, these in turn approximately defining the system transfer function G(s) [see eqn. (A.5), Appendix 1]. From G(s), the RTD can be determined as in eqn. (8). [Pg.232]

Only the special case of the impulse will be considered (Section 7.8.1). This is a particularly useful function for testing system dynamics as it does not introduce any further s terms into the analysis (equation 7.78). The determination of the response of any system in the time domain to an impulse forcing function is facilitated by noting that ... [Pg.603]

Fig. 7.30. Response of first-order system to unit impulse forcing function... Fig. 7.30. Response of first-order system to unit impulse forcing function...
Commonly encountered forcing functions (or input variables) in process control are step inputs (positive or negative), pulse functions, impulse functions, and ramp functions (refer to Figure 44). [Pg.210]

The responses in Fig. 3.8 are calibrated results by two methods of the sensor calibration. One is a calibration method by NIST, as illustrated in Fig. 3.10 (Breckenridge 1982). A large steel block of 90 cm diameter and 43 cm deep was employed. As a step-function impulse, a glass capillary source was employed, and elastic waves were detected by a capacitive transducer and by a sensor under test. The calibration curve was obtained as a ratio of the response of the sensor to that of the eapacitive transducer. The capacitive transducer (sensor) could record a Lamb s solution due to surface pulse as discussed in Chapter 7. It is reasonably assumed that the capacitive transducer detect the vertical displacement at the surface due to a step-function force. The other is known as a reciprocity method, which Hatano and Watanabe (Hatano Watanabe 1997) suggested to use, and confirmed an agreement with the NIST methods. As seen in Fig. 3.8, it is demonstrated that both method can provide similar calibration curves. [Pg.30]

In this first study, the vehicle model is exercised as it travels over the curb at a constant forward speed, Vf = 5 m/s. This high forward speed generates a severe velocity input that approximates an impulse function the duration of the input is only 0.1 s. The activity is calculated as a function of time by setting the lower bound, Ti, to zero and varying the time window, T, of the integration in (2.2). As shown in Fig. 2.7, the activities remain at zero until the vehicle hits the curb, at which point power starts to flow into the system. The activities increase due to the nonzero power flow until they approach a steady-state value as the system transients die out. Note the discontinuity in the slope of the activities (especially for tire stiffness and damping) at around 1.5 s. The high forward speed causes the wheel to lift off as the vehicle drives over the curb and contact is restored at about 1.5 s. This causes an impact force that results in the rapid increase in the activities. [Pg.66]

Figure III.22 shows the adhesive force as a function of the temperature of the surrounding medium. It should be noticed that, in determining the adhesion by centrifuging (curves 1 and 2) the dusting was carried out at a specified temperature in a thermostat and the centrifuging at 16-18°C this constitutes a disadvantage of the method. On detaching a monolayer of particles 30 /x in diameter by the impulse process, when the whole process (from depositing the dust to detachment of the latter) is carried out in a single thermostat, i.e., at the same temperature, analogous results are obtained (curve 3). Figure III.22 shows the adhesive force as a function of the temperature of the surrounding medium. It should be noticed that, in determining the adhesion by centrifuging (curves 1 and 2) the dusting was carried out at a specified temperature in a thermostat and the centrifuging at 16-18°C this constitutes a disadvantage of the method. On detaching a monolayer of particles 30 /x in diameter by the impulse process, when the whole process (from depositing the dust to detachment of the latter) is carried out in a single thermostat, i.e., at the same temperature, analogous results are obtained (curve 3).
The qualification conditions should be compared with the demand, usually represented by vibration, impact or impulse forcing functions at the anchoring on the structural support, but very stringent requirements could be derived by functionality under conditions of dust, smoke, humidity, cold temperatures or corrosive atmospheres, combined with stress. Adequate safety margins should be provided according to the item classification. [Pg.30]

For impact analysis of stiff or massive structures, load-time functions are generally preferred to define the impulse loading applied to the structure, since the influence of the structural behaviour on the characteristic of the forcing function is expected to be minor. [Pg.36]

Mechanisms of Cardiotoxicity Chemical compounds often affect the cardiac conducting system and thereby change cardiac rhythm and force of contraction. These effects are seen as alterations in the heart rate, conduction velocity of impulses within the heart, and contractivity. For example, alterations of pH and changes in ionic balance affect these cardiac functions. In principle, cardiac toxicity can be expressed in three different ways (1) pharmacological actions become amplified in an nonphysiological way (2) reactive metabolites of chemical compounds react covalently with vital macromolecules... [Pg.296]

The vertical spring and mass is an example of a stable system and by definition this means that an arbitrary small external force does not cause the mass to depart far from the position of equilibrium. Correspondingly, the mass vibrates at small distances from the position of equilibrium. Stability of this system directly follows from Equation (3.102) as long as the mechanical sensitivity has a finite value, and it holds for any position of the mass. First, suppose that at the initial moment a small impulse of force is applied, delta function, then small vibrations arise and the mass returns to its original position due to attenuation. If the external force is small and constant then the mass after small oscillations occupies a new position of equilibrium, which only differs slightly from the original one. In both cases the elastic force of the spring is directed toward the equilibrium and this provides stability. Later we will discuss this subject in some detail. [Pg.197]

We emphasize the link with the name of the already formed class of kick-excited self-adaptive systems and phenomena the external force is linked, through the function e(x), with the motion coordinate in an adaptive mode, and at the same time it exerts action in the form of short impulses much shorter than the oscillation period of the system. [Pg.111]

As it was already written above, we would like to study structural changes in the charge distribution between macroscopic objects, that is caused by the image forces, and depends on the wall-to-wall distance. To obtain direct structural information about the system, we will introduce a configurational analogue of the phase-space distribution function. At equilibrium, the definition of an fth order distribution function given by Eq. (12) can be applied to the equilibrium probability density [Eq. (13)], and the integration with respect to impulses can easily be carried out. We write for the rth order local density... [Pg.452]

The displacement response function x t, f) characterizes the average displacement (x(t) — x(to)) at time t, due to a unit impulse of force taking place at a previous time t < t. Is is easily deduced from the equation of motion (61), in which one adds to the random force F(t) a nonrandom force proportional to 5 (t — t ). One thus gets... [Pg.277]


See other pages where Forcing functions, impulse function is mentioned: [Pg.322]    [Pg.274]    [Pg.277]    [Pg.120]    [Pg.263]    [Pg.211]    [Pg.313]    [Pg.325]    [Pg.319]    [Pg.312]    [Pg.354]    [Pg.541]    [Pg.50]    [Pg.240]    [Pg.327]    [Pg.186]    [Pg.164]    [Pg.191]    [Pg.25]    [Pg.149]    [Pg.159]    [Pg.889]    [Pg.146]    [Pg.706]    [Pg.224]    [Pg.83]    [Pg.282]    [Pg.100]    [Pg.52]    [Pg.518]   
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