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Maximum phase advance

The open-loop transfer function is third-order type 2, and is unstable for all values of open-loop gain K, as can be seen from the Nichols chart in Figure 6.33. From Figure 6.33 it can be seen that the zero modulus crossover occurs at a frequency of 1.9 rad/s, with a phase margin of —21°. A lead compensator should therefore have its maximum phase advance 0m at this frequency. Flowever, inserting the lead compensator in the loop will change (increase) the modulus crossover frequency. [Pg.183]

The frequency of maximum phase advance is to occur at the frequency that corresponds to —180° on the Bode diagram constructed in section (a). The lower break frequency XjTx is to be half this value and the upper break frequency l/r2 is to be twice this value. Evaluate T and T2 and calculate values of 0 for the frequencies specified in section (a). Construct the Bode diagram for the compensation element for the condition K = X, and read off values of modulus at the same frequencies as the calculated phase values. [Pg.196]

The lead compensator contributes phase advance to the system and thus increases the overall system stability (Section 7.10.4). The degree of phase advance provided is a function of frequency. At the same time this type of compensator increases the overall system amplitude ratio, which has the effect of reducing the the stability of the system. However, the major contribution of phase advance occurs at those frequencies where the open-loop polar plot is adjacent to the (-1,0) point on the complex plane. The increase in amplitude ratio takes place at lower frequencies and, consequently, the effect of this is much less significant. As the ratio of r,/r2 is increased, the maximum phase advance supplied by the lead compensator also increases, i.e. the greater is the stabilising effect of the compensating element011. [Pg.641]

Figure 6.35 shows the Bode gain and phase for both compensated and uncompensated systems. From Figure 6.35, it can be seen that by reducing the open-loop gain by 5.4dB, the original modulus crossover frequency, where the phase advance is a maximum, can be attained. [Pg.184]

Fig. 2.19. Phase response curve for the phosphofructokinase allosteric model, indicating the phase shift caused by ADP addition. The phase shift A(P corresponding to a delay (A

0) or advance (A, over the period T = 312 s. The phase = 0 corresponds to the maximum in ADP concentration in the course of unperturbed oscillations, i.e. y= -/m = 42.4 the corresponding substrate concentration is a = 57.2. The phase shift is considered as phase advance when the first maximum induced by ADP addition exceeds the value (3/4)-yM. The two curves correspond, respectively, to the addition of a total of 14 units of y (0.7 mM ADP) within 2 s (open circles), and of 6 units of y (0.3 mM ADP) within 2 s (filled circles). Data are obtained by integration of eqns (2.7)-(2.8) for v = 0.5 s = 0.1 s ff = 8 s U = e = lOi c = 10 , e = 1, L = 5 X 10. ...

Fig. 2.19. Phase response curve for the phosphofructokinase allosteric model, indicating the phase shift caused by ADP addition. The phase shift A(P corresponding to a delay (A<P> 0) or advance (A<P< 0) of the oscillations is given as a fimction of the time of addition, 4>, over the period T = 312 s. The phase = 0 corresponds to the maximum in ADP concentration in the course of unperturbed oscillations, i.e. y= -/m = 42.4 the corresponding substrate concentration is a = 57.2. The phase shift is considered as phase advance when the first maximum induced by ADP addition exceeds the value (3/4)-yM. The two curves correspond, respectively, to the addition of a total of 14 units of y (0.7 mM ADP) within 2 s (open circles), and of 6 units of y (0.3 mM ADP) within 2 s (filled circles). Data are obtained by integration of eqns (2.7)-(2.8) for v = 0.5 s = 0.1 s ff = 8 s U = e = lOi c = 10 , e = 1, L = 5 X 10. ...
Phase-shift by ADP Delay of 1-2 min upon addition of 0.7 mM ADP (14 units of y) around the minimum of ADP oscillations of 5 min period small phase advance when the addition precedes ADP maximum Delay of 1.5 min upon addition of 0.7 mM ADP at the minimum of ADP oscillations of 5 min period small phase advemce when the addition precedes ADP maximum... [Pg.81]

In practice, it may be possible with care to float somewhat larger particles than those corresponding to the theoretical maximum. As illustrated in Fig. XIII-7, if the particle has an irregular shape, it will tend to float such that the three-phase contact occurs at an asperity since the particle would have to be depressed considerably for the line of contact to advance further. The resistance to rounding a sharp edge has been investigated by Mason and co-workers [62]. [Pg.474]

In TLC the stationary phase is pre-wet by volatile components in the mobile phase present in the vapour phase of the chromatographic chamber. The mobile phase is at the bottom of the developing chamber and advances on the stationary phase its movement depends on capillary forces. The stationary phase is equilibrated by the mobile phase front during its movement. Separations obtained under capillary flow controlled conditions are limited to a maximum of about 5000 theoretical plates. Forced-flow development requires an external force to move the mobile phase through the layer. [Pg.221]

In a sense each monolithic column is unique, or produced as a product of a separate batch, because the columns are prepared one by one by a process including monolith formation, column fabrication, and chemical modification. Reproducibility of Chro-molith columns has been examined, and found to be similar to particle-packed-silica-based columns of different batches (Kele and Guiochon, 2002). Surface coverage of a Chromolith reversed-phase (RP) column appears to be nearly maximum, but greater silanol effects were found for basic compounds and ionized amines in buffered and nonbuffered mobile phases than advanced particle-packed columns prepared from high purity silica (McCalley, 2002). Small differences were observed between monolithic silica columns derived from TMOS and those from silane mixtures for planarity in solute structure as well as polar interactions (Kobayashi et al., 2004). [Pg.157]

Irinotecan is an active chemotherapeutic agent that has been used in esophageal cancer and is also a potent radiosensitizer. In vitro studies have shown activity in esophageal cancer cell lines. A Phase I study has demonstrated its safety and tolerability with cisplatin. Phase I/II studies are currently underway determining the maximum tolerated weekly dose of irinotecan combined with concurrent radiation for locally advanced esophageal cancer (MSKCC 99081). [Pg.229]

The influence of neutral salts as well as of acids and bases on the swelling of gelatine which we have seen can be attributed to an apparent change in the solvation of the gel fibrils and may be interpreted in the light of Donnan s theory of the effect of a non-diffusible ion on the osmotic pressure differences between the two phases, is likewise to be noted in the alteration of the viscosity and alcohol precipitation values of protein solutions. From the considerations already advanced there should exist two well-defined maxima in the viscosity and alcohol precipitation curves when these properties are plotted as functions of the Ph, the maxima coinciding with the points of maximum dissociation of the salts... [Pg.320]

Time coverage includes the following stages close to maximum of light, early nebular phase and advanced nebular stage. [Pg.232]


See other pages where Maximum phase advance is mentioned: [Pg.187]    [Pg.644]    [Pg.187]    [Pg.644]    [Pg.207]    [Pg.645]    [Pg.235]    [Pg.422]    [Pg.159]    [Pg.164]    [Pg.179]    [Pg.75]    [Pg.165]    [Pg.518]    [Pg.494]    [Pg.565]    [Pg.274]    [Pg.319]    [Pg.152]    [Pg.245]    [Pg.72]    [Pg.99]    [Pg.119]    [Pg.227]    [Pg.287]    [Pg.16]    [Pg.917]    [Pg.294]    [Pg.505]    [Pg.319]    [Pg.318]    [Pg.252]    [Pg.237]    [Pg.224]    [Pg.65]    [Pg.1]    [Pg.132]    [Pg.18]    [Pg.479]    [Pg.480]   
See also in sourсe #XX -- [ Pg.187 , Pg.195 ]




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Phase advance

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