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Square wave excitation

In addition we have to take into consideration the conservation of charge. The charge balance equation reads [Pg.188]

Therefore, from (3.10.17) we obtain the following equation for the curvature [Pg.189]

T is the decay time for curvature, and rj is an effective viscosity coefficient given by [Pg.189]

Equations (3.10.14) and (3.10.18) are two coupled equations which cannot be solved analytically for any general value of Ej t) since y itself depends on E and t. However for a square wave [Pg.189]

In this case y remains constant in any half-period and the solutions are simpler and enable a physical interpretation of many of the observed phenomena. If the solutions are taken in the form  [Pg.189]


Figure 23-21 Generation of a square-wave voltammetry excitation signal. The staircase signal in (a) is added to the pulse train in (b) to give the square-wave excitation signal in (c). The current response At is equal to the cuirent at potential I minus that at potential 2. Figure 23-21 Generation of a square-wave voltammetry excitation signal. The staircase signal in (a) is added to the pulse train in (b) to give the square-wave excitation signal in (c). The current response At is equal to the cuirent at potential I minus that at potential 2.
Ait us assume that a square-wave excitation potential /i jppi is applied to the working electrode for a period of lime I as shown in Figure 25-9a. Let us further assume lhat L pp, is large enough that the ratio Cp/c" in Hqualion 25-3 is 1(XX) or greater. Under this condition, the concentration of A at the electrode surface is. for... [Pg.724]

Fig. 3.10.5. Threshold voltage versus frequency for MBBA. Sample thickness 50/ m. Open circles sinusoidal excitation triangles square wave excitation. (After the Orsay Liquid Crystals Group. )... Fig. 3.10.5. Threshold voltage versus frequency for MBBA. Sample thickness 50/ m. Open circles sinusoidal excitation triangles square wave excitation. (After the Orsay Liquid Crystals Group. )...
Fig. 3.10.8. Time dependence of the charge q and the curvature ij/ over one period of the square wave excitation, (a) Conduction regime (cot < 1, T > r). The charges oscillate but the domains are stationary, (b) Dielectric regime (cot P I, T< t). The charges are stationary and the domains oscillate. (After Smith et... Fig. 3.10.8. Time dependence of the charge q and the curvature ij/ over one period of the square wave excitation, (a) Conduction regime (cot < 1, T > r). The charges oscillate but the domains are stationary, (b) Dielectric regime (cot P I, T< t). The charges are stationary and the domains oscillate. (After Smith et...
Fig.II.3.1 Scheme of the square-wave excitation signal. E cc starting potential to delay time sw SW amplitude AE scan increment r SW period if forward current /b backward current, and ( ) points where they were sampled... Fig.II.3.1 Scheme of the square-wave excitation signal. E cc starting potential to delay time sw SW amplitude AE scan increment r SW period if forward current /b backward current, and ( ) points where they were sampled...
Figure 8.31 Simple arrangement for time domain measurements and the corresponding waveforms when using a square wave excitation. VappHed is the stimulus and voltage across the MUT (Vmut) the voltage response. is a measuring resistor. T is the duration of one period. Vj=o is the voltage immediately after a positive step and Vy/2 the voltage immediately before a... Figure 8.31 Simple arrangement for time domain measurements and the corresponding waveforms when using a square wave excitation. VappHed is the stimulus and voltage across the MUT (Vmut) the voltage response. is a measuring resistor. T is the duration of one period. Vj=o is the voltage immediately after a positive step and Vy/2 the voltage immediately before a...
We will now discuss the simplest equivalent circuits mimicking the immittance found in tissue measurements. In this section, the R-C components are considered ideal that is, frequency independent and linear. Immittance values are examined with sine waves, relaxation times with step functions. A sine wave excitation results in a sine wave response. A square wave excitation results in a single exponential response with a simple R-C combination. [Pg.335]

The threshold conditions Eth, Wth are found from (5.61) by the same procedure as for (5.39). For a square wave excitation with frequency / and amplitude E... [Pg.271]


See other pages where Square wave excitation is mentioned: [Pg.158]    [Pg.90]    [Pg.91]    [Pg.36]    [Pg.263]    [Pg.183]    [Pg.187]    [Pg.513]    [Pg.875]    [Pg.332]    [Pg.492]    [Pg.553]    [Pg.406]   


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