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Transmission line branched

After selection of the partition variable, the next step is to determine how the variable should be partitioned. It was decided to check each compressor in the branch of the transmission line associated with the partition variable, and if any compressor operated at less than 10 percent of capacity, it was assumed the compressor was not necessary in the line. (If all operate at greater than 10 percent capacity, the compressor with the smallest compression ratio was deleted.) For example, with N2 selected as the partition variable, and one of the three possible compressors in branch 2 of the gas transmission network operating at less than 10 percent of capacity, the first partition would lead to the tree shown in Figure E13.4c N2 would either be 3 or would be 0 < A2 < 2. Thus at each node in the tree, the upper or lower bound on the number of compressors in each branch of the pipeline is readjusted to be tighter. [Pg.475]

The nonlinear problem at node 2 is the same as at node 1, with two exceptions. First, the maximum number of compressors permitted in branch 2 of the transmission line is now two. Second, the objective function is changed. From the lower bounds, we know the minimum number of compressors in each branch of the pipeline. For the lower bound, the costs related to line B in Figure El3.4b apply for compressors in excess of the lower bound and up to the upper bound, the costs are represented by line A. [Pg.475]

For digital circuits, the electrical length of the line can be defined relative to the signal rise time. A common rule of thumb for simple lines with no branches is that interconnections must be treated as transmission lines when the round-trip transit time of the signal, 2t pdZ, exceeds the signal rise time, tr (37). This rule defines a critical line length (Zc) given by... [Pg.463]

Rugosity and porosity give rise to the so-called constant phase element (CPE), which can be described by groups of parallel or branched transmission lines. The CPE is manifested in real systems by an impedance spectrum altered from the expected shape, especially in the... [Pg.246]

From this physical model, an electrical model of the interface can be given. Free corrosion is the association of an anodic process (iron dissolution) and a cathodic process (electrolyte reduction). Ther ore, as discussed in Section 9.2.1, the total impedance of the system near the corrosion potential is equivalent to an anodic impedance Za in parallel with a cathodic impedance Zc with a solution resistance Re added in series as shoxvn in Figure 13.13(a). The anodic impedance Za is simply depicted by a double-layer capacitance in parallel with a charge-transfer resistance (Figure 13.13(b)). The cathodic branch is described, following the method of de Levie, by a distributed impedance in space as a transmission line in the conducting macropore (Figure 13.12). The interfacial impedance of the microporous... [Pg.256]

Here, the impedance response is independent of the working point, and the frequency dependence is determined solely by the material parameters of the composite. For / <linear branch appears only at frequencies co > a/Cfr). Doublelayer charging and proton transport dominate the overall electrode response in this regime, whereas Faradaic processes are insignificant due to the high frequencies. An equivalent representation of this system is an RC-transmission line [130], Since no fractality or branching of the network is assumed, the response resembles that of a Warburg impedance with a characteristic proportionality Z a where... [Pg.501]

An electrical grid is assiuned to consist of branches connected in nodes. A branch may consist of generators or power import branches, transmission lines, transformers and load or export branches. In addition contain these main components normally a lot of sub components or factors that can be classified as power transmitting components, protection and reclosing components, human factors and environmental factors. A composite reliability model for each branch is build by model composition taking into account all relevant components and their probability interactions. A typical branch model may have from 1000 to 20.000 composite reliability states. These composite branch models are finally reduced by model aggregation... [Pg.2108]

Figure 2.1.18. A branched transmission line circuit which shows CPE behavior. Figure 2.1.18. A branched transmission line circuit which shows CPE behavior.
This chapter is organized as follows. We start with a representation of the transmission line as two conductors in section 2. We describe the set up experimental in section 3. The next section deals with experimental determination of channel impedance and propagation constant. In section 5, the power channel model is established. In section 6 the proposed deterministic method is generalized to network with N nodes and M branches. Section 7... [Pg.1]

In our study, we have P sections of transmission lines with lengths Ip is connected to a node m, Zbrjj is the load at the terminal of each branch and Zcdij is the characteristic impedance for the node i of the j transmission hne branch. Tp is the transmission matrix of the last section P. Tdi is the equivalent transmission matrix of branches connected at node i given by ... [Pg.8]

Supercapacitor modeling enables us to predict their behavior in different apphcations, on the basis of a representation of the main physical phenomena occurring in the coirqxment. There are many different models for snpeicapacitors (two-branch model, model based on a transmission line, single-pore model, multi-pore model, etc.) [BEL 01 HAM 06]. These models are in the form of equivalent electrical circuits. Using them, we can describe the supercapacitor s behavior quite accurately. [Pg.226]

The problem of pulse voltage technique can be approached in one of two equivalent ways. The first method involves the transmission line approach which considers the channel as an infinite resistance-capacitance ladder. The current flowing through the channel divides up into these two branches at every point, one that charges up... [Pg.76]

Kinetics in the film can also be affected by the formation of pores and pits that according to the De Levie theory will modify the EIS response. Formation of active-passive corrosion pits on 304 stainless steel exposed to a sodium-chloride corrosive solution can be represented by the electrical equivalent circuit composed of two parallel branches [48,49]. The first branch represents the surface area without active pits (passive layer), where only inactive pits are present, and the second branch corresponds to the impedance of the active pits. The impedance inside the inactive pits can be represented by a transmission line, according to De Levie (Eq. 7-66). For relatively high frequencies the impedance of such a circuit can be represented by the passive layer film capacitance Cpj in parallel with the impedance in the passive pores or inactive pits Zpppp = Z,p ( tion 7-5) ... [Pg.314]

The transmission lines shown in Fig. 2 are such that the distributed capacitance Cp represents the Poisson branch and parallel branches represent each charged species. Figure 2a describes the single Warburg impedance for a single z+ z salt. This leads to an alternative approach of the charged species movement supposed to follow a difiusion migration process. If the concentrations are supposed to be distance-independent, the impedance is quite easy to obtain. If not, the derivation is more intricate and needs nmnerical techniques. [Pg.163]

Then, the two models give equivalent results. This calculation was also given by Buck without the electroneutrality hypothesis (i.e. Cp 0). The transmission line approach is often called the porous model of a conducting polymer as electrons are supposed to cross the polymer (phase 1) and ions are supposed to move into pores, filled by electrolyte, represented by the second branch of the transmission line. It is noticeable that the transmission line approach allows more complicated kinetics to be tested for a two-species problem, e.g. charge transfer in parallel to the capacity Ce(x) and C,- (x), or diffusion of the ion in the ionic pores , i.e. to introduce complex impedances instead of the real resistance p and/or p2, of the pure capacitances Ci and/or C2. It also allows position-dependent parameters to be introduced to mimic concentration gradients in the polymer [Cj(x) constant]. [Pg.167]

Fig. 11 The scattering properties of a five branches - four electrodes molecular bridge, (a) Detailed atomic structure of the molecule. A central perylene branch was included to mimic an internal measurement branch, (b) EHMO-ESQC calculated T12(E) transmission coefficient (plain) and predicted T12(E) transmission coefficient (dashed), applying the intramolecular circuit rules discussed for the four molecular fragments given in Fig. 12. The dashed (dotted) line is the Ti2(E) variation for the single molecular branch, as presented in the inset, to show the origin of the destructive interference... Fig. 11 The scattering properties of a five branches - four electrodes molecular bridge, (a) Detailed atomic structure of the molecule. A central perylene branch was included to mimic an internal measurement branch, (b) EHMO-ESQC calculated T12(E) transmission coefficient (plain) and predicted T12(E) transmission coefficient (dashed), applying the intramolecular circuit rules discussed for the four molecular fragments given in Fig. 12. The dashed (dotted) line is the Ti2(E) variation for the single molecular branch, as presented in the inset, to show the origin of the destructive interference...
The other difference between copper and tin electro-deposits is their microstracture. From the transmission electron microscope analyses, it proved that the branches of copper are a polycrystal-line structure, including a lot of nano-sized pores inside them, whereas the branches of tin are a single crystal without internal pores and grain boundaries. The poly crystallinity of copper branch is attributed to... [Pg.309]


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