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Norton Equivalent

For this example, we will find the Thevenin and Norton equivalent circuits for the circuit attached to the diode in EXERCI5E 3-5. The circuit is repeated below ... [Pg.182]

This circuit is difficult because it contains a nonlinear element (the diode) and a complex linear circuit. If we could replace VI, Rl, R2, and R3 by a simpler circuit, the analysis of the nonlinear element would be much easier. To simplify the analysis of the diode, we will find the Thevenin and Norton equivalent circuits of the circuit connected to the diode that is, we will find the Thevenin and Norton equivalents of the circuit below ... [Pg.182]

For determining the diode voltage and current, this circuit is much easier to work with than the original. This example is concerned with finding the numerical values of the equivalent circuit. The analysis of the circuit above was covered in Section 3.C. We will now find the Thevenin and Norton equivalent circuits of the circuit shown below ... [Pg.183]

EXEHCI5E 3-B Find the Thevenin and Norton equivalent circuits for the circuit below ... [Pg.187]

To determine the Norton equivalent impedance ZG in Figure 2.36, we can kill all the sources in circuit A and then calculate the impedance from n-n terminals by looking back into circuit A. Thus, the Norton impedance ZG is equal to the Thevenin impedance. The Norton current IQ is a constant current that remains the same regardless of the impedance of circuit B. It can be determined by... [Pg.75]

Note that only at the output terminals n-n are the Thevenin and Norton equivalents the same. In other words, at the output terminals n-n the voltage and current of the Thevenin equivalent circuit and the Norton equivalent circuit are identical. [Pg.75]

Fig. 13 Steps in the derivation of the Butterworth-van Dyke circuit, a Same as Fig. 6c with the circuit elements rearranged, b Norton equivalence Zx = aZ/, Zy = aZ, a = Z + Z )jZ. c Norton equivalence applied to b. c Same as c where the relation - 2/ sin(2x) + tan(x) =- cot(x) has been used. The two transformers have been merged... Fig. 13 Steps in the derivation of the Butterworth-van Dyke circuit, a Same as Fig. 6c with the circuit elements rearranged, b Norton equivalence Zx = aZ/, Zy = aZ, a = Z + Z )jZ. c Norton equivalence applied to b. c Same as c where the relation - 2/ sin(2x) + tan(x) =- cot(x) has been used. The two transformers have been merged...
By permission, Norton Chemical Process Products Corp., Bull. SI-72 and Bull. PTP-1 other manufacturer s data are equivalent, f Also available in polypropylene (including glass reinforced) high density polyethylene, rigid PVC, fluorinated vinyls. [Pg.252]

Cost of the packing and its effect on the system costs must be considered, as some packings are much more expensive than others, yet produce very little improved performance. Table 9-17 presents some comparative information. The most common packings and hence the ones with the most available data are Raschig rings, Berl saddles, several saddle types and Pall Rings (Norton Co.) or equivalent. [Pg.280]

Figure 9-21C. Generalized pressure drop correlation essentially equivalent to Figure 9-21B. Used by permission of Norton Chemical Process Products Corp. Figure 9-21C. Generalized pressure drop correlation essentially equivalent to Figure 9-21B. Used by permission of Norton Chemical Process Products Corp.
Capture and PSpice can be used to easily calculate the Norton and Thevenin equivalents of a circuit. The method we will use is the same as if we were going to find the equivalent circuits in the lab. We will make two measurements, the open circuit voltage and the short circuit current. The Thevenin resistance is then the open circuit voltage divided by the short circuit current. This will require us to create two circuits, one to find the open circuit voltage, and the second to find the short circuit current. In this example, we will find the Norton and Thevenin equivalent circuits for a DC circuit. This same procedure can be used to find the equivalent circuits of an AC circuit (a circuit with capacitors or inductors). However, instead of finding the open circuit voltage and short circuit current using the DC Nodal Analysis, we would need to use the AC analysis. [Pg.182]

Figure 25.2 Constant-current source using a battery and series resistor, (a) Dummy (resistor) load (b) Norton s equivalent circuit for part a (c) electrolysis cell as the load. Figure 25.2 Constant-current source using a battery and series resistor, (a) Dummy (resistor) load (b) Norton s equivalent circuit for part a (c) electrolysis cell as the load.
For more complex current sources, it is necessary to employ Norton s theorem0 which states that any linear network of impedances and voltage sources can be substituted by an equivalent circuit containing a current source iN in parallel with an impedance 2 x, where iN is the current which flows when the output terminals of the network are short-circuited and 2EX is the network impedance with all source voltages put equal to zero and replaced by their internal impedances. [Pg.546]

Intalox saddles are available in ceramic only from the Norton Company. Packings that are normally considered equivalent to the Intalox saddles are marketed under the trade names of Flexisaddle by Koch Engineering Company, Inc. and Novalox saddles by Jaeger... [Pg.425]

Other methods to simplify the circuit are Thevenin s and Norton s theorems. These two theorems can be used to replace the entire circuit by employing equivalent circuits. For example, Figure 2.34 shows a circuit separated into two parts. Circuit A is linear. Circuit B contains non-linear elements. The essence of Thevenin s and Norton s theorems is that no dependent source in circuit A can be controlled by a voltage or current associated with an element in circuit B, and vice versa. [Pg.74]

Similar to Thevenin s theorem, Norton s theorem states that a section of a linear circuit containing one or more sources and impedances can be replaced with an equivalent circuit model containing only one constant current source and one parallel-connected impedance, as shown in Figure 2.36. [Pg.75]

The corresponding constitutive law for steady state contains elements named after Arrhenius (T-dependence) and Norton (a-dependence), both of them being strong functions of their parameters ds/dt = C o" exp(-QcyRT)-Even a small temperature difference would therefore produce an appreciable difference in the creep rate for a given applied stress, if the specimen was to be considered as a set of independent coaxial shells. This is equivalent to the... [Pg.15]

In a first step, we set the load on the back side of the crystal (left-hand side in Fig. 6a) to zero and short-circuit the respective port. In a second step we apply the Norton transformation (Fig. 13b). The circuit from Fig. 13c is fully equivalent to the circuit shown in Fig. 13a. The equivalence of Figs. 13c and 13d is based on the relation ... [Pg.100]

Figure 3.11. The reflectivity of a mixture of deuteropolyethylene propylene (d-PEP) at a volume fraction of 0.137, in its hydrogenous equivalent. Segregation of the d-PEP at the surface results in the creation of a potential well for the neutrons, leading to an enhancement of incoherent scattering under resonant conditions. The result is that the reflectivity drops below unity at resonant k vector values below the critical value. After Norton et al. (1994). Figure 3.11. The reflectivity of a mixture of deuteropolyethylene propylene (d-PEP) at a volume fraction of 0.137, in its hydrogenous equivalent. Segregation of the d-PEP at the surface results in the creation of a potential well for the neutrons, leading to an enhancement of incoherent scattering under resonant conditions. The result is that the reflectivity drops below unity at resonant k vector values below the critical value. After Norton et al. (1994).
Calculate the current-flow on a given resistivity on an arbitrary DC circuit. Prove that this task could be solved by the minimization of the sum of dissipation fluxes or by the principle of minimal entropy production, like we did in the case of parallel connection of the Figure 6., when the circuit regarding the contacts of the resistor is replaced with the Norton s current source equivalent circuit [53]. [Pg.298]


See other pages where Norton Equivalent is mentioned: [Pg.182]    [Pg.546]    [Pg.182]    [Pg.546]    [Pg.743]    [Pg.546]    [Pg.107]    [Pg.42]    [Pg.427]    [Pg.442]    [Pg.463]    [Pg.4919]    [Pg.356]    [Pg.69]    [Pg.448]    [Pg.66]    [Pg.427]    [Pg.442]    [Pg.68]    [Pg.359]   
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