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The Thevenin equivalent of Fig. 59 appears in the solution to problem 56, and the Norton equivalent appears above. Setting RL 10 ohms in the Thevenin equivalent generator and applying Ohm s law, and setting GL 1=10 0:1 mho in eq. (67), we have that Thevenin case: IL 32:143=14:179 2:267 amperes; approx: Norton case: IL 0:7692308=0:339316 2:267 amperes; approx: there being some di erence beyond the third decimal place because the same degree of accuracy was not used in calculating in problem 56 as in problem 58.

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Note: Some, but not all, SPICE simulators allow the keywords Time, Freq, or Temp in B element expressions. Format: EnameN + N Value = {EXP R} Gname N + N Value = {EXPR}

3. In a method with a primitive return type, you can return any value or variable that can be implicitly converted to the declared return type.

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59. Let a, b be the output terminals of any given network; to convert the network into the Thevenin equivalent generator we must take the following two steps. (a) (b) Find the open-circuit voltage at the terminals a, b; this is the generated voltage, Vg , of the equivalent generator (Fig. 57). Find the resistance looking into the open-circuited terminals a, b; this is the internal resistance, Rg , of the equivalent generator (Fig. 57). Here we use the basic Ohm s law formula V RI 1=G I, thus V (b) Isc 6:155 56:468 volts Vg Gg 0:109

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4. In a method with a primitive return type, you can return any value or variable that can be explicitly cast to the declared return type.

Now apply the two steps to Fig. 60 (keeping the switch open), as follows. (a)

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One of these two poles is canceled by R4 and C3, which has a corner frequency of 1 F= = 1064 Hz 2 R4 C3

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We must now replace all generators with their internal resistances. In this case we must remember that a constant-current generator has INFINITELY GREAT internal resistance. Thus, as far as resistance is concerned, the constant-current generator has no shunting e ect on Gg , and thus 1=Gg 1=0:109 9:174 ohms Rg hence the Thevenin equivalent generator is

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60. First note that Fig. 63 contains 7 node points (including the zero-volt reference node at ground potential), but note that only two of the node voltages, at nodes 1 and 2, are unknown. Let us therefore begin by writing the Kirchho current law equations for nodes 1 and 2; if we take the current direction as they happen to be drawn in Fig. 63 we have at node 1: I1 I2 I3 I4 0 A at node 2: I4 I5 I6 0 B

package hierarchy. In other words, immediately inside the JAR there is a suncertify directory that contains a db directory, and the db directory contains the ExamProject.class file. What About Command-Line Arguments Your project s main application will almost certainly need command-line arguments. They might be used to pass host names and/or port numbers, or a variety of other configuration information. Most likely, though, your instructions will restrict you to a very small list of command-line arguments. For example, you might be instructed to use something like the following:

A third pole is caused by capacitor C2, which is used to provide maximum DC gain for regulation purposes. R5 provides a zero with C2 at a frequency of F= 1 = 338 Hz 2 R5 C2

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