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Let us continue with the symmetrical T of Fig. 203, which depicts the particular con" " " dition in which Zin ZL Z0 . As we know, eq. (340) applies to this condition and, in addition to eq. (340), several other useful relationships exist. As an aid in nding these relations let us begin by redrawing Fig. 203 as Fig. 207.

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By Kirchho s voltage law, the sum of the voltage drops AROUND ANY CLOSED PATH IN A NETWORK is equal to the sum of the generator voltages in that path. Thus,

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The log file is opened by way of creating a new PrintWriter instance for writing to the file. If the file cannot be opened, an error dialog box is displayed by calling showError( ). The crawling flag is set to true to indicate to the actionSearch( ) method that crawling is underway. The following code kicks off the actual search crawling by invoking the crawl( ) method:

in Fig. 207, around the closed path abcda we have that " " " " " " " V1 Z1 I1 =2 Z1 I2 =2 Z0 I2 " " " or, since V1 I1 Z0 ; " " " " " " " " Z0 I1 Z1 I1 =2 Z1 I2 =2 Z0 I2 from which we have the important relationship " Z1 " " I1 Z 0 2 " " I2 Z " Z0 1 2 342

Problem 177 " " " Find the ratio of I1 to I2 in Fig. 206 for the frequency at which Zin 2 ohms. (Answer: 0:500 j0:866 As you can see from the above, eq. (342) was derived for the particular frequency for " " " which Zin ZL Z0 . For any frequency in general, eq. (342) becomes " " " I1 ZL Z1 =2 " " " Zin Z1 =2 I2 " " in which ZL will be a given load impedance and Zin can be found by eq. (338). Problem 178 Derive eq. (343), using the same procedure as in deriving eq. (342). Problem 179 " " In Fig. 206, nd I1 =I2 for ! 200 rad/sec. 343

// Perform the actual crawling. crawl(startUrl, maxUrls, limitCheckBox.isSelected(), searchString, caseCheckBox.isSelected());

Problem 180 If the T network in problem 174 is terminated in its characteristic impedance, nd " " the magnitude and phase angle of I1 relative to I2 . It s important to note, here, that the equation for the current ratio can also be written " in the following form, in which ZL denotes ANY VALUE of load impedance: " " " I1 Z1 ZL 344 * " 1 2Z 2 Z 2 " " I2 " " Or, setting ZL Z0 , then making use of eq. (340), and noting that r s " " "2 Z2 Z1 1 Z1 " Z1 Z2 1 "2 " " 4 Z2 4Z2 Z2 " " eq. (344) becomes, for the special case in which ZL Z0 , s " " " " !2 I1 Z1 Z1 Z1 " " " 1 2Z2 Z2 2Z2 " I2

In the above, the actual contents of the box could, for example, consist of a series connection of ip- ops, or perhaps an array of charge-coupled devices. It will be a helpful reminder to conclude this section with a summary of certain algebraic operations that apply in the manipulation of z-transform equations. This is done in Table 2, with discussion below.

After crawling has completed, the crawling flag is turned off and the matches log file is closed, as shown here:

Table 2. 1. 2. 3. 4. Some Valid Operations in the z-Domain, where Zv nT F z Zav nT aF z , where a is constant Z v1 nT v2 nT F1 z F2 z Zan v nT F z=a , where a is constant Zv nT kT Zv n k T z k F z , where v n k T 0 for n < k. This is the timedelay theorem.

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