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Figure 2.9 is the reluctance model that represents the magnetic structure at the top of Fig. 2.8. Now we need to convert this reluctance model to an equivalent electric circuit model, but before we can do that, it will help to brie y review the duality transformation. We can then proceed to convert the reluctance model. An example of a duality transformation is given in Fig. 2.10. A node is placed within each mesh, including the outer mesh. Branches, which

/* *this is a block comment *it occupies several lines */

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* As you can from Fig. 362, this is closely true for samples taken near the maximum value of the analog wave, while increasingly less so for samples taken farther from the maximum.

Use a single line comment in the same place you would block comments, but for shorter descriptions. They should also be preceded by a blank line for readability, and we recommend the following form:

/* this is a single line comment */

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Fig. 362), and this e ect is increasingly great between samples taken farther from the maximum value. This is why the magnitude of the output decreases with increasing analog frequency (Fig. 359), and it is due to the fact that the amplitude of the high-frequency analog wave changes rapidly with time. Now consider Fig. 364. The gure is based upon the requirements of the basic sampling theorem (section 13.1), and illustrates the condition in which r has the maximum allowable value of r 0:5. In this condition the HIGHEST ANALOG FREQUENCY that can be sampled and allowed to enter a digital lter system is equal to one-half the sampling frequency the system uses. Thus two samples per cycle must be taken of the highest permitted frequency component of the analog signal; this is the condition shown in Fig. 364. From the gure, note that the algebraic sum of samples 1 and 2 is always zero; that is, the output of the lter of Fig. 358 is zero for the highest allowable frequency analog signal (as we see in Fig. 359).

It is acceptable to use this alternate form:

R1 =

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When you want to add a comment to the end of a line of code, use the aptly named end of line comment. If you have several of these comments in a row, make sure to align them vertically. We recommend the following form:

Problem 319 Rework the foregoing example for b0 1:0 and b1 1:0, as shown in Fig. 365. Problem 320 Here we wish to sketch the magnitude of the frequency response curve of the following low-pass digital lter.

doRiskyStuff(); doComplexStuff();

For the above, nd the values of jH r j for r 0; 0:1; 0:2; 0:3; 0:4; 0:5, then sketch the curve of jH r j versus r, from r 0 to r 0:5. Problem 321 Digital lters can be of the band-pass and band-elimination types as well as the lowpass and high-pass types. To illustrate this, consider Fig. 366, which is drawn in the Direct Form II con guration of Fig. 356 in section 13.8 (where, in this particular case, a1 and b1 are both equal to zero).

It is acceptable to use this alternate form:

doRiskyStuff() doComplexStuff(); /* this method might throw a FileNotFoundException /* instantiate the rete network */ */

(b c )

(a) (b)

Often in the course of developing software, you might want to mask a code segment from the compiler without removing it from the file. This technique is useful during development, but be sure to remove any such code segments from your code before finishing your project. Masking comments should look like this:

// // // // // // if (moreRecs == true) { ProcessRecord(); } else { doFileCleanUp(); }

Show that the given lter is stable. Fill in the following table of values for the given values of r, then sketch the curve of jH r j versus r.

It is important to use comments where the code itself may not be clear, and it is equally important to avoid comments where the code is obvious. The following is a classic, from the Bad Comments Hall of Fame:

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