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In the above it might seem, at rst glance, that the entire denominator could be reduced to 1, since, in practical work, d and k are both very much less than 1. This, however, will not be the case because in practical work Q will generally be much greater than 1 (a value of Q 100 is entirely possible). Thus products of the forms dQ and kQ can have signi cant values, and hence must not be dropped from the denominator. " In the above equation the voltage gain G is expressed in complex form. However, in " most work it will be su cient to know only how the magnitude of G varies with frequency. With this in mind, let us write eq. (412) in the form kQ2 " jGj G gm !0 L q 1 k2 Q2 4d 2 Q2 2 16d 2 Q2 413

1. 2. 3. 4. import java.io.*; public class MyProgram { public static void main(String args[]){ FileOutputStream out = null;

5. 6. 7. 8. 9. 10. 11. 12. 13. 14. 15. 16.

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In the above, remember that d is the fractional deviation of any frequency ! from the resonant frequency !0 (thus d 0 for ! !0 ). What we now wish to investigate is how the value of k a ects the way in which G varies relative to the value of d. That is, how the value of k a ects the shape of the curve of G versus d. As an illustration of how G varies with d, let s rst consider a speci c value, after which we ll point out some practical, general conclusions regarding Fig. 232. Let us take, as our example, the case for Q 50 (a reasonable value). Then, for this value of Q (and omitting the constant multiplier gm !0 L), eq. (413) becomes 2500k G q 1 2500k2 10,000d 2 2 40,000d 2 414

further reduced by using a higher order active lter (which will reduce the corner frequency of the existing lters) or replacing the quasisquare waveform with a more sophisticated waveform in order to eliminate several additional harmonics. Care must be taken in the placement of the lters, because component tolerances can easily alter the angles between phases. A Monte Carlo simulation can be performed to analyze the effect of component tolerances on the phase angles (and amplitudes) of the sine-wave outputs. The resulting ltered sine-wave output is shown in Fig. 7.16.

try { out = new FileOutputStream("test.txt"); out.write(122); } catch(IOException io) { System.out.println("IO Error."); } finally { out.close(); } } }

in which we ll take d as the independent variable and k, the coe cient of coupling, as a parameter whose e ect we wish to investigate. In regard to k, it should be noted that what is called critical coupling is de ned as being equal to 1=Q. Thus, if kc denotes critical coupling, we have that kc 1=Q. Hence, in the present example we have that kc 1=50 0:02 2%. In the above example it will be interesting to plot the curves of G versus d for several di erent values of the parameter k; let us select the values k 0:01, k kc 0:02, k 0:03. To do this, we successively substitute into eq. (414) the chosen values of k, with the results shown in the table below, with nal calculator values rounded to one decimal place.

and given that all methods of class FileOutputStream, including close(), throw an IOException, which of these is true (Choose one.)

A. This program will compile successfully. B. This program fails to compile due to an error at line 4. C. This program fails to compile due to an error at line 6. D. This program fails to compile due to an error at line 9. E. This program fails to compile due to an error at line 13. 14. Given the following,

Value of G for k 0:01 20.0 17.7 12.4 5.2 2.6 1.5 Value of G for k 0:02 25.0 24.8 22.4 11.2 5.4 3.1 Value of G for k 0:03 23.1 23.7 24.9 18.4 9.0 5.0

The circuit in Fig. 7.17 demonstrates another stepped waveform. Although the 120 conduction angle of the circuit in Fig. 7.14 eliminated the third harmonic, this waveform can eliminate all harmonics up to the eleventh harmonic. Resistors R1 through R5 form a cheap and dirty D/A converter, while the ampli er circuit is con gured as a bandpass lter. This circuit can be used as a reference circuit but is also widely used in power stages. When used in a power stage, the stepped waveform is generally created by summing the outputs of several transformers, each

1. 2. 3. 4. 5. 6. 7. 8. 9. 10. 11. 12. 13. 14. 15. public class MyProgram { public static void throwit() { throw new RuntimeException(); } public static void main(String args[]){ try { System.out.println("Hello world "); throwit(); System.out.println("Done with try block "); } finally { System.out.println("Finally executing "); } } }

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