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As shown in the previous example, we can use the .Step command to sweep the values of the damping capacitor and the damping resistor. If we use a range of 3 to 5 times the value of the real capacitor, we will sweep the damper capacitor from 42 to 70 F in steps of 14 F. We will sweep the damper resistor from one-half to twice the Zo of the lter, i.e., from 0.8 to 3.2 in 0.2- steps. The schematic for the fourth-order lter and its impedance response are shown in Fig. 3.9. Note that two 10-M resistors have been added. To aid circuit convergence, the resistors were added to the nodes that are purely reactive. The circuit listing and output le are shown below. A sweep of the maximum impedance as a function of the damping resistor and the damping capacitor was also performed. The results of the sweep are shown in Fig. 3.10. Each curve is for a different value of damping capacitor.

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Instance variables (also called member variables) are variables defined at the class level. That means the variable declaration is not made within a method, constructor, or any other initializer block. Instance variables are initialized to a default value each time a new instance is created. Table 1-3 lists the default values for primitive and object types.

Equation (12-A) is true for the ideal condition in which all frequency components are delayed the same amount of time, T seconds, in passing through a network. Thus an sin n!t, applied at the INPUT, appears at the OUTPUT as bn sin n!t n bn sin n!t n!T

In the following example, the integer year is defined as a class member because it is within the initial curly braces of the class and not within a method s curly braces:

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public class BirthDate { int year; // Instance variable public static void main(String [] args) { BirthDate bd = new BirthDate(); bd.showYear(); } public void showYear() { System.out.println("The year is " + year); } }

where n n! T PHASE SHIFT in radians, where n! frequency; n 1; 2; 3; . . .). Thus we have the ratio n T n! 13-A

When the program is started, it gives the variable year a value of zero, the default value for primitive number instance variables.

4THORD: A 4TH ORDER FILTER .AC DEC 10 100HZ 1MEGHZ .PROBE .PARAM CDAMP=42u .PARAM RDAMP=0.8 .STEP PARAM CDAMP 42U 70U 14U .STEP PARAMRDAMP .8 3.2 .2 .PRINT AC V(4) VP(4) 1 1 0 5.7U C2 4 2 {CDAMP} R1 2 0 {RDAMP} I1 0 4 AC 1 L2 1 4 37U C3 4 0 14U R2 1 0 10MEG R3 4 0 10MEG L1 0 1 15U .END

TABLE 1-3

which, since T is constant for all frequencies in the ideal case, shows that, in order to have zero phase-shift distortion (constant time delay), the RATIO of PHASE SHIFT TO FREQUENCY must have the same constant value T at all frequencies.

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It s a good idea to initialize all your variables, even if you re assigning them with the default value. Your code will be easier to read; programmers who have to maintain your code (after you win the lottery and move to Tahiti) will be grateful.

Ordinary linear graph paper is not generally suitable for plotting frequency response curves One reason is that detection by the ear of a CHANGE IN FREQUENCY, f2 f1 , depends not only upon the value of f2 f1 but also upon the values of f2 and f1 themselves Thus, for example, an increase in frequency from 50 Hz to 70 Hz produces a CHANGE of 20 Hz which, as experience shows, would most de nitely be detected by the ear On the other hand, a frequency change from 7000 Hz to 7020 Hz would also produce a change of 20 Hz which, however, as experience shows, the ear would scarcely detect, if at all (The ear would, however, readily detect, for example, a change from 7000 Hz to 8000 Hz.

When compared with uninitialized primitive variables, Object references that aren t initialized are a completely different story. Let s look at the following code:

public class Book { private String title; public String getTitle() { return title; } public static void main(String [] args) { Book b = new Book(); System.out.println("The title is " + b.getTitle()); } }

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) Hence, what is needed is a type of horizontal frequency axis in which EQUAL DISTANCES represent larger and larger values of f2 f1 To show that a logarithmic scale meets this requirement, let us examine the horizontal axis in Fig 189, as follows In Fig 189 notice, for example, that a frequency change from 50 to 70 Hz occupies a distance of 02 inch, a frequency change from 500 to 700 Hz occupies the same distance of 02 inch, a frequency change from 5000 to 7000 Hz occupies the same distance of 02 inch, and so on Thus equal segments of distance on the axis have approximately EQUAL EFFECTS as far as the ear is concerned.

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