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Now, going back to eq. (400), replace (XL XC ) with the right-hand side of the above equation. Next, in eq. (400), set Xm !M k!L (by eq. (371)) and also set XC 1=!C. Doing this, eq. (400) becomes " G r2 k2 !2 L2 jgm kL=!C2 4!2 L2 d 2 j4r!0 Ld 0 407

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1. 2. 3. 4. 5. 6. 7. int I = 0; label: if (I < 2) { System.out.print("I is " + I); I++; continue label; }

Next, what is called the Q factor of an inductor coil is universally de ned as the ratio of the REACTANCE of the coil to its RESISTANCE. If the coil appears in a resonant circuit, then we ll de ne the Q in terms of the resonant frequency of the circuit; thus Q !0 L r 408

Exceptions (Sun Objectives 2.3 and 2.4)

11. Given the following,

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where r is the total resistance in series with the coil, including any resistance the coil windings may have. One reason it s convenient to work in terms of Q is because it s easy to nd both the inductance of a coil and its Q by use of a standard piece of laboratory equipment called a Q-meter. Let us therefore write our equations in terms of Q; thus, noting that r !0 L=Q, eq. (407) becomes " G jgm kL=!C2 !2 L2 j4!2 L2 d 0 0 k2 !2 L2 4!2 L2 d 2 0 Q Q2 409

1. 2. 3. 4. System.out.print("Start "); try { System.out.print("Hello world"); throw new FileNotFoundException();

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5. 6. 7. 8. 9. 10. 11. 12.

We next might note that the second term in the denominator of the above equation can be written as 2 ! 2 2 2 2 2 2 2 2 2 2 2 k ! L k ! !0 L =!0 k !0 L !0 and, upon making this change, note that !2 L2 factors from the denominator. Doing this, 0 then multiplying the numerator and denominator by Q2 , eq. (409) becomes " G jgm LkQ2 =!C2 !2 L2 1 k2 Q2 !=!0 2 4Q2 d 2 j4Qd 0 410

} System.out.print(" Catch Here "); catch(EOFException e) { System.out.print("End of file exception"); } catch(FileNotFoundException e) { System.out.print("File not found"); }

and given that EOFException and FileNotFoundException are both subclasses of IOException, and further assuming this block of code is placed into a class, which statement is most true concerning this code

Now multiply the denominator by 1=!2 L2 and the numerator by !2 C 2 (which is per0 0 missible, because, by eq. (401), 1=!0 L !0 C). Doing this, eq. (410) becomes " G jgm !0 LQ2 !0 =! k 1 k2 Q2 !=!0 2 4Q2 d 2 j4Qd 411

A. The code will not compile. B. Code output: Start Hello world File Not Found. C. Code output: Start Hello world End of file exception. D. Code output: Start Hello world Catch Here File not found. 12. Given the following,

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At this point let s pause to consider some relationships that are known to exist in practical applications of Fig. 232. To make the rst point, note that, by eq. (404), ! 1 d !0 and therefore (see discussion following eq. (405)) it follows that, for almost all practical applications, it s perfectly permissible to write that (!=!0 !0 =! 1; hence, for practical purposes eq. (411) becomes " G jgm !0 LkQ2 1 k2 Q2 4d 2 Q2 j4dQ 412

1. 2. 3. 4. 5. 6. 7. 8. 9. 10. public class MyProgram { public static void main(String args[]){ try { System.out.print("Hello world "); } finally { System.out.println("Finally executing "); } } }

A. Nothing. The program will not compile because no exceptions are specified. B. Nothing. The program will not compile because no catch clauses are specified. C. Hello world. D. Hello world Finally executing 13. Given the following,

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