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(a) Move R vertically upward by one unit to form a new region R . The line y = 1 moves up to become the x-axis. R is bounded above by y = x 2 + 1 and below by the line y = 1. The volume we want is obtained by revolving R

PART 5 APPENDICES Appendix A The RobotBASIC IDE A.1 The Editor Screen A.2 The Terminal Screen A.3 The Help Screen A.4 The Debugger Screen Appendix B The RobotBASIC Language B.1 Statements B.2 Comments B.3 Assignment Statements B.4 Command Statements B.5 Labels B.6 Flow-Control Statements

( 1)]2

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Fig. 33-16

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The distance determined in this manner is often referred to as the Euclidean distance in acknowledgment of its geometric origins, and the distance squared is known as the Euclidean distance metric. On this basis, the received codeword is closest to the 000 codeword, and the decoder would produce a binary 0 output. Soft decision decoding results in about a 2-dB reduction in the [Eb/N0] required for a given BER (Taub and Schilling, 1986). This reference also gives a table of comparative values for soft and hard decision coding for various block and convolutional codes. Clearly, soft decision decoding is more complex to implement than hard decision decoding and is only used where the improvement it provides must be had. 11.10 Shannon Capacity In a paper on the mathematical theory of communication (Shannon, 1948) Shannon showed that the probability of bit error could be made arbitrarily small by limiting the bit rate Rb to less than (and at most equal to) the channel capacity, denoted by C. Thus Rb C (11.17)

B.7.1 B.7.2 B.7.3 B.7.4 B.7.5 B.7.6 B.7.7 Numbers Strings Simple Variables Arrays Operators Constants Functions

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For random noise where the spectrum density is flat (this is the N0 spectral density previously introduced) the channel capacity is given by C W log2 a1 S b N (11.18)

Here, W is the baseband bandwidth, and S/N is the baseband signal to noise power ratio (not decibels). Shannon s theorem can be written as Rb W log2 a1 S b N (11.19)

1 2 + 5 3

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Letting PR represent the average signal power, and Tb the bit period then as shown by Eq. (10.17) the bit energy is Eb PRTb. The noise power is N WN0 and the signal to noise ratio is S N PR N Eb TbWN0 (11.20)

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The bit rate is Rb 1/Tb. Substituting this in Eq. (11.20) then in the inequality (11.19) gives Rb W log2 a1 R b Eb W N0 b (11.21)

(b) Move R two units to the right to form a new region R # [see Fig. 33-16(b)]. The line x = 2 moves over to become the y-axis. R # is bounded above by y = (x 2)2 and below by the x-axis and lies between x = 2 and x = 3. The volume we want is obtained by revolving R # about the y-axis. The cylindrical shell formula applies, V = 2 = 2

As noted in Sec. 10.6.3, the ratio of bit rate to bandwidth (Rb/W in the inequality (11.21) is an important characteristic of any digital system. The greater this ratio, the more efficient the system. The limiting case is when the inequality sign is replaced by the equal sign. Rb W log2 a1 R b Eb W N0 b (11.22)

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Keep in mind that this relationship is for the condition of arbitrarily small probability of bit error. A plot of Rb/W as a function of Eb/N0 is shown in

1 4 4 3 (3) (3) + 2(3)2 4 3

C.6.1 C.6.2 C.6.3 C.6.4 C.6.5 C.6.6 C.6.7 C.6.8 C.6.9 C.6.10 C.6.11 C.6.12 C.7.1 C.7.2 C.7.3 C.7.4 C.7.5 C.7.6 If-Then Statement If-ElseIf Statement For-Next Loop Repeat-Until Loop While-Wend Loop Break Statement Continue Statement Case Construct GoSub Statement OnError Statemet End Command Goto Statement Input and Output Commands Screen and Graphics Commands Array Commands Array Math Commands Other Commands DrawShape Details

6 5.75

5 (dB)

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1 4 4 3 (2) (2) + 2(2)2 4 3

Figure 11.10 Graph showing the Shannon limit, Eq. (11.22). The units for the y-axis are (bits/s)/Hz (a dimensionless ratio in fact). The points for BPSK and QPSK are evaluated for a Pe 10 5.

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