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The getMessageContent( ) method, shown here, retrieves a message s content. Notice that this method is declared public and static so that it can be accessed from other classes without requiring a reference to the EmailClient class:

which is read A and B is equal to Z. In writing equations we usually omit the and symbol and just write AB, as shown in eq. (559), the expression AB again being read A and B.

It should be emphasized that eq. (559), A B AB Z, is simply a shorthand way of expressing the information contained in the truth table for Fig. 313. Equation (559) is valid because we have de ned that a b A; B; and Z can have only the values 1 and 0; and that 1 1 1; 1 0 0; 0 1 0; 0 0 0;

// Get a message's content. public static String getMessageContent(Message message) throws Exception { Object content = message.getContent(); if (content instanceof Multipart) { StringBuffer messageContent = new StringBuffer(); Multipart multipart = (Multipart) content; for (int i = 0; i < multipart.getCount(); i++) { Part part = (Part) multipart.getBodyPart(i);

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and with these rules agreed upon it s clear that the and operation of eq. (559), AB Z, does satisfy the truth table of Fig. 313 and thus represents the basic two-switch series connection of the gure. Also, since it s immaterial in what order switches are connected in series, it follows that either of the Boolean products, AB or BA, produces the truth table for Fig. 313. Thus Boolean multiplication is commutative, meaning that AB BA Z, just as in ordinary algebra. It s also apparent that the foregoing extends to any number of series-connected switches; for example, if A; B; C, and Z represent the 0 and 1 states of, say, three series-connected switches, thus

it will be noted that the truth table for this series connection is A B C Z 1 1 1 1 1 1 0 0 1 0 1 0 1 0 0 0 A 0 0 0 0 B 1 1 0 0 C Z 1 0 0 0 1 0 0 0

if (part.isMimeType("text/plain")) { messageContent.append(part.getContent().toString()); } } return messageContent.toString(); } else { return content.toString(); } }

which, given that 1 1 1 1; 1 1 0 0; 1 0 1 0; . . . ; 0 0 0 0, shows that the above truth table is represented by the Boolean algebraic equation A B C ABC Z, in which the Boolean product ABC is to be read as A and B and C. Likewise for any Boolean and product, ABCD Z, we have Z 1 only if all the variables are equal to 1; otherwise Z 0. Now let us continue, and examine Fig. 314 and its truth table. The truth table for Fig. 314 de nes what is called the OR operation, because Z 1 not only if A and B are both equal to 1, but also if either A or B is equal to 1, as inspection of the table shows. The truth table for Fig. 314 is de ned to be represented mathematically by the Boolean equation A B Z 560

in which the symbol does not mean plus in the usual sense but is now used to indicate the or relationship between A and B. Thus the quantity A B is to be read as A or B and not as A plus B. Remember that Boolean variables, such as A; B; Z, and so on, can have only the two values 1 and 0. With this in mind, and since eq. (560) is de ned to represent the truth table for Fig. 314, it follows that eq. (560) can have only the four possible states 1 1 1 1 0 1 0 1 1 0 0 0

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