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Note that h12 is the ratio of volts to volts and h21 is the ratio of amperes to amperes and hence are equal to pure numbers, and are thus said to be dimensionless quantities. Now, to illustrate why a parameter may carry a negative sign, let us suppose that the network inside the box in Fig. 277 happens to be a T network, as shown in Fig. 278, in which (for simplicity in making our point here) the elements all have equal values of R ohms.

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Now let us note, again, that eqs. (515) through (518) are de ned for the two di erent conditions of V2 0 and I1 0; with this in mind, consider Figs. 279 and 280. In these two gures, note that the voltage and current arrows are all drawn in the positive sense as de ned in accordance with Fig. 277.

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But also note that, although the T network itself is the same in both gures, the values of the voltages and currents will be completely di erent in the two gures. Therefore, just for this discussion, let us denote the values in Fig. 280 by I10 , I20 , V10 , and V20 , as shown. Then the equations will be, for the given arrow directions, & ' 2RI1 RI2 V1 case of V2 0 for Fig: 279: RI1 2RI2 0 & ' I20 V20 =2R for Fig: 280: case of I10 0 V10 RI20 V20 =2

// This class manages the e-mail table's data. public class MessagesTableModel extends AbstractTableModel { // These are the names for the table's columns. private static final String[] columnNames = {"Sender", "Subject", "Date"}; // The table's list of messages. private ArrayList messageList = new ArrayList(); // Sets the table's list of messages. public void setMessages(Message[] messages) { for (int i = messages.length - 1; i >= 0; i--) { messageList.add(messages[i]); } // Fire table data change notification to table. fireTableDataChanged(); } // Get a message for the specified row. public Message getMessage(int row) { return (Message) messageList.get(row);

Now, upon making use of the above relationships and eqs. (515) through (518), you should nd that h11 h12 V1 3R=2 I1 V10 1=2 V20 h21 h22 I2 1=2 I1 I20 1=2R V20

Thus, for the network of Fig. 278, h21 has a negative value. This happens because of the particular de nitions of the positive senses laid down in Fig. 277. To show this, suppose, in Fig. 279, that the positive sense of both I1 and I2 had been given to be in the clockwise sense. In that case, note that the equations for Fig. 279 would be 2RI1 RI2 V1 RI1 2RI2 0 in which case 2 V1 R I2 1 0 1=2 V1 1 I1 R 0 2

} // Remove a message from the list. public void deleteMessage(int row) { messageList.remove(row); // Fire table row deletion notification to table. fireTableRowsDeleted(row, row); } // Get table's column count. public int getColumnCount() { return columnNames.length; } // Get a column's name. public String getColumnName(int col) { return columnNames[col]; } // Get table's row count. public int getRowCount() { return messageList.size(); } // Get value for a specific row and column combination. public Object getValueAt(int row, int col) { try { Message message = (Message) messageList.get(row); switch (col) { case 0: // Sender Address[] senders = message.getFrom(); if (senders != null || senders.length > 0) { return senders[0].toString(); } else { return "[none]"; } case 1: // Subject String subject = message.getSubject(); if (subject != null && subject.length() > 0) { return subject; } else { return "[none]"; } case 2: // Date

illustrating how the sign of a parameter can depend upon the positive senses originally chosen in Fig. 277. Let us be reminded that our procedures are based upon the fact that sinusoidal voltages and currents can be represented as complex numbers and manipulated as vectors on the complex plane. Thus the vector diagram for the purely resistive circuit of Fig. 279, taking V1 as the reference vector, would have the form

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