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Similar to the previous two dialog classes, the MessageDialog constructor begins by calling its parent class constructor to specify that the dialog box is modal. Next, a switch statement is used to set the dialog box s title based on the type of message being created. The switch statement also serves to retrieve message fields from an original message supplied as an argument to the constructor (REPLY and FORWARD types). These original message fields are then used to populate MessageDialog s fields later in the constructor. Notice that the REPLY and FORWARD messages content is prefixed with text to denote the original message. After the switch statement has concluded, the fields panel is created, and each field s control is initialized and added to the panel. The content and buttons panels are set up next, and then all the panels are added to the display. Next, pack( ) is called to size the dialog box window to the minimum size required by its GUI controls. Finally, a call to setLocationRelativeTo( ) centers the dialog box over the parent window.

! 502

is the admittance matrix for the equivalent network. Another useful relationship can be found as follows. From eq. (497) we have z I V and hence (by section 11.3) I z 1 V Comparison of the last equation with eq. (503) shows that y z 1 504

The actionSend( ) method, shown here, confirms that all the message fields have been entered and then disposes the dialog box when the Send button is clicked:

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that is, the admittance matrix is the inverse of the impedance matrix (and vice versa, the impedance matrix is the inverse of the admittance matrix). Equations for the experimental determination of the values of the y coe cients can be found in the same general way as for the z coe cients. For example, if we apply a known voltage V1 to terminals 1; 1 in Fig. 277 and measure I1 with terminals 2; 2 shortcircuited, for which V2 0, solution of eq. (500) gives y11 I1 V1 V2 0 505

Another very useful description of the contents of the box is in terms of the hybrid or h parameters. In this system I1 and V2 are taken as the independent variables, and the simultaneous equations for the equivalent network are written in the form V1 h11 I1 h12 V2 I2 h21 I1 h22 V2 or, in matrix form, V1 I2 506 507

// Validate message fields and close dialog box. private void actionSend() { if (fromTextField.getText().trim().length() < 1

! 508

Note that eq (506) says that V1 volts volts volts, and thus, by Ohm s law, we see that h11 has the dimension of ohms, while h12 is simply a dimensionless ratio Likewise, eq (507) says that I2 amperes amperes amperes, and thus, by Ohm s law, we see that h21 is a dimensionless ratio while h22 has the dimension of reciprocal ohms ; that is, h22 has the dimension of 1=ohms mhos: In regard to the above, it should be mentioned that the following notation is also often used with the h parameters: h11 hi input impedance in ohms; h12 hr reverse voltage feedback factor; h21 hf forward current transfer ratio, h22 ho output admittance in mhos It should also be noted here that the h parameters (and also the y parameters) nd especially wide use in practical work involving transistors.

|| toTextField.getText().trim().length() < 1 || subjectTextField.getText().trim().length() < 1 || contentTextArea.getText().trim().length() < 1) { JOptionPane.showMessageDialog(this, "One or more fields is missing.", "Missing Field(s)", JOptionPane.ERROR_MESSAGE); return; } // Close dialog box. dispose(); }

One reason for this is that it is relatively easy to nd the values of these parameters by direct experiment in the laboratory From eq (508) note that the h-parameter matrix for the equivalent circuit is ! h11 h12 h h21 h22 So far we ve listed three pairs of simultaneous equations that can be used to describe the network inside the box in Fig 277 Thus, eqs (494) and (495) constitute the impedance or z form of the equations, eqs (500) and (501) the admittance or y form, and eqs (506) and (507) the hybrid or h form It s also possible to write three more pairs of such equations Of these three, the two pairs of principal interest are written in terms of what are generally called the g and a parameters, as follows, beginning with the g parameters.

I1 g11 V1 g12 I2 V2 g21 V1 g22 I2 and hence, in matrix form, I1 V2 509 510.

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