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Here we wish to emphasize that time is required to change the amount of energy stored in the electric eld of a capacitor. To illustrate this, consider the basic series RC circuit, to which a constant voltage of V volts is applied at the closing of a switch, as shown in Fig. 21-A. We wish to examine the manner in which the VOLTAGE ACROSS THE CAPACITOR increases after the switch is closed. In Fig. 21-A, R is resistance in ohms, C is capacitance in farads, and i is current in amperes owing at any time t seconds after the switch is closed. We ll assume that initially (at t 0) there is zero voltage across the capacitor. We rst note that, at the instant the switch is closed at t 0, the capacitor momentarily behaves like a short circuit ; thus, at t 0 the current is equal to V/R amperes. Then, as time increases and the capacitor begins to charge, the current i decreases exponentially, in

Your instruction packet will probably require you to use certain technologies to implement your GUI for this project. If, for instance, your instructions indicate that you are to use Java Swing components and specifically the JTable component, not only do you have to use them, but you also need to use them appropriately. Before jumping in to implementing your GUI, you need to understand the strengths and weaknesses of the technologies you are using. In addition, each of the required technologies is meant to be used in a certain fashion for instance, if you re going to use a JTable, you ll want to use the appropriate models and listeners. The bottom line is, don t use a widget until you really understand how Sun intended for you to use it.

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Your exam instructions will probably say that the GUI you build should be flexible and relatively easy to extend. If so, you ll probably end up considering the Model View Controller (MVC) design pattern. We recommend that you do consider the MVC approach. If you are familiar with it, so much the better. If you are not, this is a good opportunity to study it. The MVC pattern has plenty of benefits:

the manner of Fig. 18-A, approaching the limiting value of zero. Thus, as time increases, the voltage across the capacitor rises, in an exponential-type curve, toward the nal limiting value of V volts. Letting vc denote the voltage across the capacitor, the relationship between vc and time t is shown graphically in Fig. 22-A, the equation of the curve being vc V 1 t=RC 7-A

It s very popular, and you re bound to run into it sooner or later. It anticipates that end users will ask for iteration after iteration of changes to

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Note that when t 0, then vc 0, as already mentioned and as shown in Fig. 22-A. Then, as time increases, the term t=RC decreases exponentially toward the value zero (as in Fig. 18-A). Thus, as t increases, the voltage vc increases toward the limiting value of V volts, as shown in Fig. 22-A. In Fig. 22-A, note that time is expressed in multiples of RC. This can be done because the product ohms times farads is time in seconds, as the following shows. First, by Ohm s law, R in ohms and then by eq. (184), C in farads hence, RC volts seconds coulombs seconds coulombs volts coulombs volts volts volts volts seconds amperes coulombs=sec coulombs

It scales well to large teams. It anticipates Java s write once run anywhere philosophy, reducing the

The product, ohms times farads, is called the time constant of the basic series circuit of Fig. 21-A. As Fig. 22-A shows, at the end of one time constant (RC seconds) the voltage across the capacitor has risen to 63% of its nal value of V volts. (To show this, set t RC in eq. (7-A).)

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effort required to port your GUI layer to additional environments such as browsers or mobile devices.

If you re instructed to use Swing (and we can virtually guarantee you will be), you must understand the Listener paradigm. Be certain that you understand how Swing components are meant to handle events, and how components relate to their models and their listeners. In addition, you should understand how inner classes are used to help implement these capabilities.

First, ! 2 f 2 =T, where T is time of one cycle (eq. (91), Chap. 5). Thus, since is simply the ratio of two lengths, we see that ! is basically measured in terms of 1=T, that is, in reciprocal seconds.

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