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cylinder This means that gravity-induced pressure gradients in the gas are very small relative to its pressure and that changes in potential energy of the gas are negligible in comparison with the potential-energy changes of the piston assembly The piston in Fig 22 confines the gas at a pressure just sufficient to balance the weight of the piston and all that it supports This is a condition of equilibrium, for the system has no tendency to change Mass must be removed from the piston if it is to rise Imagine first that a mass m is suddenly slid from the piston to a shelf (at the same level) The piston assembly accelerates upward, reaching its maximum velocity at the point where the upward force on the piston just balances its weight Its momentum then carries it to a higher level, where it reverses direction If the piston were held in this position of maximum elevation, its potential-energy increase would very nearly equal the work done by the gas during the initial stroke However, when unconstrained, the piston assembly oscillates, with decreasing amplitude, ultimately coming to rest at a new equilibrium position at a level above its initial position

contextfillStyle = "rgb(166,42,42)";

for(int i=0; i<8; i++) mystack2push(i); // pop those numbers off the stack Systemoutprintln("Stack in mystack1:"); for(int i=0; i<5; i++) Systemoutprintln(mystack1pop()); Systemoutprintln("Stack in mystack2:"); for(int i=0; i<8; i++) Systemoutprintln(mystack2pop());

contextstrokeStyle = "rgba(218, 112, 214, 04)";

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The oscillations of the piston assembly are damped out because the viscous nature of the gas gradually converts gross directed motion of the molecules into chaotic molecular motion This dissipative process transforms some of the work initially done by the gas in accelerating the piston back into internal energy of the gas Once the process is initiated, no injinitesimal change in external conditions can reverse its direction; the process is irreversible All processes carried out in finite time with real substances are accompanied in some degree by dissipative effects of one kind or another, and all are therefore irreversible However, one can imagine processes that are free of dissipative effects For the expansion process of Fig 22, such effects have their origin in the sudden removal of a finite mass from the piston The resulting imbalance of forces acting on the piston causes its acceleration, and leads to its subsequent oscillation The sudden removal of smaller mass increments reduces but does not eliminate this dissipative effect Even the removal of an infinitesimal mass leads to piston

Notice that the program creates two stacks: one five elements deep and the other eight elements deep As you can see, the fact that arrays maintain their own length information makes it easy to create stacks of any size

TABLE 3-15

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3:

It is possible to define a class within another class; such classes are known as nested classes The scope of a nested class is bounded by the scope of its enclosing class Thus, if class B is defined within class A, then B is known to A, but not outside of A A nested class has access to the members, including private members, of the class in which it is nested However, the enclosing class does not have access to the members of the nested class There are two types of nested classes: static and non-static A static nested class is one which has the static modifier applied Because it is static, it must access the members of its enclosing class through an object That is, it cannot refer to members of its enclosing class directly Because of this restriction, static nested classes are seldom used The most important type of nested class is the inner class An inner class is a non-static nested class It has access to all of the variables and methods of its outer class and may refer to them directly in the same way that other non-static members of the outer class do Thus, an inner class is fully within the scope of its enclosing class The following program illustrates how to define and use an inner class The class named Outer has one instance variable named outer_x, one instance method named test( ), and defines one inner class called Inner // Demonstrate an inner class class Outer { int outer_x = 100;

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