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It s time to fess up: The mysterious force that tells init when to change runlevels is actually the telinit command This command takes two command-line parameters One is the desired runlevel that init needs to know about, and the other is -t sec, where sec is the number of seconds to wait before telling init NOTE Whether init actually changes runlevels is its decision Obviously, it usually does, or this command wouldn t be terribly useful It is extremely rare that you ll ever have to run the telinit command yourself Usually, this is all handled for you by the startup and shutdown scripts NOTE Under most UNIX implementations (including Linux), the telinit command is really just a symbolic link to the init program Because of this, some folks prefer running init with the runlevel they want rather than using telinit

A reversible process: Is frictionless Is never more than differentially removed from equilibrium Traverses a succession of equilibrium states Is driven by forces whose imbalance is differential in magnitude Can be reversed at any point by a differential change in external conditions When reversed, retraces its forward path, and restores the initial state of system and surroundings The work of compression or expansion of a gas caused by the differential displacement of a piston in a cylinder is derived in Sec 17: d w =-pdvt (12)

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The xinetd and inetd programs are two popular services on Linux systems; xinetd is the more modern incarnation of the older inetd Strictly speaking, a Linux system can run effectively without the presence of either of them But some daemons rely solely on the functionality they provide So if you need either xinetd or inetd, then you need it, and there are no two ways about it The inetd and xinetd programs are daemon processes You probably know that daemons are special programs that, after starting, voluntarily release control of the terminal

The work done on the system is given by this equation only when certain characteristics of the reversible process are realized The first requirement is that the system be no more than infinitesimally displaced from a state of internal equilibrium characterized by uniformity of temperature and pressure The system then always has an identifiableset of properties, including pressure P The second requirement is that the system be no more than infinitesimallydisplaced from mechanicalequilibrium with its surroundingsIn this event, the internal pressure P is never more than minutely out of balance with the external force, and we may make the substitution F = P A that transforms Eq (11) into Eq (12) Processes for which these requirements are met are said to be mechanically reversible, and Eq (12) may be integrated:

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The reversible process is ideal in that it can never be fully realized; it represents a limit to the performance of actual processes In thermodynamics, the calculation of work is usually made for reversible processes, because of their tractability to mathematical analysis The choice is between these calculations and no calculations at all Results for reversible processes in combination with appropriate eficiencies yield reasonable approximations of the work for actual processes

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it s a fake block). The first thing I m going to do is attach a very small color keyboard to the e block so I can change the color. This color keyboard is a strange type of keyboard, though; it will only let me type colors. If I try to type in Jim or five, the keyboard will buzz to let me know that it s not going to cooperate. Take a look at the updated COLOR block in Figure 7-2.

h he simple procedure used here to find a correlation for G ~ / R T would no doubt be improved by a regression / procedure that determines the values of Azl and AI2 that minimize the sumof squares of theresiduals S ( G ~R T )

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