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Table 10-1 lists some /proc entries that you may find useful in managing your Linux system Note that this is a far cry from an exhaustive list For more detail, peruse the directories yourself and see what you find Or you can also read the proctxt file in the Documentation directory of the Linux kernel source code Unless otherwise stated, you can simply use the cat program to view the contents of a particular file in the /proc directory

Substitution of this equation into Eq (1325) provides an equilibrium expression displaying the pressure and the composition:

Contents Information about the CPU(s) in the system Internetworking Service Request (IRQ) usage in your system Displays a listing of the registered port regions used for input or output (I/O) communication with devices Displays the current map of the system s memory for each physical device Status of Redundant Array of Inexpensive Disks (RAID) configuration Status of memory usage This file represents the physical memory of the system Unlike the other files under /proc, this file has a size associated with it Its size is usually equal to the total amount of physical RAM available Same information produced as output from lsmod Information stored in this file can be used for diagnosing memory fragmentation issues Displays the parameters passed to the kernel when the kernel started up (boot time parameters) Status of swap partitions, volume, and/or files

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vi and P " is the standard-state pressure of 1 bar, expressed in the same units used where v for P The yi's may be eliminated in favor of the equilibrium value of the reaction coordinate E, Then, for a fixed temperature Eq (1326) relates E , to P In principle, specification of the pressure allows solution for E, However, the problem may be complicated by the dependence of $i on composition, ie, on E, The methods of Secs 116 and 117 can be applied to the calculation of $i values, for example, by Eq (1161) Because of the complexity of the calculations, an iterative procedure, initiated by setting Ji = 1 and formulated for computer solution, is indicated Once the initial set { Y ~ ) is calculated, {Ji) is determined, and the procedure is repeated to convergence If the assumption that the equilibrium mixture is an ideal solution is justified, then each $i becomes 4i, the fugacity coefficient of pure species i at T and P [Eq (118 I)] In this case, Eq (1326) becomes:

10:

Each 4; for a pure species can be evaluated from a generalized correlation once the equilibrium T and P are specified For pressures sufficiently low or temperatures sufficiently high, the equilibrium mixture behaves essentially as an ideal gas In this event, each $i = 1, and Eq (1326) reduces to:

In this equation the temperature-, pressure-, and composition-dependent terms are distinct and separate, and solution for any one of E,, T, or P, given the other two, is straightforward Although Eq (1328) holds only for an ideal-gas reaction, we can base some conclusions on it that are true in general: According to Eq (1314), the effect of temperature on the equilibrium constant K is determined by the sign of A H 0 Thus when A H 0 is positive, ie, when the standard reaction is endothermic, an increase in T results in an increase in K Equation (1328) shows that an increase in K at constant P results in an increase in ni(yi)"l ;this implies a shift of the reaction to the right and an increase in E, Conversely, when A H is negative, ie, when the standard reaction is exothermic, an increase in T causes a decrease in K and a decrease in ni(yi)">at constant P This implies a shift of the reaction to the left and a decrease in E,

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