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file systems are mounted so that they appear as just another subdirectory on the system This helps to promote the illusion of one large directory tree structure, even though there may be several different file systems in use This characteristic is especially helpful to the administrator, who can relocate data stored on a physical partition to a new location (possibly a different partition) under the directory tree, with the system users being none the wiser The file system management process begins with the root directory This partition is also called slash and likewise symbolized by a slash character (/) The partition containing the kernel and core directory structure is mounted at boot time It is possible and usual for the physical partition that houses the Linux kernel to be on a separate file system, such as /boot It is also possible for the root file system ( / ) to house both the kernel and other required utilities and configuration files to bring the system up to single-user mode As the boot scripts run, additional file systems are mounted, adding to the structure of the root file system The mount process overlays a single subdirectory with the directory tree of the partition it is trying to mount For example, let s say that /dev/sda2 is the root partition It has the directory /usr, which contains no files The partition /dev/sda3 contains all the files that you want in /usr, so you mount /dev/sda3 to the directory /usr Users can now simply change directories to /usr to see all the files from that partition The user doesn t need to know that /usr is actually a separate partition NOTE In this and other chapters, we might inadvertently say that a partition is being mounted at such and such a directory Please note that it is actually the file system on the partition that is being mounted For the sake of simplicity, and in keeping with everyday verbiage, we might interchange these two meanings Keep in mind that when a new directory is mounted, the mount process hides all the contents of the previously mounted directory So in our /usr example, if the root partition did have files in /usr before mounting /dev/sda3, those /usr files would no longer be visible (They re not erased, of course once /dev/sda3 is unmounted, the /usr files would become visible again).

These equations establish a thermodynamic foundation for the activity coefficient, which appeared in Sec 105 as a factor introduced into Raoult's law to account for liquid-phase nonidealities Comparison with Eq (1147) shows that Eq (1188) relates yi to GE exactly as Eq (1147) relates $i to For an ideal solution, GE = 0, m therefore yi = 1 d An alternative form of Eq (1186) follows by introduction of the activity coefficient through Eq (1188):

Like many command-line tools, the mount command has a plethora of options, most of which you won t be using in daily work You can get full details on these options from the mount man page In this section, we ll explore the most common uses of the command The structure of the mount command is as follows:

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The generality of these equations precludes their direct practical application Rather, use is made of restricted forms, which are written by inspection:

where options may be any of those shown in Table 7-1 The options available for use with the mount -o flag are shown in Table 7-2

Equations (1189) through (1192) are analogs of Eqs (1152) through (1155) for residual properties Whereas the fundamental residual-property relation derives its usefulness from its direct relation to experimental P V T data and equations of state, the fundamental excessproperty relation is useful because V E , H ~and yi are all experimentally accessible Activity , coefficients are found from vaporniquid equilibrium data, and vE and H~ values come from mixing experiments, topics treated in the following chapter Equation (1192) demonstrates that In yi is a partial property with respect to GE/RT It is the analog of Eq (1 155), which shows the same relation of 1nJi to GR/RT The partialproperty analogs of Eqs (1190) and (1191) are:

These equations allow calculation of the effect of pressure and temperature on the activity coefficient

7:

The following forms of the summability and GibbsIDuhem equations result from the fact that In y is a partial property with respect to G ~ / R T : i

Description Mounts all the file systems listed in /etc/ fstab (this file is examined later in this section) Specifies the type of file system being mounted Linux can mount file systems other than the ext2 standard For example, File Allocation Table (FAT), Virtual File Allocation Table (VFAT), New Technology File System (NTFS), ReiserFS, etc The mount command can usually sense this information on its own Specifies options applying to this mount process These are usually options specific to the file system type (options for mounting network file systems may not apply to mounting local file systems)

These equations find important applications in phase-equilibrium thermodynamics Equations (1190) and (1191) allow direct calculation of the effects of pressure and temperature on the excess Gibbs energy For example, an equimolar mixture of benzene and cyclohexane at 29815 K (25 C) and 1 bar has an excess volume of about 065 cm3 molpl and an excess enthalpy of about 800 J mol-' Thus at these conditions, 065 = 262 x lop5 bar-' [ a ( G z T ) ] T , x = (8314)(29815)

Description Mounts the partition as read-only Mounts the partition as read/write (default) Permits the execution of binaries (default) Disables update of the access time on i-nodes For partitions where the access time doesn t matter, enabling this improves performance

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