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There really isn t much difference between the master and slave devices; both use Bluetooth to communicate, but I would suggest making the master the robot that will have the most responsibilities. An example is a robot that sends a signal to another robot to move or make a sound or take a sensor reading. Sometimes multiple robots will all be running the same program and sending signals back and forth; in this case, pick any robot as master and the remaining robots (up to three more) will be configured as slave devices. Since you have four possible values, it s possible to connect the slave Bricks to one master Brick. This is what will allow you to control up to three additional robots with a single NXT robot.

Click OK when done 9 The completed Make LVM Volume Group dialog box should resemble the one shown here:

Except for high pressures, the exponential term is close to unity and may be omitted Then,

Click OK to close the dialog box 10 You will be returned to the main Disk Setup screen The final screen should be similar to the one shown here:

(1332)

and the only problem is determination of the activity coefficients An equation such as the Wilson equation [Eq (1219)]or the UNIFAC method can in principle be applied, and the compositions can be found from Eq(1332) by a complex iterative computer program However, the relative ease of experimental investigation for liquid mixtures has worked against the application of Eq (1332) If the equilibrium mixture is an ideal solution, then yi is unity, and Eq(1332) becomes:

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You will notice that we have some free unpartitioned space left under the device column This was done deliberately so that we can play with that space in a later chapter without necessarily having to reinstall the entire operating system to create free space 11 Click Next to complete the disk-partitioning portion of the installation

(1333)

NOTE You might get a warning about Writing partitioning to disk before the changes are actually written to disk If you do get this warning, it is okay to confirm writing the changes to disk Also, if you get a Low memory warning message, click Yes to immediately turn on the swap space

This simple relation is known as the l~zw mass action Since liquids often form nonideal of solutions, Eq (1333) can be expected in many instances to yield poor results For species known to be present in high concentration, the equation fi f , = xi is usually / nearly correct The reason, as discussed in Sec 121,is that the LewisIRandall rule [Eq(1 180)] always becomes valid for a species as its concentration approaches xi = 1 For species at low concentration in aqueous solution, a different procedure has been widely adopted, because in this case the equality of fi f , and xi is usually far from correct The method is based on use I of a fictitious or hypothetical standard state for the solute, taken as the state that would exist if the solute obeyed Henry's law up to a molality nz of unity7 In this application, Henry's law is expressed as

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and it is always valid for a species whose concentration approaches zero This hypothetical state is illustrated in Fig 133 The dashed line drawn tangent to the curve at the origin represents Henry's law, and is valid in the case shown to a molality much less than unity However, one can calculate the properties the solute would have if it obeyed Henry's law to a concentration of 1 molal, and this hypothetical state often serves as a convenient standard state for solutes The standard-state fugacity is

2:

Hence, for any species at a concentration low enough for Henry's law to hold,

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