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The trade-off between what to hand over to the device and what to keep in the control of the user has cognitive implications (see 3), and is linked to social aspects of collaboration (see 4) An example relating to our shared calendar system was discussed in Box 42 of 4: should the system allow users to book meetings in others' calendars without asking their consent first In addition, if the cognitive load is too high for the user, then the device may be too stressful to use On the other hand, if the device takes on too much and is too inflexible, then it may not be used at all Another aspect concerns the functions the hardware will perform, ie.

Write and implement an effective administrator authentication plan. Identify weaknesses and quickly address them. Consider the use of tokens and biometrics for strengthened administrator authentication. ______________________________________________________________________ ______________________________________________________________________ ______________________________________________________________________

, what functions will be hard-wired into the device and what will be left under software control, and thereby possibly indirectly in the control of the human dser This leads to considerations of the architecture of the device, although you Would riot expect necessarily to have a clear architectural design at this stage of development..

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You still need to type the password, but after that, everything that normally happens at login for the root user happens after the su command is completed. Your current directory will be root s home directory (probably /root), and things such as the root user s PATH variable will be used. If you become the root user by just typing su, rather than su -, you won t change directories or the environment of the current login session. You can also use the su command to become a user other than root. This is useful for troubleshooting a problem that is being experienced by a particular user, but not by others on the computer (such as an inability to print or send e-mail). For example, to have the permissions of a user named jsmith, you d type the following:

When upgrading to a newer distribution, use dist-upgrade instead of upgrade. This changes the rules that APT uses when deciding which actions to take, making it expect major changes in dependencies and handle them appropriately.

A further special case of (8A.8) corresponds to S1p = S2p = Sp , N1p = N2p = Np , 1p = 2p , in which case we obtain a b 0

70

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Supply Chain Planning and Optimization Manufacturing Planning Transportation Planning Distribution Planning Demand Planning

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Measurement of charged particle beam intensities is largely done using physical methods, although some older radiochemical methods are used occasionally. The most common techniques to measure the intensity of a charged particle beam is through the use of a Faraday cup. The beam is stopped in an electrically isolated section of beam pipe referred to as a Faraday cup (Fig. 19.3). The collected charge is measured with an electrometer that functions as a current integrator. The beam intensity is just the current divided by the charge on each ion. Care must be taken regarding the loss of secondary electrons. (The beam will liberate secondary electrons in the material in which it stops.) If these electrons escape, their positive ion partners will add to the positive charges of the stopped ions, thus causing an overestimate of the beam current. The Faraday cup is thus made as a long cylinder to inhibit electron escape geometrically, and a magnetic eld is applied to the cup along with a suppressing voltage to further prevent electron loss. When the energy of the charged particle beam is too large to easily stop the beam in a Faraday cup, the beam intensity is frequently monitored by a secondary ionization chamber. These ion chambers have thin entrance and exit windows and measure the differential energy loss when the beam traverses them. They must be calibrated to give absolute beam intensities. If the charged particle beam intensity is very low (,106 particles/s), then individual particles can be counted in a plastic scintillator detector mounted on a photomultiplier tube. When performing irradiations with neutrons or high-energy protons, it is common to measure the beam intensity using a monitor reaction. A thin foil of a