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Here, qi is a charge in distribution A, qj is a charge in distribution B, and rij is the separation between charges qi and qj Quantity 0 is the electric permittivity of vacuum, a physical constant3 equal to 8854 19 x lo-'' C V-' m-' (The unit of electric charge is the coulomb C, and the unit of electric potential difference is the volt V) The sums are taken over all charges in the distributions Equation (162) is exact, but awkward to use as it stands Application is facilitated when the charge separation rij is replaced by the center-of-mass separation r of the two distributions Statistical averaging of contributions from all orientations of charge distribution yields the following approximate expression for U(e1) for two neutral rigid charge distribution^:^



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Description This permission allows the group to perform management tasks on your Oracle Application Servers or WebSphere servers This includes the ability to modify the configuration and bounce the application server This setting allows users in the group to upload software to the repository in Server Manager This is the Managed Software quick link in Server Manager This setting allows the members of the group to use the monitoring features in Server Manager They can start, stop, and configure monitors

One of the key points in determining how to protect information is: A The day of the week B The name of the document C The form of the information itself D None of the above





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J K-l ; p~ and p~ are the permanent Quantity k is Boltzmann's constant, equal to 1381 x dipole moments for charge distributions A and B associated with the molecules This contribution to the pair-potential function vanishes only when one of the permanent dipole moments is zero The averaging procedure which leads to Eq (163) produces several remarkable results:

TABLE 12-8

Even though the distributions are electrically neutral, there is a net attraction between them The dependence of U(e1) on charge-distributionorientation becomes on averaging an rP6 dependence As given by Eq (163) U(e1) varies with T-' Hence the magnitude of the permanentdipole interaction decreases with increasing temperature Equation (163) is the simplest example of a direct electrostatic potential for two neutral molecules; here, the dipole moment emerges as an important physical property Dipole moments are measures of the net separation of charge within a molecule For a spherically symmetric neutral charge distribution (eg, an atom of argon), p is zero For a molecule in which charge Iq 1 is separated from charge - Iq 1 by distance 1, the dipole moment is p = Iq 1 1 Hence p

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Paper documents are often considered easier to secure, as they: A Are not dependent on power B Are less valuable C Do not deteriorate with age D All of the above

Description This permission allows members of the group assigned the permission to actually change the configuration of Server Manager itself This means they can update the agents, set up managed homes, remove managed homes, and other administrative options in Server Manager This allows the users of the group assigned the permission to administer the Server Manager console users and permissions

3~nrelated the well depth E of Fig 161 to 4 ~ h iresult is only valid for modest dipole moments For a discussion, see T M Reed and K E Gubbins, Applied s Statistical Mechanics, sec 5-7, McGraw-Hill, New York, 1973

has dimensions of charge x length; its SI unit is the coulomb(C)~meter(m)However, values are usually reported in debyes ( D ) ;1 D = 33357 x low3' C m A molecule with a nonzero dipole moment is called polar Water ( p = 19 D), acetone ( p = 29 D), and acetonitrile ( p = 40 D) are strongly polar molecules Carbon monoxide ( p = 01 D), propylene ( p = 04 D), and toluene ( p = 04 D) are slightly polar Carbon dioxide, neon, nitrogen, and n-octane are nonpolar ( p = 0) The dipole moments just discussed are permanent dipole moments, intrinsic properties of a molecule A net separation of charge may also be induced in any molecule by application of an external electric field The induced dipole moment p(ind) so created is approximately proportional to the strength of the applied field Thus, for molecule A, pA(ind)= a A E ,where E is the applied field strength and a~ is the polarizability of A If the source of the electric field is a permanent dipole in a neighboring molecule B, then the contribution to U from the permanent dipolelinduced dipole interaction is:

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PDF Focus .Net - Convert PDF to Images in C# and VB . Net
PDF to Image , Jpeg, multipage TIFF, PNG in C# and VB . Net . PDF to Images . Now let's get to know another benefit of the library. PDF Focus .Net offers great ...

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