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The Security Center (see Figure 14.16), which is also available in the Control Panel, is the central location for working with security settings, including malware protection and the Windows Firewall. For complete information on the Security Center, please refer to 7.
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'Use the data adapter to create a fill a new DataTable called _ Customers oDataAdapter.Fill(oDataSet, "Customers")
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mysql> select * from teams order by city; +----+-----------+-----------+-----------------+------+--------+ | id | team_name | city | logo | wins | losses | +----+-----------+-----------+-----------------+------+--------+ | 5 | Orioles | Baltimore | orioles.jpg | 64 | 98 | | 3 | Red Sox | Boston | redsox.jpg | 95 | 67 | | 2 | Yankees | New York | yankees.jpg | 103 | 59 | | 4 | Rays | Tampa Bay | rays.jpg | 84 | 78 | | 1 | Blue Jays | Toronto | bluejays.jpg | 75 | 87 | +----+-----------+-----------+-----------------+------+--------+ 5 rows in set (0.00 sec) mysql> select * from teams order by losses desc; +----+-----------+-----------+-----------------+------+--------+ | id | team_name | city | logo | wins | losses | +----+-----------+-----------+-----------------+------+--------+ | 5 | Orioles | Baltimore | orioles.jpg | 64 | 98 | | 1 | Blue Jays | Toronto | bluejays.jpg | 75 | 87 | | 4 | Rays | Tampa Bay | rays.jpg | 84 | 78 | | 3 | Red Sox | Boston | redsox.jpg | 95 | 67 | | 2 | Yankees | New York | yankees.jpg | 103 | 59 | +----+-----------+-----------+-----------------+------+--------+ 5 rows in set (0.00 sec)
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stoichiometry and an agreement within 3 10 % was found between calculated and nominal concentrations. The measurements were performed using an X-ray microbeam with 177 m diameter. Generalized iterative procedures based on FP for quantitative XRF analysis were published (Szal ki et al., 1999). In general, the estimation of o the matrix attenuation for the iterative calculation is based on the average atomic number of the sample matrix. The procedure offers a wide ranging extension for quantitative standardless XRF analysis of complex samples, especially for environmental and biological materials. In contrast to these methods, our approach uses the MC technique. The quanti cation method presented below is based on MC simulations for dealing with the energy and spatial distribution of the X-ray microbeam, the interaction between the exciting photons and the sample elements taking into account the geometry effects caused by the size and topology of the particles. The applicability of the method is demonstrated on y ash particles because they are common atmospheric particles having relatively elevated concentrations of some toxic elements (Vincze et al., 2002b).
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connected to its own ampli er. The position of the strip hit provides a coordinate, the signal height the energy of the X-rays. For a fraction of events the signal will be split between neighbouring strips due to the size of the charge cloud caused by electrostatic repulsion and diffusion on their way towards the strips. For low energy X-rays the preferred radiation entrance side is the unstructured n+ backside. This is due to the bad charge collection properties in the gap regions between the strips where electrons experience no drift towards the backside but have to cross a potential barrier with the help of diffusion. Typical strip pitches p are in the range of 20 to a few hundred micrometres. This may require a large number of readout channels. This number can be decreased by using capacitive charge division readout as shown in Figure 4.1.4. Here only every fourth strip is connected to an electronics channel and the charge collected at non-connected strips couples capacitively through the naturally present inter-strip capacitances to those strips connected to the electronics. The ratio of signals in neighbouring readout strips is used for position interpolation.
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