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To use GnuPG encryption on Evolution, you ll need to do a few things. First, you ll need to generate a key pair. Follow these steps: 1. Open a terminal window. 2. At the command prompt, type gpg --gen-key. 3. You are presented with a choice of key types. Unless you have a reason not to, select the first type (DSA and Elgamel). 4. You are asked to specify the size of your key. Again, unless you have a reason not to, you can select the default (2048 bits) just by hitting the Enter key. 5. You are asked to select how long your key will be valid. This is up to you. Select 0 if you don t want your key to expire. You are asked to confirm this choice. 6. You are now asked to answer a few questions in order to create a User ID for your key. 7. Next, you need to create a passphrase for your key. This is a very important step. Your passphrase can be anything, and it can include spaces. Select a phrase that you will remember. 8. The computer now generates your key. This may take awhile. You can do other things on your computer while this is going on. This is helpful because the computer uses random bits of information from things like keystrokes and mouse movements to help generate the key. When it s done, it prints some information about your key and returns you to the system prompt. Second, upload your public key to a key server. This way, people who need to download your key can do so and use it to decrypt your messages. To do this, follow these steps:

FIGURE 7.1 Geometry of a proposed broadband microstrip antenna with directly coupled and parasitic patches. (From Ref. 3, C 1999 John Wiley & Sons, Inc.)

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CLose: Closes the polyline by drawing an arc from the endpoint of the last arc to the start point of the polyline. Direction: Specifies the direction of the arc from the start point. Halfwidth: Defines half of the width of the polyline the distance from the center of the polyline to its edge. The option asks you for the starting halfwidth and the ending halfwidth. Line: Returns you to the main polyline prompt so that you can draw line segments. Radius: Specifies the arc s radius. Second pt: Specifies the second point of the arc. Undo: Undoes the last arc. Width: Defines the width of the polyline. The option asks you for the starting width and the ending width. Specify endpoint of arc: Specifies the endpoint of the arc. This is the default. This option creates an arc tangent to the previous arc (continuing in the same direction). PLINE continues to display the arc submenu until you use the Line suboption or end the command by pressing Enter.

$<input type= text name= new_price > <xsl:attribute name= value ><xsl:value-of select= PRODUCT_PRICE /></xsl:attribute> <xsl:attribute name= onChange >validatePrice(this,"<xsl:value-of select= PRODUCT_NAME />")</xsl:attribute> </input>

$test_var = 8.23;

The granular data found in the data warehouse supports more than data marts. It also supports the processes of exploration and data mining. Exploration and data mining take masses of detailed, historical data and examine it for previously unknown patterns of business activity. The data warehouse contains a very useful source of data for the explorer and data miner. The data found in the data warehouse is cleansed, integrated, and organized. Plus, the data is historical. This foundation is precisely what the data miner and the explorer need in order to start the exploration and data mining activity. It is noteworthy that while the data warehouse provides an excellent source of data for the miner and the explorer, the data warehouse is often not the only source. External data and other data can be freely mixed with data warehouse data in the course of doing exploration and mining. Refer to the book Exploration Warehousing: Turning Business Information into Business Opportunity (Hoboken, N.J.: Wiley, 2000) for more information on this topic.

So far we have ignored the interaction of the beam with its surroundings. Typically, a beam travels within a beam pipe made of some conducting material. So, in general, the electric field distribution will be influenced by the conducting boundary. Also, within a magnet, the magnetic field distribution will be shaped in part by the presence of magnetic materials. We take up the problem of static effects due to electric fields. The method of images is well suited to problems of this type. Take, for example, the electric field distribution of a line charge near a perfectly conducting plane. The field lines are perpendicular to the plane everywhere, and the resulting distribution is the same as if the conducting plane were replaced by a second line distribution of opposite charge equidistant from the boundary, as shown in Figure 6.1. Therefore, the force on the line charge due to the conducting plane is the same as the force calculated due to the image.

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