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Each time you create a shape, Photoshop places it on its own layer. However, you can combine shapes if required, but not in the conventional way of combining pixel-based layers at least, not without rasterizing the two layers first. To do so, take the following steps: 1. In the Layers palette, click the vector mask of the source shape layer that you want to combine. 2. Choose Edit Copy, or Ctrl+C (Windows), +C (Mac OS). If you want to delete the source shape layer, select the path with the Path Selection tool and then cut the path by pressing Ctrl+X (Windows), +X (Mac OS). 3. Select the vector mask of the target shape layer. 4. Choose Edit Paste, or Ctrl+V (Windows), +V (Mac OS). Photoshop combines the two shapes and applies any effects that might be present in the target layer.

Generating a plain KML file is fine when either the information or the icons and other data are available freely on the Internet. However, there are times when you want to create a standalone file that incorporates the KML with the icons, images, and any other files that make your Google Earth file. The format is quite straightforward. It is simply a Zip file that contains the KML and images. For clarity, you should use the following format:

3.13 Choose where to store the footage, which Event to make it part of, and whether to split days into new Events.

(13.11)

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4. Under Batch Options, select an operation to apply to your batch and click the Add button to add it to the Include in Batch list. The newly added operation is selected by default, and options for that operation (if any) appear in the lower portion of the Batch Process dialog box. Of course, you can click the Remove button to remove an operation from the Include in Batch list, as well. 5. Specify options for newly added operation. For example, if you add a Scale operation (as shown in Figure 18-16), you can choose No Scaling, Scale to Size, Scale to Fit Area, or Scale to Percentage, and specify the appropriate height, width, or percentage, as required.

Figure 20-5: With the Actions Panel in Normal Mode, you can clearly see the options and settings of the loadMovie action.

To start editing one of your styles immediately, double-click the style in the list window of the Edit Style Sheet dialog box. This sequence takes you to the CSS Style Definition dialog box, in which you redefine your selected style.

plasmas with good uniformity using microwave excitation due to the strong magnetic fields that confine the plasma and influence the profile. This leads to other magnetic configurations to produce the plasma using microwave ECR techniques. In a volume-ionization ECR source, like that shown in Fig. 4-36, a significant fraction of the discharge chamber must be filled with a strong magnetic field to satisfy the resonance condition. If this field is produced by a solenoid, the electrical power required to achieve a sufficient field strength can represent a significant energy cost to the thruster. Likewise, if the field is produced by permanent magnets, the weight of the magnetic material required to produce this field can represent a significant weight penalty for the thruster. This problem can be mitigated by using magnetic multipole boundaries that produce strong magnetic fields at the discharge chamber wall using ring or line-cusp magnet configurations. Figure 4-38 shows the field lines between two magnet rings and the regions of strong magnetic field close to the magnet where the resonant condition is satisfied. Injection of the microwave radiation between the cusps, either by cutoff waveguides inserted between the rows [52], by slotted waveguides run along the rows [53], or by antenna structures placed between the rows, will couple the microwaves to the high magnetic field interaction region. While this geometry eliminates the solenoidal magnet coils and minimizes the size of the permanent magnets required to produce the resonant field strength, there are several issues remaining. First, the magnetic field strength in the cusp region decreases as one over the distance from the surface squared. This means that very strong magnets are required to produce the resonant field at any significant distance from the wall. Second, electrons that gain energy from the

9

5.1 INTRODUCTION In Section 4.4, asymptotic ray-based techniques where described. They turned out to be very efficient tools when combined with the MoM or FE-BI methods for the analysis of conformal antennas. However, there is a fundamental question to be answered before these techniques can be applied: How does one find the proper ray(s) that connect(s) arbitrarily located points on a smooth surface For a correct solution, the rays must obey certain conditions in order to be valid geodesics on the surface.

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