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To understand how critical the transit time effect is, realize that at 1 GHz, one RF cycle is 1 ns (1029 s) In one cycle at 1 GHz, the electrons will travel 105 m/s 1029 s 100 microns (mm) For reasonable performance the electrons must move through the transistor in less than one-tenth of a cycle, which means the spacing between doping regions in the transistor must be less than 10 mm At 10 GHz, the spacings must be less than 1 mm RF power ampli ers use two techniques to achieve the required transit times: reduced spacings between transistor elements and use of semiconductor materials like gallium arsenide (GaAs) and silicon germanium (SiGe), in which electrons move faster than they do in silicon Figure 117 shows a measurement of a typical RF power ampli er made with a VNA.



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Dragging the Rollback bar with the cursor. Right mouse button (RMB) clicking and selecting one of the Rollback options. Editing a feature other than the last one in the design tree. (SolidWorks rolls back the model automatically.) Choose Tools Options FeatureManager Arrow key navigation to control the Rollback bar with the arrow keys. Saving the model while editing a feature or sketch, and then exiting the model. When the part is opened again, it is rolled back to the location of the sketch that was being edited. Pressing Esc during a long model rebuild. This method is supposed to roll you back to the last feature that was rebuilt when you pressed Esc; however, in practice, I have rarely seen it do this, and it usually rebuilds the entire model anyway.

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For this measurement, the VNA is adjusted to measure and display gain and output power as a function of RF input power at a single frequency of 245 GHz The VNA is calibrated with a power meter, so the output power measurement has only +02 dBm uncertainty The gain measurement is calibrated with the VNA standards, and so it has an uncertainty of only +005 dB The input power is swept over the power range from 7 to 13 dBm, so each horizontal scale division is 2 dBm The left-hand graph shows the gain in decibels and the right-hand graph shows the output power in decibels relative to 1 mW At the left-hand edge of each graph, the ampli er is operating in the linear range, where the RF output power is exactly proportional to the RF input power.

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At the right-hand edge of each graph, the ampli er is operating approximately at saturation The markers on both graphs are set at the 1 dB compression point, where the gain has dropped from its linear value by 1 dB Figure 117 shows characteristics that are common to all RF ampli ers Every RF ampli er has a nonlinear output power versus input power curve because the ampli er cannot generate more power that its battery supplies Typical ampli er ef ciency is about 50% at saturation, which is its maximum power output point Most RF transistors draw the same power from their battery, regardless of whether they are operated at full power or at an input level that provides very little output power At small output power levels, the RF output power is proportional to the RF input power This is called the linear range.

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Operation near saturation causes distortion Operation in the linear range causes low ef ciency The usual compromise is to use a 2 higher.

1. Click DVD in the Tasks pane. Windows prompts you that it will open Windows DVD Maker. 2. Insert a blank writeable or rewritable DVD into your computer s optical drive. Windows DVD maker starts, as shown in Figure 20.34. Note that you don t need to add anything manually; in fact, you shouldn t if you wish only to publish your current video project to this DVD.

The default value for the scale variable is zero. Before the scale value is set, the bash calculator provides the answer to zero decimal places. After setting the scale variable value to four, the bash calculator displays the answer to four decimal places. The -q commandline parameter suppresses the lengthy welcome banner from the bash calculator. Besides normal numbers, the bash calculator also understands variables:

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