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However, in order to function as desired, coupling and decoupling capacitors must not be near their parallel (high-impedance) resonant mode, while decoupling inductors must not be close to any series (low-impedance) resonant modes nor should the inductors be above their maximum frequency of operation, in which case they would start to become capacitive Inductors are far from perfect components, and possess parasitic capacitances So when an amplifier must be able to function properly across a wide band of frequencies, two RFCs (Fig 397) will normally be required: a lowinductance coil that works at very high frequencies without encountering any series resonances, and a high-inductance coil used to block the lower frequencies This is necessary because the low-frequency, high-impedance inductor will begin to pass the higher frequencies of the passband through the natural turnto-turn capacitance of any coil.

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0.3289 0.6568 0.9829 1.3063 1.6262

You can use the for loop, the if statement, and code blocks to create an improved version of the Fahrenheit-to-Celsius converter that you developed in the first Try This example. This new version will print a table of conversions, beginning with 0 degrees Fahrenheit and ending with 99. After every 10 degrees, a blank line will be output. This is accomplished through the use of a variable called counter that counts the number of lines that have been output. Pay special attention to its use.

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An additional bypass capacitor to ground may be placed between the larger coil and ground to further decouple any RF into the amplifier s supply This type of decoupling will permit the amplifier s wide passband to sustain a nearly flat gain response over its entire frequency range Coupling There are various coupling techniques that can be used between stages, depending on frequency, cost, performance, and impedance-matching needs Capacitor coupling (Fig 3111), also referred to as RC coupling, is found in AC and RF amplifiers only, and is capable of amplifying over a very wide bandwidth (the amplifier s required impedance matching circuit will limit this bandwidth, however) As shown in the figure, the series coupling capacitor CC blocks the DC bias to the next stage, but allows the RF signal to pass unattenuated.

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Figure 6.10 shows the graphs of loga x for several different values of a > 1. Figure 6.11 shows the graphs of a x for several different values of a > 1. You Try It: Sketch the graph of y = 4x and y = log4 x on the same set of axes.

The coupling capacitor and R6 form a voltage divider, allowing most of the RF signal to be dropped across the high resistance of R6 located at the input to the next stage The voltage divider functions as described because the capacitor has a much lower impedance to the RF than does the resistor This signal across R6 will then add to or subtract from the second stage s emitter-base junction, forcing its collector current to vary through R7, producing an amplified output voltage..

2. The first time you access a particular list of values, the possible list of values screen may be empty. Click Refresh Values to launch the list of values query. 3. For each of the prompts, select the prompt from the top of the dialog, and then select the desired values. For example, position your mouse on Select Product Line(s), labeled 1 in the preceding illustration. 4. In the possible values list, select an additional filter criterion, such as Sweaters, labeled 2.

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