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be utilized even if a series specified crystal is employed, but in this case it will vary the frequency of the oscillator from about 5 ppm to around 50 ppm above the marked series resonant frequency However, since the impedance increases as the crystal gets closer to its true parallel resonant frequency (which is always above its series resonance frequency) whether in series or parallel mode the feedback gain will begin to decrease as the frequency of the oscillator is tweaked upward Thus there will be a point reached where the feedback gain will decrease so much so that oscillations are no longer possible This is why it is prudent to maintain the frequency of the oscillator as close to the actual series resonant frequency of the crystal as possible, without excessive tweaking; whether or not it is a series or parallel crystal If the oscillator s designer does not supply the crystal manufacturer with what is called the load capacitance (CL) for a parallel resonant crystal, the manufacturer will assume it to be around 30 pF The load capacitance is simply the load that the crystal will see when placed in the oscillator circuit, and slightly affects the accuracy of the parallel crystal s marked frequency It can easily and more accurately be computed in a Pierce oscillator by:

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originating the packet, the packet is dropped; otherwise duplicate delivery of packets for that packet would result Keep track of the age of each entry in the station cache An entry is deleted after a period of time if no packets are received with that address as the source address This ensures that if a workstation is moved from one LAN to another, the "old" entry in the station cache associating that address with a now incorrect interface is deleted Using this logic, and assuming that workstations A, B, C, and D in Fig 5-12 all communicate with one another, the bridge will produce a station cache that associates workstations A and B with interface 1, then C and D with interface 2 This potentially relieves congestion in a network All traffic that originates at and is destined for LAN 1 will not be seen on LAN 2 and vice versa This form of bridging works well for any LAN topology that does not include multiple paths between two LANs We know that multiple paths between network segments is desirable to maintain connectivity if one path fails for one reason or another Let's look at what a simple transparent bridge would do if implemented in a LAN environment such as that shown in Fig 5-13

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The last example of filled text we want to show you is a little different This time, we ll use the Type Mask tool As with the regular Type tool, there s a horizontal and vertical version of the Type Mask tool For now, select the Horizontal Type Mask tool from the Toolbox it shares a spot with the regular Type tool Click the Type tool button and hold down the mouse button, then click the Horizontal Type Mask tool (it s the T with a dashed outline) to select it

Specifying the crystal in its series resonant mode will not require the above formula, and even a parallel crystal will be fine for most applications without this CL specification unless extreme frequency accuracy is required Obtain the crystal s motional capacitance (CM), motional inductance (LM), series resistance (RS), and parallel plate capacitance (CP) from the manufacturer for the crystal s frequency of operation, type of holder, and cut (typically AT) This will allow us to utilize the equivalent circuit of Fig 49 to model the crystal in the linear circuit open-loop simulation program as a simple LCR circuit The Pierce oscillator is meant to work only on the crystal s fundamentalmode series resonance, but can function with overtone crystals if C1 is replaced with a parallel resonant tank that is tuned midway between the desired overtone and the overtone just below it (Fig 427) In this case, the crystal manufacturer must be told if the crystal is being run out of its fundamental mode Choose a transistor with a much higher ft than required for the oscillation frequency (5ft), and with a very high gain as well The high ft is required to assure as close to a 180 degree phase shift from the transistor s input to its output as possible, while the high gain is necessary because of this oscillator s rather high loop losses R, C1, XTAL, and C2 of Fig 426 form a 180 phase-shift network, while R is also the feedback control element employed to place less stress on the crystal As mentioned, the Pierce oscillates just slightly above the series resonant frequency of a series crystal, so C3 is included to tune the oscillator toward the series XTAL frequency (but the oscillator can never quite reach it) By increasing C3 s capacitance, the frequency is lowered closer to the desired fr of the oscillator, while decreasing C3 increases the fr further away from the series resonance of the crystal RVCC and CBYPASS act in the decoupling role, while Rf, RVCC, and RC are the oscillator s bias resistors CCOUP is used to couple power out of the oscillator into a 50-ohm load without loading the oscillator down below a safe gain margin If CCOUP is not of a high enough reactance value, the oscillator s feedback may become too low to maintain, or even begin, oscillations (see Oscillator output coupling in Sec 425) Since the open-loop output and input impedance of a Pierce crystal oscillator are higher than 50 ohms, set the linear software simulator s termination impedances to about 300 ohms for more accurate results Follow these design equations to complete: 1 CBYPASS 2 C1 C2 (CFACTOR 3 C3 CC 1 ohm(XC) 2 MHz; 08 4 MHz; 09 6 MHz; 1 8 MHz).

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