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LMH6560 Datasheet(PDF) 20 Page - National Semiconductor (TI) |
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LMH6560 Datasheet(HTML) 20 Page - National Semiconductor (TI) |
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20 / 23 page ![]() Application Notes (Continued) Discontinuities in a Ground Plane A ground plane with traces routed over this plane results in the build up of an electric field between the trace and the ground plane as seen in Figure 13. This field is build up over the entire routing of the trace. For the highest performance the ground plane should not be interrupted because to do so will cause the field lines to follow a roundabout path. In Figure 17 it was necessary to interrupt the ground plane with the blue crossing trace. This interruption causes the return current to follow a longer route than the signal path follows to overcome the discontinuity. If needed it is possible to bypass the interruption with traces that are parallel to the signal trace in order to reduce the negative effects of the discontinuity in the ground plane. In doing so, the current in the ground plane closely follows the signal trace on the return path as can be seen in Figure 18. Care must be taken not to place too many traces in the ground plane or the ground plane effectively vanishes such that even bypasses are unsuccessful in reducing negative effects. If the overall density becomes too high it is better to make a design which contains additional metal layers such that the ground planes actually function as ground planes. The costs for such a pcb are increased but the payoff is in overall effectiveness and ease of design. Ground Planes at Top and Bottom Layer of a PCB In addition to the bottom layer ground plane another useful practice is to leave as much copper as possible at the top layer. This is done to reduce the amount of copper to be removed from the top layer in the chemical process. This causes less pollution of the chemical baths allowing the manufacturer to make more pcb’s with a certain amount of chemicals. Connecting this upper copper to ground provides additional shielding and signal performance is enhanced. For lower frequencies this is specifically true. However, at higher frequencies other effects become more and more important such that unwanted coupling may result in a re- duction in the bandwidth of a circuit. In the design of a test circuit for the LMH6559 this effect was clearly noticeable and the useful bandwidth was reduced from 1500MHz to around 850MHz. As can be seen in Figure 19 the presence of a copper field close to the transmission line to and from the buffer causes unwanted coupling effects which can be seen in the dip at about 850MHz. This dip has a depth of about 5dB for the case when all of the unused space is filled with copper. In case of only one area being filled with copper this dip is about 9dB. PCB BOARD LAYOUT AND COMPONENT SELECTION Sound practice in the area of high frequency design requires that both active and passive components be used for the purposes for which they were designed. It is possible to amplify signals at frequencies of several hundreds of MHz using standard through hole resistors. Surface mount de- vices, however, are better suited for this purpose. Surface mount resistors and capacitors are smaller and therefore parasitics are of lower value and therefore have less influ- ence on the properties of the amplifier. Another important issue is the pcb itself, which is no longer a simple carrier for all the parts and a medium to interconnect them. The pcb board becomes a real component itself and consequently contributes its own high frequency properties to the overall performance of the circuit. Sound practice dictates that a 20064260 FIGURE 17. 20064261 FIGURE 18. 20064262 FIGURE 19. www.national.com 20 |
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