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It is generally agreed that when the diameter of plated holes is equal to or less than 03 mm and the core thickness is equal to 06 mm or less, these holes can be filled effectively by the lamination process (although the resin thickness of 80 m is preferred in the case of RCC) See Fig 2215 When the diameter/thickness conditions are not met, it is necessary to fill the holes using a separate process A screening process does this from one side of the panel with polyester screen with an oversized hole pattern After hole filling and curing the resin completely, the fabricator removes excess resin using a belt sander (#600 to #800) or a ceramic brush Figure 2216 illustrates the processThis is a tricky but necessary operation for microvia board makers, particularly for photovia processing.

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How to Generate Code 128 Barcode in RDLC Reports
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Dynamic hydrostatic bearings, electrostatic pneumatic bearings and guideways, ball or roller pre-load bearings or guideways

Hole filling is costly but yields a few advantages over simultaneous hole filling by lamination of RCC or prepreg The edge of the plated holes is well protected; therefore, forming.

A useful empirical equation for calculating the manufacturing cost is: Cost C = (material + process costs) Yield Y (2.3)

To establish the effect of the interconnection density Id on the final yield of substrates, the total processing yield can be split into two components: one that depends on the conductor density, i.e., YId, and the second, which is a function of the combined yields of the rest of the manufacturing processes: Ytotal = YId*Yproc (2.4)

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In a well controlled manufacturing operation, the process-dependent yields (such as plating) remain fairly constant for a given technology, permitting the yield function to be based solely on the changes in the conductor widths.

Differential transformers, inductosyn scales, photo electric moir scales, precision air micrometers, strain gauges, vidicons, CCDs Precision differential transformers, laser interferometers, electro-magnetic comparators, radiation counters

As seen from Fig. 2.11, the defects that affect this density-dependent yield function YId are conductor opens and shorts between them. It would be reasonable to assume that such defects have a Poisson distribution over the total length TL of conductors of a substrate, with an average defect frequency of v. The yield is the probability of zero defects (n = 0) in the total conductor length TL. Thus, Y = (at n = 0) = e( n*TL) (Poisson distribution) (2.5)

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As seen from Figs. 2.10 and 2.11, the defect frequency n depends also on the widths of lines and spaces, i.e., on the conductor pitch Cp. With a decrease of Cp, n will increase, but for very large Cp, n should be 0, since YId will be 100 percent. For instance, in the case of a design using invisible pads, where Cp = 2w, the interconnection density Id can be expressed as Id = TL/A, and Id is proportional to Cp, i.e., Id * Cp = 1, and TL = A/Cp. Therefore, n in this equation can be empirically expressed as: n = ln Y0 Cp0 * TL0 Cp

(2.6)

where b is an exponent dependent on the technology or process used to form the conductors. This exponent b varies considerably from facility to facility and among various pattern formation methods, and must be empirically determined for each case. 2.7.4 Increase in Number of Conductor Layers This is the simplest and most straightforward solution: when there is insufficient room on existing layers to place all the necessary interconnecting paths, add a layer. This approach has been widely practiced in the past, but when cost effectiveness of the substrates is of paramount importance, a very careful design analysis must be made to minimize layer counts in MLBs, because there is a significant cost increase with every additional layer in the board. As seen from Table 2.6, calculated for 6- 8-in MLBs produced in large quantity with yields and conductor density kept constant, there is almost a linear relationship between board costs and layer count. Table 2.6 also shows that any increase in the number of signal layers in boards operating at frequencies requiring transmission line characteristics will double the total number of layers, due to the need to interleave ground or DC power planes between signal planes. A typical example of the effect of layer count on the finished MLB yield can be seen from Fig. 2.12, prepared some years ago by BPA. We can see that there is a definite decrease in the manufacturing yields with an increased number of layers in any of the linewidth categories. This is rather a typical situation in board manufacturing because increased complexity and thickness of MLB with a higher number of layers usually leads to a larger number of problems on the production floor.

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