Uneeda Audio Universal Pad Board



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Transcription:

Uneeda Audio Universal Pad Board Sometimes you need a fixed attenuator when you are designing a sound system. Sometimes this is to force a microphone input to accept a line level signal, sometimes it is to get the clipping points of various devices in the system to line up correctly, and sometimes is just because. The Uneeda Audio Universal Pad Board is designed for all of these things and more. It s small, easy to build, and easy to mount (just one hole needed). It can be configured with all of the commonly used pad topologies: H, T, L, U, O, Pi, Bridged Tee. It can be configured for balanced or unbalanced circuits. You can solder the i/o connections or you can use screw terminals. It s all in how you stuff the board. It s beyond the scope of this manual to discuss what a pad does. If you re here already, then you ve got this much figured out. If not, then refer to the following web page for that introduction: http://www.uneeda-audio.com/pads/ You ll find design information at the end of this document. Selecting a Circuit With so many circuits to choose from, what s a person to do? The circuit board could have been designed for only one or two circuits, but then there was always the possibility that someone would as why the board didn t accommodate their pet circuit. It just made more sense to mae the board applicable to all of the major circuits. The only circuit that the board doesn t handle directly is the Lattice pad, which is a variant of an O pad. With some creative forcing, you could manage even that configuration although it might tae a bit of creativity and there are no pads dedicated to maing this configuration wor. That said, the H, U, and Bridged Tee configurations are probably most often used. All perform their tas as designed. We won t argue sonics here. Table shows the more common configurations and points out some of the important differences. ight off, see that the Bridged-Tee configuration only requires two different resistors and two that are always equal to the line impedance. Table shows which resistors are stuffed for each pad configuration. Figures 3 through 0 are stuffing diagrams for each pad configuration. Calculating Values You can use the formulas and values from the Pads section of the Uneeda Audio website. For pads used in an all-matched (i.e. 600 input and output) system, refer to Table 4, at the end of this document. A spreadsheet program is probably the easiest way to do the math involved (which is really simpler than it loos), or you can use a calculator. With the -factor table, a four-banger calculator will do the job. Component Selection We won t argue sonics here either. That s a personal religious preference. The board was laid out with ¼-watt resistors in mind. These could be carbon film 5% tolerance units, carbon composition units, or precision % metal film units. As calculated, the resistor values are guaranteed to come out in oddball values. Generally speaing, unless you own a resistor factory, you can just convert the values to the nearest standard value and you ll be close enough. This is certainly not a case of sound vs no sound. There is a standard value conversion program available from the Uneeda Audio website. In the Olde Days, many pads were made using carbon composition resistors and a small hand grinder (i.e. a Dremel tool). You d start with a resistor of lower than desired value and you d Copyright 008 by Uneeda Audio. All rights reserved. evision A. Page

grind the body away until the ohmmeter read the magic number. A dab of varnish over the incision sealed things up against moisture. Construction Simple:. Decide on a configuration.. Calculate values. 3. Decide on resistor type. 4. Procure. 5. Figure out where things go. 6. Stuff parts. 7. Solder. 8. Swage the mounting standoff. 9. Installation. Where Things Go See Table. Inputs and Outputs You have two choices: Solder directly to the board. Use a 4-pin Phoenix connector (p/n: 7 5 67 / MPT 0,5/4-,54). Note that the unbalanced configurations use a different set of pins than the balanced configurations. Swaging the Standoff You need a solid surface that can survive a hammer hit, a # phillips screwdriver, and a hammer. Insert the standoff into the hole in the board. Place the board, with the larger end of the standoff on the wor surface. Put the screwdriver into the smaller end of the standoff, and smac the handle of the screwdriver with the hammer, deforming the end of the standoff and attaching it to the board. Figure. Top View Board Dims:.06 x 0.85 Copyright 008 by Uneeda Audio. All rights reserved. evision A. Page

Figure. Schematic Diagram Configuration Number of unique resistor values Number of nonunique resistor values emars T and H 3, sometimes Can wor between asymmetrical impedances. U and L 0 (sort-of) The output resistor value is generally the pad output impedance, except at low values of attenuation. This configuration normally does not attempt to match the source. Bridged Tee (balanced or unbalanced) Only between equal impedances Table. Pad Configurations and esistor Values. Copyright 008 by Uneeda Audio. All rights reserved. evision A. Page 3

Configuration Stuff these parts I/O pins emars L, 5, 3, 4 3 is 0-ohm jumper U, 9, 6,, 4 T, 5, 3, 3, 4 H, 7, 5, 3, 8,, 4 Pi 4,, 6, 3, 4 7, 8 are 0-ohm jumpers O 4, 6,, 9,, 4 Bridged-tee, 5,, 3, 3, 4 3 Balanced Bridged Tee, 9,, 3, 7, 8, 5,, 4 3 ½ 7 8 ½ I/O Connections: Pin is always signal hot. The balanced configurations use pins and for the signal connections. Unbalanced configurations use pin for signal hot, pin 3 for ground. Use pin 4 for the cable shield, when needed. Table. Stuffing Guide. Figure 3. L Pad Figure 4. U Pad Copyright 008 by Uneeda Audio. All rights reserved. evision A. Page 4

Figure 5. T Pad Figure 6. H Pad Figure 7. Pi Pad Copyright 008 by Uneeda Audio. All rights reserved. evision A. Page 5

Figure 8. O Pad Figure 9. Bridged T Pad Figure 0. Balanced Bridged T Pad Copyright 008 by Uneeda Audio. All rights reserved. evision A. Page 6

Pads For Use in Matched Systems The pad values calculated here are for use in matched systems, where the source impedance equals the pad impedance and the pad impedance equals the load impedance. This is ancient practice and is somewhat useable in modern sound system design, provided that the equipment is capable of operating in a 600-ohm environment. The generalized procedure is:. Decide on a configuration. Locate your configuration in Table 4.. Calculate the values needed. The -factors can be found in Table 3. 3. Loo up the nearest % resistor values. Purchase the parts needed. 4. Stuff the board. 5. Solder all connections. 6. Swage the standoff in place. 7. Installation. Example using the -factor tables Design a tee-pad to provide 5dB attenuation with 600-ohm input and output impedances.. Locate the formulas. Since i o, the formulas to use are in the bottom left cell of table 4a.. In the -factor table, locate the row representing 5dB. 3. For, in the 5dB row, find the column that says -/ +. The value is 0.8935. Multiply that by 600. 536.-ohms. 4. For 3, in the equal impedance case, 3. 5. For 5, it s / -, but this time it is just multiplied by. So, 00*0.0564 67.68-ohms. As you can see, the -factor table just saved you from having to do a bunch of really yuy math. olling your own -Factors If you need -factors for values not in Table 3, you can download the Excel spreadsheet that created the table at: http://www.uneeda-audio.com/pads/-factors.xls. Although I can imagine how tables lie this were created before the spreadsheet era, I prefer not to. Standard esistor Values The results from the formulas are exact values. Unless you re really lucy, you can t buy resistors with these values. If you own a resistor factory (or have a relative who does), then you can buy what you want. So can Bill Gates. The rest of us must mae do. esistors are available in standardized values. These values are equally spaced on a logarithmic scale. The number of values available per decade (a spread of 0x) varies according to tolerance: 0%, 5% 4, % 96. The table of preferred values is usually referred to by putting the letter e ahead of the number of values in the series. The % series is nown as the e-96 series. As you can see, tighter tolerance means more values to choose from. The values follow a predictable pattern, although I don t now anyone who has memorized the e-96 value series. Uneeda Audio has a freeware program available that tells you what the standard value is for your exact value. Get that program at: http://www.uneeda-audio.com/pads/stdval.htm. As a bonus, it can also tell you what 5% values you can parallel to approximate your exact value. Copyright 008 by Uneeda Audio. All rights reserved. evision A. Page 7

Pads For Bridging Systems Bridging systems are voltage based, and don t depend on precise source impedances and load impedances. They are the basis for nearly ALL modern audio systems. Discussion of the pros and cons, ins and outs is beyond the scope of this manual. Instead, here are two websites: The Uneeda Audio page about Pads and Pad Design: http://www.uneeda-audio.com/pads/ ichard Hess excellent article about voltage-based transmission systems: http://www.richardhess.com/be/aes-80.htm Since these pads don t depend upon impedance matching, one design suffices, the U pad. efer to Table 5 or to the Uneeda Audio page for the design equations and/or values. Unbalanced Operation The layout of the board allows eeping the low-side (usually grounded) of the signal off of the chassis ground. It s up to you to decide how you ll treat this in your installation. Usually the simple thing to do is to insert the pad into the signal wiring, ignoring the connection labeled SHIELD. When you mount the pad board, the chassis ground connection connects to the pad board s ground plane and that should be sufficient. Copyright 008 by Uneeda Audio. All rights reserved. evision A. Page 8

n(db) r / - (-)/(+) (+)/(-) /( -) -/-r +/ - -/-r /-/-r /- n(db) 0.893.0 0.0.589 0.0575 7.390 4.3334 0.308 8.74 0.087 9.955 8.955 0.7943.589 0.589.5849 0.46 8.74.54 0.4646 4.494 0.057 4.86 3.86 3 0.7079.45 0.45.9953 0.70 5.8480.493 0.7046 3.0095 0.9 3.440.440 3 4 0.630.5849 0.5849.59 0.63 4.494.0483 0.9539.39 0.3690.7097.7097 4 5 0.563.7783 0.7783 3.63 0.80 3.5698 0.84.59.950 0.4377.849.849 5 6 0.50.9953 0.9953 3.98 0.333 3.0095 0.6693.494.6709 0.4988.0048.0048 6 7 0.4467.387.387 5.09 0.385.646 0.5580.790.4985 0.5533.8073 0.8073 7 8 0.398.59.59 6 0.4305.39 0.473.38.3767 0.609.664 0.664 8 9 0.3548.884.884 8 0.476.0999 0.4059.4636.880 0.645.5499 0.5499 9 0 0.36 3.63.63 0 0.595.950 0.354.8460. 0.6838.465 0.465 0 0.5 3.98.98 6 0.5985.6709 0.68 3.799.347 0.7488.3354 0.3354 4 0.995 5.09 4.09 5 0.6673.4985 0.078 4.83.089 0.8005.493 0.493 4 5 0.778 5.634 4.634 3 0.6980.436 0.836 5.4456.0653 0.8.63 0.63 5 6 0.585 6.3096 5.3096 40 0.764.3767 0.66 6.5.055 0.845.883 0.883 6 8 0.59 7.9433 6.9433 63 0.7764.880 0.79 7.874.03 0.874.440 0.440 8 0 0.000 0.0000 9.0000 00 0.88. 0.00 9.9000.00 0.9000. 0. 0 5 0.056 7.788 6.788 36 0.8935.9 0.0564 7.766.0063 0.9438.0596 0.0596 5 30 0.036 3.68 30.68 000 0.9387.0653 0.037 3.59.000 0.9684.037 0.037 30 35 0.078 56.34 55.34 36 0.965.036 0.078 56.63.0006 0.98.08 0.08 35 40 0.000 00.0000 99.0000 0000 0.980.00 0.000 99.9900.000 0.9900.00 0.00 40 45 0.0056 77.879 76.879 363 0.9888.03 0.0056 77.83.000 0.9944.0057 0.0057 45 50 0.003 36.78 35.78 00000 0.9937.0063 0.003 36.46.0000 0.9968.003 0.003 50 55 0.008 56.343 56.343 368 0.9964.0036 0.008 56.3395.0000 0.998.008 0.008 55 60 0.000 000.0000 999.0000 000000 0.9980.000 0.000 999.9990.0000 0.9990.000 0.000 60 65 0.0006 778.794 777.794 3678 0.9989.00 0.0006 778.788.0000 0.9994.0006 0.0006 65 70 0.0003 36.777 36.777 0000000 0.9994.0006 0.0003 36.773.0000 0.9997.0003 0.0003 70 80 0.000 0000.0000 9999.0000 00000000 0.9998.000 0.000 9999.9999.0000 0.9999.000 0.000 80 Table 3. -Factors Copyright 008 by Uneeda Audio. All rights reserved. evision A. Page 9

Copyright 008 by Uneeda Audio. All rights reserved. evision A. Page 0 L Where i o 5 Where i > o o i s 5 S S S S i i Where i<o 5 Minium loss between two impedances ) ( o i i 5 Loss 0log + o i o i U (balanced L) Where i o 6 9 Where i > o ( ) o i s 0.5 6 9 S S S S i i Where i < o 6 9 Minimum loss between two impedances 9 ( o) i i 6 Loss 0log + o i o i T Where i o + 3 5 Where i o + io i + 3 io o 5 io Table 4a. Pad Value Calculations for Impedance Matched Systems

H (Balanced T) BT PI Where i o 3 + 5 Unbalanced Bridged T 3 ( ) 5 Where i o + 4 6 Where i o + a i io then 7 a + b o io then 3 8 b 5 io Balanced Bridged T 3 7 8 9 ( ) 5 Where i o and s 4 i + s i o then 4 i s + O (Balanced PI) Where i o : Design for unbalanced case (PI). Where i o: Design for the unbalanced case (PI) 9 Where is the value calculated for the PI pad. 9 Where is the value calculated for the PI pad. Table 4b. Pad Value Calculations for Impedance Matched Systems Copyright 008 by Uneeda Audio. All rights reserved. evision A. Page

U Microphones Pic in > r ( mic ) r is the bridging ratio, typically 5. It should approximate the preamp s input impedance. Pic out mic ( ) Chec: 6 r if not, the pad s input impedance will be too low. Line Level Sources Pic 6 out 604 it can be some other value too. ( ) 6 Chec: in + + 6 This should be a value that the source can drive. If it is too low, then choose a higher value for 6 and recomputed. Table 5. Pad Value Calculations for Voltage based Systems (Bridging) evision History A. birth Copyright 008 by Uneeda Audio. All rights reserved. evision A. Page