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Audio, Power, andControl Lines
RF Feedback, Hum, and Distortion 
Improperly connectedor configured audio
 and power supply
 lines can cause hum
 or distortion in
 audio systems. This
 includes
 microphones,
 headsets, computer
 sound cards, and
 nearly any other low
 level audio system
 or device.
 
RF feedback is characterized by anything from a little distortion causing aslightly rough sound on transmitted audio, to highly-distorted, unintelligible,
 raspy bursts of audio. The gateway for RF feedback is always an equipment design
 limitation.
 
RF feedback, and even hum and noise ingress, requires a few things. First, theequipment must have some sort of
 shielding or wiring error, inside or outside the equipment. The wiring error
 or imperfect shielding allows RF feedback, but does not actually
 cause RF feedback. Less-than-perfect shielding and wiring technique problems are
 called to our attention by excessive common mode RF currents, or
 by exceptionally strong direct fields from nearby transmitting antennas. The
 problems are not actually created by the excessive current or
 field levels, but by a mix of design problems. Since problems are level
 sensitive, anything that increases electric or magnetic field levels, voltage,
 current, or power can highlight wiring and equipment shortfalls or problems. The
 true cause is less-than-perfect shielding and/or wiring in the presence of a
 problematic field level, current, or voltage. An ideal design has a reasonable
 compromise between equipment design time and cost, and allowable common-mode RF
 current levels and/or local field intensity levels.
 
Audio systems and RF systems behave the same in many ways, and behave quitedifferently in other ways. For example, at audio frequencies shield dc
 resistance is critical. At very high radio frequencies, gaps in braid and the
 angle of braid weave, control leakage. At very low frequencies shield resistance
 and material can be critical, while small gaps or weave angle might be
 meaningless. At radio frequencies, aluminum works as well as (and often much
 better than) steel for shielding magnetic fields. At audio frequencies, steel
 might be required to stop magnetic flux leakage.
 
At radio frequencies, even a very thin foil can be many skin depths thick. Thisis because the shield is not thick compared to
 skin depth at low frequencies.
 Nothing passes through the shield, neither magnetic nor electric fields. This is
 true even if the shield is thin aluminum foil, and braid thickness or shield
 thickness is nearly meaningless.
 
To be most reliable with reasonable equipment cost and wiring complexity,designers must understand balanced systems, unbalanced systems, shields, audio,
 and RF system behavior.
 
SSB transmitters draw a very large portion of dc power supply current in directproportion to audio input levels. The dc power supply negative ground lead can
 modulate a low-level audio line with the rough “brah
 waah braah” sound of
 SSB without a
 carrier. Many
 “RF-sounding”
 problems are
 actually caused by
 low frequency ac or
 dc ground loops from
 power supply
 negative leads,
 acting in concert with other grounding, wiring,
 or shielding shortfalls.
 
Treating Audio LinesCorrectly
In the early 1970’s through 80’s, I worked at various broadcast stations. Muchof the work was wiring studios and switching racks, which employed hundreds of
 line-level audio feeds.
 One very basic rule
 was followed by better, more-experienced audio and
 broadcast engineers. Never ground a shield at both ends of
 signal paths between different pieces of equipment. An audio
 shield, or any
 ground return lead
 with low-level
 audio, should only be grounded at the audio
 device’s input port, or at one end of a path.
 This prevents inducting noise and hum from ground loops between
 device cabinets, which are almost always at slightly different AC potential.
 This rule is often ignored by
 amateur radio
 operators and amateur radio equipment manufacturers.
 
 
PowerLine induced hum
 
Harmful ground loopsare caused by
 grounding sensitive
 leads or systems to
 different points. In
 this example current
 returning to the
 pole transformer
 causes a voltage
 drop along CABL1,
 from the pole to the
 house.
 
If we ground a lowlevel audio source,
 like V1, to any
 external ground some
 AC current from the
 mains neutral will
 partially flow
 through shield
 resistance (R1) and
 modulate source V1
 with hum.
 
Vac represents theAC loop caused by
 voltage drop in the
 power mains neutral
 system.
 
The ONLYcorrect place for an
 audio ground is at
 the microphone
 connector entrance
 to the shield
 enclosure of the
 radio. That ground
 has to be virtually
 zero resistance to
 the cabinet. Nothing
 else on the audio
 line should be
 grounded, unless it
 is grounded to that
 jack-to-chassis
 connection.
 
  
  
  
  
 
  
  
 Radios using mainspowered 13.8 VDC
 power supplies
 suffer all the same
 ill effects from
 power mains hum,
 plus they have a new
 problem. The small
 resistance (R4) of
 the negative lead
 allows the power
 supply to modulate
 audio lines at a
 rate tied to the SSB
 envelope. This
 produces and audio
 sound much like RFI
 or SSB with a BFO
 turned off. This
 voltage is
 represented by Vdc.
 
  
  
Again the faultoccurs because of
 the extra
 unnecessary ground
 at the audio source
 (V1).
 
Vac can occur alongwith Vdc, and
 usually does.
 
  
Once again the onlyplace the audio line
 should be grounded
 is at the entrance
 to the radio
 housing.
 
     
 
Computer to Radio
 Interfaces
 
While we can onoccasion get lucky
 and get away with
 breaking good
 engineering practice
 rules, we should use
 isolation
 transformers on
 audio lines. Many
 trashy PSK signals
 are created because
 users don’t isolate
 the grounds, and
 often times this
 trash is out of the
 receiver’s bandpass. Because
 the hum and noise is
 off-frequency from
 desired tones,
 many problems go
 unnoticed (except by
 people up or down
 the band who have
 noise or hum pop on
 their frequency when
 someone up or down
 the band transmits).
 
 T1 and T2 isolatethe ground paths on
 the computer and the
 ground paths on the
 radio cabinet or
 chassis. Without T1
 and T2 the
 resistance of the
 shields would drop
 voltage, and that
 voltage would
 effectively be in
 series with the
 audio inputs and
 outputs.
 
This can result inhum, or the dc power
 amplifier current of
 a power amplifier
 using an external
 supply modulating
 the audio system.
 
T1 and T2 can besmall audio
 transformers of
 150-1000 ohms
 impedance.
 
  
  
  
  
 
This is my houseoperating desk audio
 system. The
 transformers are
 normally behind the
 radios out of sight.
 
Pay particularattention to the
 nylon insulator
 system on my CW key
 jack. This is to
 prevent the CW
 keyer, which
 operates on 13.8
 volts dc as well as
 connecting to the
 radio, from
 grounding to the
 headphone jack
 ground. If I short
 the key jack shell
 to the metal panel
 where audio lines
 are “grounded”, hum
 appears in the
 headset.
 
The green audio linetransformers are
 42TU013-RC They are
 8-ohm CT to 1000-ohm
 CT 1/2-watt
 transistor output
 transformers. I run
 the radio speaker
 audio output into
 the full eight-ohm
 winding. I use half
 of the 1000-ohm
 winding to drive the
 audio switching and
 buss system. The
 audio buss (gray
 cable) is terminated
 in  47-ohm
 resistors for each
 of the four audio
 channels.
 
The computerinterface connects
 through the red
 transformers, which
 are 500:500 ohm
 Xicon 42TU500
 transformers.
 
  
  
  
  
  
 
This is my basic headphone wiring in both my contest barn and house shack. Itcan be built out to handle as many radios as necessary, and will interface in
 stereo. It allows any radio to be on any ear, and multiple switch and jack units
 can be bridged.
 
The buss in my contest barn covers 4 operating tables in stereo. The left half of the schematic drives the audiobuss, the right half bridges the audio buss. With a low source impedance (like
 the speaker output of a radio) driving the buss, plus the intentionally heavy
 buss loading resistances R1 through R3(+), volume changes are minimal as
 headphones are switched in or out on any given radio.
     Special note on T1-T3(+) . As many transformers canbe added as the S1 and S2 will accommodate. The windings are center tapped. I
 use the full 8-ohm winding for the input from radios, and only half of the
 secondary to drive the audio buss. This makes the impedance ratio around 4 : 125
 ohms. I load the secondary intentionally slightly heavy with no ill effects. The
 extra winding impedance extends low frequency response and limits the highs
 slightly, to slightly reduce hiss in headphones when using narrow CW filters.
   
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    Audiotransformer test
 for you!
 
    If I have an1000-ohm CT
 transformer and
 I only use
 one-half of the
 winding, from
 one end to the
 center tap, what
 is the new
 winding
 impedance?
 
 
    Most peopleintuitively
 answer 500 ohms.
   
    The impedance is
 250 ohms! This
 is because
 impedance
 changes by the
 square of the
 turns ratio. The
 center tap to
 one end is half
 of the turns, so
 it has 1/4th the
 impedance.
 
    An 8-ohm center
 tapped winding
 is not 4 ohms
 each side of
 center tap, it
 is 2 ohms
 each side of
 center tap.
 Double the turns
 ratio and we
 have four times
 the impedance.
 Halve it, and we
 have 1/4 the
 impedance.
   |  
  
Moreon Transformer
 Impedance
 
When a transformerhas too little
 impedance low
 frequency response
 suffers. It also
 saturates easier.
 When the transformerimpedance is too
 high, high frequency
 response suffers.
 It is the load thatdetermines the
 “match” for
 transformer
 impedance, not the
 source. If we want
 a 600-ohm
 transformer to be
 flattest running
 into a 10K ohm
 radio input , we
 should connect a
 680-ohm resistor
 across the secondary
 (load) side going
 into the radio. The
 10,000 ohm radio can
 then bridge directly across
 the loaded
 secondary. If we
 needed to match the
 10,000 ohms because
 the input of the
 radio is fussy
 (this is normally
 not an
 issue when a high-Z
 load bridges a low-Z
 source) we could
 use an L-pad. A
 suitable L-pad would
 be a 680 ohm
 resistor to ground,
 and a 10,000 ohm
 series resistor to
 the high impedance
 load. Power loss
 would be almost
 20-dB.
 
As for thetransformer going to
 the computer, most
 computers should
 have a line input
 impedance or be
 designed to bridge
 the source without
 issues so long as
 the source Z is less
 than load Z
 presented by the
 computer. If we
 wanted to get fussy
 we could load the
 secondary and bridge
 across it with the
 computer.
 I very rarely findit necessary, unless
 I want high fidelity
 or maximum power
 transfer, to worry
 about getting an
 optimum match. All
 of my radios go into
 an 8-ohm to 250-ohm
 audio transformer
 to drive the audio
 busses in the shack.
 This transformer is
 an 8- to 1000-ohm
 transformer, and
 only use half of the
 1000-ohm winding. There are separate
 isolation
 transformers on each
 piece of gear at the
 outputs, including
 the computer.
 Shields are ONLY
 grounded at inputs.
 Without
 this I have audio
 line noise and hum.
 
Wiring Blocks
To facilitate moving things around on my desks, I use movable wiring blocks.This minimizes the number of individual wires or cables running all over the
 room. In this example I have several power plugs connected to one supply line
 (fused at the source). The CAT5 cables connected to other items on the shelf,
 like antennas switches.
 
Every pin number, color code, and functions gets documented on a list! 
 
 
  
  
  
  
  
  
  
  
  
  
  
  
 
  
  
  
  
  
  
  
  
  
  
  
  
  
  
  
  
  
  
  
  
  
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