Building your own Phase Coupler and Noise Blocker

Phase Coupler

The following trivial circuit can become an efficient phase coupler for X-10 signals.  The circuit shown below is a series-connected R-L-C circuit which tunes out the capacitor's reactive impedance. Used for phase coupling, it would be connected across two 110VAC phases leading to your power panel in your house.  The closer you can mount/connect this coupler to your panel, the better..

I suspect that this $4 circuit is the phase coupler sold commercially for 20 times as much. Alternatively, they can be wired right into the breaker box.

Phase coupling: The components are small enough to be built into a 2 or 3 phase plug. Electric code dictates no circuitry in breaker boxes, so build a plug, if you're a purist.

Bill of materials for each phase couple (three phase systems would need double of this):

Procedure:
  1. Connect a 18uH inductor in series with a 0.1uF,630V capacitor in series with a 0.25A fuse.
  2. Connect these between phases that need to be coupled in the plug.
  3. It is highly recommended that these connections made to your power panel be made via a spare 3 phase circuit breaker in your panel.
Simple theory behind it:

The inductor-capacitor values are such that they resonate at the frequency of typical X-10 signals, thus allowing the X-10 signals to pass across to the other phase.

The complex impedance of a capacitor is: Z = [1/jwC]. X10 signals are sent at 120KHz. At this frequency, a 0.1uF capacitor would create an impedance of 13.2 ohm, which might hinder obtaining equal signal strength on the two phases. A larger capacitor could be used, but that is more expensive, physically larger, and increases the reactive power load on the circuit from the 2.2 VA with 0.1 uF capacitor.

The series R-L-C circuit complex impedance is given by:

where w = 2(pi)f. The resonating frequency in which the capacitive reactive impedance is canceled is for L = 1/(Cw^2). At this value of L, the circuit impedance is purely resistive with Z = R. The circuit is tuned to resonate at the frequency.

The inductance required to bring a 0.1uF capacitor to resonance at 120 KHz is 17.6 uH. A 18uH inductance is an "off the shelf" value.

The finished signal-bridge therefore consisted of a 0.1uF 630 V capacitor in series with a 18uH inductor - plus a 1/4 amp fuse.
 

 

Another Noise Blocker/Filter

The X-10 noise block/filter circuit acts just the opposite as the coupler circuit in that instead of "passing: the X-10 signal, it "blocks" the X-10 signal.

LEVITON 5 AMP X-10 AC FILTER MODEL # 6287 SCHEMATIC
----------------------------------------------------

                  7uH*          7uH*

  BLACK  ----+---))))))---+---))))))---+----  BLACK
             |            |            |
             |    | |     |     | |    |
             -----| |-----+-----| |-----
                  | |     |     | |
                          |
               0.22uF   -----  0.22uF
                        -----
                          | 1uF
* 12 turns #18 wire       |
   on a toroidial core    /
   0.5" OD                \   "FUSE" (1 strand #18 wire on PCB)
   0.25" ID               /          (probably about 1 amp)
   0.25" THICK            |

                        WHITE
 
 

A simulated response of this "notch" filter is shown below.  As can be seen, it blocks well around the 120-130KHz frequencies (the frequency of typical X-10 signals):

x10filter.jpg (45154 bytes)
 

Figure 7 below shows a noise block connected in a fixture (Line side). Figure 8 shows a noise block connected at module (load side). Black are the live leads, white the
neutral lead. In both cases it couples any 120kHz signal generated by the noisy device to ground.


 


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