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The goniometer is a device that can produce any desired phase shift with respect to an input voltage. Since it may not be apparent how this can be acheived, the description below expands on this.
 | In this diagram are a fixed coil A-B and an additional coil C-D which may be rotated about its centre with respect to the fixed coil. In the situation shown, if an RF voltage is applied across A-B then a current will flow in the coil, and by transformer action, a current will be induced in the rotatable coil C-D. The voltage produced across C-D will be in the same phase as the the voltage across A-B. |
 | In this diagram, the moving coil has been rotated through 180 degrees. The voltage produced across C-D will now be 180 degrees out of phase with the voltage across A-B. By rotating the moving coil to other positions, corresponding changes in phase will result. |
 | There is however a slight snag, which is that when the two coils are at 90 degrees to each other, no magnetic coupling occurs and hence there will be no output when the moving coil is set as shown here. |
 | To overcome this, an extra fixed winding is provided which is connected to the same voltage A-B but through a capacitor C1. This component is chosen so that the current in the horizontal coil is 90 degrees out of phase (in other words, in phase quadrature) to that in the vertical coil. Now, when the moving coil is rotated to the 90 degree position, an output results which is 90 degrees out of phase with the voltage A-B.
Any phase may now be obtained at will merely by positioning the moving coil appropriately with respect to the fixed coils. |
We now have a means of generating any desired phase shift in an RF signal between 0 and 360 degrees. In the HiFix receiver, the goniometer is used as part of the display system. Consider the diagram below, which shows a part of the display block. An electric motor drives a reduction gear, which rotates the goniometer. It also rotates a mechanical counter display, such that one complete turn of the goniometer changes the display by 1.00
Let us assume for a moment that the IF input is in phase with the master oscillator and the goniometer is set for zero phase shift. Then the two inputs to the discriminator will be in phase, and its output at point A will by zero. The servo amplifier output will also be at zero and the motor will be at rest. Under these conditions, we can mechanically zero the display if we wish to read 000.00.
Now if the IF signal phase has changed, because we have moved with respect to the master and slave transmitters- then the phase of the two inputs to the discriminator will be different, and accordingly an ouput voltage will appear corresponding to the amount and direction of phase difference. The servo amplifier will now drive the motor in the appropriate direction, thus turning the goniometer, until the zero phase condition has been restored. Here's an example:
We have moved 0.1 of a lane away from the master and slave stations. This will correspond to a phase change of +36 degrees. The discriminator output will now be a small positive voltage, which will cause the servo amplifier to drive the motor in the direction needed to move the goniometer until its output is also at +36 degrees, i.e until the difference between the discriminator inputs is restored to zero. When this has been achieved and the motor is once again at rest, the mechanical gearing will have moved the goniometer by 0.1 turn, and the mechanical display counter will read 000.10.
There are of course two displays, one for each of the two patterns: master - slave 1, and master - slave 2.
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