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Pre-zero crossing detector improves automotive relay performance

Posted: 29 Feb 2008 ?? ?Print Version ?Bookmark and Share

Keywords:pre-zero crossing detector? automotive relay performance? relays?

By John Bottrill
Texas Instruments

Relays are used to connect, or disconnect, ring generators to-and-from telephone lines. If the two points are at different potentials, there are high-current transients at the moment of contact.

Figure 1
(Click to view image.)

This results in arcing and pitting of the contacts which shortens a relay's life from contact failures and causes expensive repairs.

For these reasons, having the contact "make", or "break", at the moment of zero potential between the two points is desirable. However, relays can take a "long time" in terms of modern electronics to transition from the open-to-closed position or from the closed-to-open position. This paper discusses a method of developing a signal that will close, or open, a relay so that the contacts close, or open, when the ring generator's ring signal is at zero potential.

This discussion includes describing a circuit that provides a simple circuit delivering a pulse for both the negative- and positive-side zero crossing and anticipating the zero crossing by a fixed-time, or the time necessary for the relay to operate.

Figure 2
(Click to view image.)

In a ring generator, the relay's finite operating time is a significant portion of the period of the incoming ring voltage. If switching at the desired voltage is to occur, it's important to have the pulse initiation take place at a defined time preceding the ring signal's desired voltage.

The principal of the circuit is simple. By connecting a capacitor and resistor in series with one end connected to the signal and the other to the ground, it is possible to have the current through the series combination lead the voltage. The phase shift will be a function of the two elements. For instance, a series-connected R/C circuit, where the R is 60ks and the C is 200nF, will have the current leading the voltage by 33.5.

Figure 1 shows a simple R/C circuit and the relationship of the voltage and current through that simple R/C circuit. The current is leading relative to the voltage.

The sine wave that carries the ring voltage has a DC offset, so the positive-going crossing is at a different angle and slope than the negative-going crossing and neither is at the zero, or the 180, point of the voltage's sine wave.

Because the capacitor blocks DC, the current waveform is symmetrical at zero while the voltage that has a -48V offset is symmetrical at the -48V level. However, the offset means that it is not symmetrical about the ground.

Figure 3: The effects of adding a resistor across the capacitor ; circuit (upper) and waveform (lower).

Figure 2 shows a method of generating a simple zero current-crossing detector.

With this detector and the current leading the voltage, it is possible to generate pulses (see Figure 7 for the pulse-generating circuit) prior to the voltage crossing zero.

In Figure 2, the voltage at the anode of D2 (labeled VD2) goes to one diode drop above 5V for current flowing out of R2 into the junction with D2. It then goes one diode drop below ground for current flowing into R2 from the junction with D3. This transition signifies a change in the current's polarity.

Figure 4a
(Click to view image.)

Deal with non-symmetry
However, as shown in Figure 2, the current is still symmetrical about zero. This results in the two current crossings not proceeding across the voltage crossings by the same amount.

There are significant differences caused by the DC-offset of the voltage. These differences can be partially compensated for by the addition of a resistor across the capacitor C1.

With the addition of a resistor across the capacitor C1 (Figure 3), a DC-component is added to the current similar to that of the voltage which this gives an asymmetrical zero current-crossing.

Figure 4b
(Click to view image.)

The current crossover detector voltage (VD2 anode) and the sinewave voltage trace are marked with arrows in Figure 4 showing how close these two waveforms are to crossing the zero point, relative to each other.

Using this phase-shift and the DC-offset that the added resistor causes to the current trace, a lead factor can be programmed into the current so that the current crosses zero at a point prior to the voltage crossing zero in nearly the same amount of time. The relay requires that the coil be energized approximately 2.5ms prior to the relay's closing.

A time of 2.5ms is the equivalent of an 18 angle, for a 20Hz signal. Using Mathcad and solving the equation for the inverse angle of the impedance where R2 is allowed to vary results in:

Graph 1: Angle equation and graph of equation results.

From equation 1 and Graph 1, the value of R2 can be set to 41.7 k. Unfortunately, the zero crossing of the down slope and the up slope are still not the same pre-determined time, as shown by the arrows in Figure 4. Neither meets the requirement as the time from the current zero crossing to the voltage zero crossing is greater than needed for the upslope and the reverse for the downslope.

Figure 5
(Click to view image.)

By increasing R2 to 60k, the upslope time meets the requirement of about 2.5ms prior to the voltage crossing but the downslope is only about 1ms. In the remaining 1.5ms, the voltage would have dropped by 20V, causing a significant voltage to be present at the time the contacts of the relay either "opened" or "closed" (Figure 5).

If there is an additional resistor and diode added from the capacitor to ground (D4 and R4 in Figure 6), it will affect only one polarity of the current.

With the configuration shown, the change in timing of the positive current is the only parameter that is being affected by the new components.

Figure 6: Final circuit (upper) and resultant waveforms (middle); expanded part of waveform showing both transitions (lower).

Putting it all together
Using this complete circuit and the zero-current detector, it is possible to generate a pulse that indicates a pre-determined time ahead of the voltage crossings. At this point, the relay was "triggered" to close at the time of the zero-voltage crossing.

Figure 7: Pre-crossover detector and pulse-generator schematic.

As shown in Figure 6, the detector pulse for both the positive-and-negative crossing precedes the actual crossing by approximately the same amount. This addition allowed the use of the same circuit in Figure 7 for detecting both the positive and negative pre-crossover points.

Figure 8
(Click to view image.)

This pulse also allowed the circuit to trigger the relay so that the contacts closed at the zero-voltage crossing. The results: longer contact life and higher product reliability.

The circuit was built and tested with a UCC3570 ring generator controller (Figure 8) generating the "ring" signal.

Those results are shown in the scope waveforms (Figure 9a).

The test used the circuit from Figure 8 to generate zero-current crossing pulses. There was good correspondence between the simulated results and the actual measured results as can be seen below in Figure 9 which shows measured against simulated.

Figure 9: Measured results (upper) compared to simulated results (lower) for the circuit in Figures 6 and 8.

In Figure 10, both the measured and calculated results are shown for comparison purposes.

The scaling is increased so that measurements could be taken. The current transition, and hence the trigger pulse, occurs approximately 2.5ms before the actual voltage zero voltage crossover.

Figure 10: Measured results (upper) vs. calculated results (lower) for the circuit of figure 7.

This circuit provides a programmable anticipation of the zero-voltage crossing of the voltage waveform. By anticipating when the zero crossing will occur and starting the relay's action early to take the time of operation into account, the relay closure can occur at the zero-voltage crossing. This results in the contacts being protected from damage due to arcing and increases the life of the relay thus reducing the maintenance cost and increasing the total unit's mean time between failure.

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