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L6223 Datasheet(PDF) 17 Page - STMicroelectronics |
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L6223 Datasheet(HTML) 17 Page - STMicroelectronics |
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17 / 33 page ![]() The behaviour of the oscillator at each phase change allows the L6223 to drive high speed unipolar stepper motors. This is the main functional difference between the L6223 and the L6223 (see fig. 21b). In the latter, the phase change starts only when the clock pulse sets the F-F (Fig. 22) that is when the capacitor voltage reaches the discharge threshold. As a result, a variable delay between the leading edge of the input signal and the beginning of the current decay to zero can be expected. Because of that, driving high speedy stepper mo- tors is produced a noisy beating between chop- ping frequency and phase change rate. In the L6223 as soon as the phase change is driven by the inputs, the oscillator voltage Jumps to its top level, a new discharge period is gener- ated and the chopping transistor is switched ON (Q5 in fig. 22). The advantages are a motor phase change synchronous to the driving signal and no beating for whatever rotation speed. By setting pin 14 at a voltage equal or less than Vrs = 0.9V, when the IC is normally supplied and the oscillator is running, the 6 bit shift register is quickly reset and the power outputs are disabled: a delay of 700nsec max must be expected. The use of this behaviour to reset the device at the turn-on is not allowed; however the reset is automatically provided by the Logic Supply Volt- age crossing the threshold of 3.5V (typ.) both at the turn-ON and at the turn-OFF. Protection The protection zeners on the outputs protect the IC from overvoltage during chopping and phase change. Actually, at the phase change, the out- puts rise to a voltage equal to VO =2VS +Vm, where VS is the power supply and Vm the product of the motor resistance Rm with the peak phase current Ip. Vs is doubled because in the unipolar motor we have two coupled phases connected in series(phase A and A, B and B) for each of the two windings of the motor (MA, MB see Fig. 22). The leakage inductance, seen from the outputs of the L6223, can generate an overvoltage higher than VO. To protect the IC, the zeners must be able to sustain a power of 400W for 1 microsec and must be able to conduct at a voltage Vz higher than V0 =2Vs(max) +Vm. It’s important that during the transition, at the max operating ambi- ent temperature, the zener conduction is guaran- teed for a voltage lower than 125V (see Absolute Max Ratings). The ST-BZWO4-85 satisfies this requirement. The diode connected to the com- mon protects this input from the undergounds due to the leakage inductances and/or the imbalanc- ing between the phase currents. Figure21a:Relationshipbetweencapacitordischarge of the oscillator, window and sensing voltage Figure 21b: Oscillator behaviour of the L6223 and of the L6223 (simplified waveforms). L6223 17/33 |
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