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IXMS150PSI 数据表(PDF) 7 Page - IXYS Corporation |
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IXMS150PSI 数据表(HTML) 7 Page - IXYS Corporation |
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7 / 10 page ![]() I - 41 © 1998 IXYS All rights reserved Use the formula C2 = 100 µF 100 kHz/f OSC for other frequencies. With V DD = 12 V and an oscillator fre- quency of 100 kHz, the bias generator should be able to source 3 mA at -2.4 V using these component values. This capability may be used to power other external circuitry as long as there is sufficient remaining negative bias to allow the IXMS150 to operate properly. Impact of PWM Frequency on System Operation PWM switching frequency has a pronounced effect on ripple current through the motor windings, the resul- ting eddy current losses in the motor, and system efficiency. As expected, motor current ripple goes down as frequency increases and therefore losses resulting from ripple currents are also reduced. Switching frequency also impacts losses in the power stage. These losses are associated with the energy necessary to turn on and off the power MOSFEts and are proportional to the switching frequency. In addition, the switching frequency has a limiting effect on maximum current loop band- width and therefore system bandwidth and therefore system bandwidth and maximum motor velocity. Oscillator The oscillator block diagram is shown in Fig. 6. The frequency is set by the values of R O and CO: f OSC = 1/RO (CO + CP)) (10) Note: C P is a 38 pF (typ.) internal parasitic capacitor. IXMS 150 V A 1/F O V(t) 2 V (PIN 7) 7 V (PIN 7 Open) [ ] V A = 1/f OSC = Ro (Co + Cp) > > Fig. 6a: Oscillator Block Diagram Fig. 6b: Oscillator Waveform Diagram Feedforward The amplitude of the oscillator wave- form and overall system gain are modu- lated by the voltage applied to the feedforward pin (FFWD). This is nomi- nally 3.5 V which should be divided down from the motor high voltage supply. This will allow system band- width to be maximized by making overall system gain inversely propor- tional to the motor supply voltage. Refer to Fig. 7 for an example of how feedforward is connected to the motor supply. It is recommended that a filter capacitor be connected from FFWD to AGND to filter noise spikes from the motor supply. Its value should be chosen so that the time constant of the capacitor and the parallel combination of R ff1 and Rff2 is such that switching noise will be filtered but not variations in the motor supply such as 120 Hz ripple, etc. Minimum Pulse Width The minimum output pulse width can also be modified by adjusting the oscil- lator capacitor C O. The relationship is: t pw(min) = Rmp (CO + Cp)(11) Note: R mp is a 3.6 kΩ (typ.) internal resistor, and C p is a 38 pF (typ.) internal parasitic capacitor. Dead Time Dead time is adjusted via the external oscillator capacitor C O. There is an internal resistor in the dead time circuit as well. The relationship is: t DT = RDT (CO + Cp) (12) Note: R DT is a 1.4 kΩ (typ.) internal resistor and C p is a 38 pF (typ.) internal parasitic capacitor. Fig. 7 Feedforward Connection Diagram Motor Slew Rate Limitations The maximum motor velocity in a microstepping application is determined by the maximum rate of change of the phase currents. Once this limit is reached the system is slew rate limited, at which point the peak undistorted phase current times the frequency of the input command is a fixed value. The theoretical limit for the maximum di/dt of the phase currents is determined by the motor supply voltage and the inductance of the motor: di/dt (max) = V HV/Lm (13) The limit does not take into account the back EMF of the motor, the bandwidth of the current loop driving the motor, or the minimum pulse width. The motors backEMF willtend to reduce the voltage applied across the motor windings, effectively reducing the maximum slew rate. The bandwidth of the current loop must also be high enough so as not to degrade system performance. Non-Circulating Operating Mode The IXMS150 is designed to control an H-bridge in the non-circulating mode. The equivalent circuit for an H-bridge is shown in Fig. 8. In the non-circulating 1/f OSC |
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