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IXDP630PI 数据表(PDF) 5 Page - IXYS Corporation |
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IXDP630PI 数据表(HTML) 5 Page - IXYS Corporation |
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5 / 7 page ![]() I - 18 © 1998 IXYS All rights reserved IXDP630 IXDP631 Selecting Components for a Specific Requirement Deadtime in the IXDP630/631 is exactly 8 clock periods: DT= 8/fclk. Once the worst case (minimum) deadtime has been determined (from Power switching component manufacturer data sheets, drive circuit analysis, breadboard measurements, etc.) the clock frequency is calculated: fclk(max) = 8/ DT(min). This is the highest allowable clock frequency, including the effects of initial accuracy, tolerance, temperature coeffi- cient, etc. When choosing oscillator components, special attention to resistor and capacitor construction is mandatory. Oscillator Design There are two versions of the deadtime generator. They have distinctly different internal oscillator designs to serve different application. In either case, however, the internal oscillator can be disabled by simply leaving its external components off. An HCMOS compatible clock up to 24 MHz can be fed directly into the RCIN or XTLIN pin. IXDP630 RC Oscillator Design The IXDP630 uses a Schmitt trigger inverter oscillator (Fig. 3). Two external components, R OSC and COSC, determine the clock frequency and consequently the deadtime. This design allows a significant cost reduction over a standard crystal oscillator, but entails a trade-off in frequency accuracy. The initial accuracy and drift are a function of the external component tolerance and temperature coefficients, supply voltage, and IXDP630 internal para- meters. At frequencies under 1 MHz, assuming the external components were perfect, the IXDP630 would introduce an initial accuracy error of 5 %, and a temperature dependence of -400 ppm. The shift in frequency over the V CC range 4.5 V to 5.5 V is typically less than 5 %. At higher frequencies and with resistor values below 1 kΩ, the IXDP630 internal parameters become more influential factors. This results in greater frequency variation from one device to another, as well as with temperature and supply voltage variations. If high accuracy is a requirement, the IXDP631 with a crystal oscillator would be the better choice. Oscillator frequency vs. Rosc and Cosc is shown in Fig. 4. For an analytical method of setting the oscillator, the design equation is for operation below 1 MHz approximately: 0.95 f OSC ≈ Cosc Rosc For operation above 1 MHz, 0.95 f OSC ≈ Cosc (Rosc+30) + 3 10-8 IXDP631 Precision Crystal Oscillator Design The IXDP631 uses a more common standard internal crystal oscillator design. For proper operation the crys- tal must be of the parallel resonant type, resonating at the crystal's funda- mental frequency. Fig. 5 illustrates the recommended oscillator configuration. Note the external components required. The capacitors are needed to achieve the calibrated crystal frequency (their value is determined by the crystal manufacturer), and the resistor is necessary to assure that the circuit starts in every case. While the circuit will usually operate without these extra parts, this is not recommended. The crystal oscillator in the IXDP631 is significantly more accurate than the RC oscillator in the IXDP630. The total tolerance (including effects of initial accuracy, temperature, supply voltage, drift, etc.) is better than ±100 ppm. This improves the accuracy and repeatability of the desired deadtime, but at the added expense of a crystal. Which version is appropriate for your application? That depends on how you are willing to trade off component cost for deadtime accuracy. Fig. 4. Oscillator frequency component selection for IXDP630. Fig. 3: IXDP630 internal Schmitt Trigger inverter oscillator (R OSC, COSC are external) C OSC = 470 pF C OSC = 270 pF C OSC = 100 pF C OSC = 47 pF C OSC = 1 nF C OSC = 2.2 nF C OSC = 4.7 nF C OSC = 10 nF 0.1 1 10 100 1000 10 000 Oscillator - kHz |
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