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LT1956IGN データシート(PDF) 21 Page - Linear Technology |
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LT1956IGN データシート(HTML) 21 Page - Linear Technology |
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21 / 28 page ![]() 21 LT1956/LT1956-5 1956f APPLICATIO S I FOR ATIO Input Voltage vs Operating Frequency Considerations The absolute maximum input supply voltage for the LT1956 is specified at 60V. This is based on internal semiconduc- tor junction breakdown effects. The practical maximum input supply voltage for the LT1956 may be less than 60V due to internal power dissipation or switch minimum on time considerations. For the extreme case of an output short-circuit fault to ground, see the section Short-Circuit Considerations. A detailed theoretical basis for estimating internal power dissipation is given in the Thermal Calculations section. This will allow a first pass check of whether an application’s maximum input voltage requirement is suitable for the LT1956. Be aware that these calculations are for DC input voltages and that input voltage transients as high as 60V are possible if the resulting increase in internal power dissipation is of insufficient time duration to raise die temperature significantly. For the FE package, this means high voltage transients on the order of hundreds of milli- seconds are possible. If LT1956 (FE package) thermal calculations show power dissipation is not suitable for the given application, the LT1766 (FE package) is a recom- mended alternative since it is identical to the LT1956 but runs cooler at 200kHz. Switch minimum on time is the other factor that may limit the maximum operational input voltage for the LT1956 if pulse-skipping behavior is not allowed. For the LT1956, pulse-skipping may occur for VIN/(VOUT + VF) ratios > 4. (VF = Schottky diode D1 forward voltage drop, Figure 5.) If the LT1766 is used, the ratio increases to 10. Pulse- skipping is the regulator’s way of missing switch pulses to maintain output voltage regulation. Although an increase in output ripple voltage can occur during pulse-skipping, a ceramic output capacitor can be used to keep ripple voltage to a minimum (see output ripple voltage compari- son for tantalum vs ceramic output capacitors, Figure 3). FREQUENCY COMPENSATION Before starting on the theoretical analysis of frequency response, the following should be remembered—the worse the board layout, the more difficult the circuit will be to stabilize. This is true of almost all high frequency analog circuits, read the Layout Considerations section first. Common layout errors that appear as stability problems are distant placement of input decoupling capacitor and/ or catch diode, and connecting the VC compensation to a ground track carrying significant switch current. In addi- tion, the theoretical analysis considers only first order non-ideal component behavior. For these reasons, it is important that a final stability check is made with produc- tion layout and components. The LT1956 uses current mode control. This alleviates many of the phase shift problems associated with the inductor. The basic regulator loop is shown in Figure 10. The LT1956 can be considered as two gm blocks, the error amplifier and the power stage. Figure 11 shows the overall loop response. At the VC pin, the frequency compensation components used are: RC = 2.2k, CC = 0.022µF and CF = 220pF. The output capacitor used is a 100 µF, 10V tantalum capacitor with typical ESR of 100m Ω. The ESR of the tantalum output capacitor provides a useful zero in the loop frequency response for maintaining stabil- ity. This ESR, however, contributes significantly to the ripple voltage at the output (see Output Ripple Voltage in the Applications Information section). It is possible to reduce capacitor size and output ripple voltage by replac- ing the tantalum output capacitor with a ceramic output capacitor because of its very low ESR. The zero provided by the tantalum output capacitor must now be reinserted back into the loop. Alternatively, there may be cases where, even with the tantalum output capacitor, an addi- tional zero is required in the loop to increase phase margin for improved transient response. A zero can be added into the loop by placing a resistor (RC) at the VC pin in series with the compensation capacitor, CC, or by placing a capacitor (CFB) between the output and the FB pin. When using RC, the maximum value has two limitations. First, the combination of output capacitor ESR and RC may stop the loop rolling off altogether. Second, if the loop gain is not rolled off sufficiently at the switching frequency, output ripple will perturb the VC pin enough to cause unstable duty cycle switching similar to subharmonic |
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