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LT1777 Datasheet(PDF) 13 Page - Linear Technology |
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LT1777 Datasheet(HTML) 13 Page - Linear Technology |
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13 / 24 page ![]() 13 LT1777 APPLICATIONS INFORMATION through the main inductor has most of its energy concen- trated in the fundamental and lower harmonics.) Toroidal style inductors, many available in surface mount configu- ration, offer a reduced external magnetic field, generally at an increase in cost and physical size. Although custom design is always a possibility, most potential LT1777 ap- plications can be handled by the array of standard, off-the- shelf inductor products offered by the major suppliers. Selecting Bypass Capacitors The basic topology as shown in the Typical Application on the first page uses two bypass capacitors, one for the VIN input supply and one for the VOUT output supply. User selection of an appropriate output capacitor is rela- tively easy, as this capacitor sees only the AC ripple current in the inductor L1. As the LT1777 is designed for buck or step-down applications, output voltage will nearly always be compatible with tantalum type capacitors, which are generally available in ratings up to 35V or so. These tantalum types offer good volumetric efficiency, and many are available with specified ESR performance. The product of inductor AC ripple current and output capacitor ESR will manifest itself as peak-to-peak voltage ripple on the output node. (Note: If this ripple becomes too large, heavier control loop compensation, at least at the switching fre- quency, may be required on the VC pin.) The input bypass capacitor can present a more difficult choice. In a typical application e.g., 24VIN to 5VOUT, relatively heavy VIN current is drawn by the power switch for only a small portion of the oscillator period (low ON duty cycle). The resulting RMS ripple current, for which the capacitor must be rated, can be several times the DC average VIN current. The straightforward choice for a low volume, surface mountable electrolytic capacitor with good ESR/ripple current ratings is a tantalum type. How- ever, worst-case (high) input voltage coupled with stan- dard capacitor voltage derating may exceed the 35V or so for which tantalum capacitors are generally available. Relatively bulky “high frequency” aluminum electrolytic types, specifically constructed and rated for switching supply applications, may then be the only choice. Additionally, it may be advantageous to parallel the input and output capacitors with 0.1 µF ceramic bypass capaci- 500ns/DIV 1777 F06 GND Figure 6. LT1676 VSW Node Voltage Behavior for Comparison Purposes Only, VIN = 36V Selecting Main Inductor There are several parameters to consider when selecting a main inductor. These include inductance value, peak current rating (to avoid core saturation), DC resistance, construction type, physical size, and of course, cost. Once the inductance value is decided, inductor peak current rating and resistance need to be considered. Here, the inductor peak current rating refers to the onset of saturation in the core material, although manufacturers sometimes specify a “peak current rating” which is de- rived from a worst-case combination of core saturation and self-heating effects. Inductor winding resistance alone limits the inductor’s current carrying capability as the I2R power threatens to overheat the inductor. Remember to include the condition of output short circuit, if applicable. Although the peak current rating of the inductor can be exceeded in short-circuit operation, as core saturation per se is not destructive to the core, excess resistive self- heating is still a potential problem. The final inductor selection is generally based on cost, which usually translates into choosing the smallest physi- cal size part which meets the desired inductance value, resistance and current carrying capability. An additional factor to consider is that of physical construction. Briefly stated, “open” inductors built on a rod- or barrel-shaped core generally offer the smallest physical size and lowest cost. However their open construction does not contain the resulting magnetic field, and they may not be accept- able in RFI-sensitive applications. (A mitigating factor is that, as mentioned previously, the AC current passing |
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