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LTC1530CS8 Datasheet(PDF) 13 Page - Linear Technology |
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LTC1530CS8 Datasheet(HTML) 13 Page - Linear Technology |
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13 / 24 page ![]() 13 LTC1530 Inductor Selection The inductor is often the largest component in an LTC1530 design and must be chosen carefully. Choose the inductor value and type based on output slew rate requirements and expected peak current. The required output slew rate primarily controls the inductor value. The maximum rate of rise of inductor current is set by the inductor’s value, the input-to-output voltage differential and the LTC1530’s maximum duty cycle. In a typical 5V input, 2.8V output application, the maximum rise time will be: DC VV LL MAX IN OUT − = 185 . A s µ where L is the inductor value in µH. With proper frequency compensation, the combination of the inductor and output capacitor values determine the transient recovery time. In general, a smaller value inductor improves transient response at the expense of ripple and inductor core saturation rating. A 2 µH inductor has a 0.9A/µs rise time in this application, resulting in a 5.5 µs delay in responding to a 5A load current step. During this 5.5 µs, the difference between the inductor current and the output current is made up by the output capacitor. This action causes a temporary voltage droop at the output. To minimize this effect, the inductor value should usually be in the 1 µH to 5 µH range for most 5V input LTC1530 circuits. Different combinations of input and output voltages and expected loads may require different values. Once the required inductor value is selected, choose the inductor core type based on peak current and efficiency requirements. Peak current in the inductor is equal to the maximum output load current plus half of the peak-to- peak inductor ripple current. Inductor ripple current is set by the inductor’s value, the input voltage, the output voltage and the operating frequency. If the efficiency is high, ripple current is approximately equal to: I VV V fL V RIPPLE IN OUT OUT OSC O IN = − ()( ) ()( )( ) where fOSC = LTC1530 oscillator frequency LO = Inductor value Solving this equation for a typical 5V to 2.8V application with a 2 µH inductor, ripple current is: 22 056 300 2 2 .. V kHz H A ()( ) ()( ) = µ P-P Peak inductor current at 11.2A load: 11 2 2 2 12 2 .. A A A += The ripple current should generally fall between 10% and 40% of the output current. The inductor must be able to withstand this peak current without saturating, and the copper resistance in the winding should be kept as low as possible to minimize resistive power loss. Note that in circuits not employing the current limit function, the current in the inductor may rise above this maximum under short circuit or fault conditions; the inductor should be sized accordingly to withstand this additional current. Inductors with gradual saturation characteristics (example: powdered iron) are often the best choice. Input and Output Capacitors A typical LTC1530 design places significant demands on both the input and the output capacitors. During normal steady load operation, a buck converter like the LTC1530 draws square waves of current from the input supply at the switching frequency. The peak current value is equal to the output load current plus 1/2 the peak-to-peak ripple cur- rent. Most of this current is supplied by the input bypass capacitor. The resulting RMS current flow in the input capacitor heats it and causes premature capacitor failure in extreme cases. Maximum RMS current occurs with 50% PWM duty cycle, giving an RMS current value equal to IOUT/2. A low ESR input capacitor with an adequate ripple current rating must be used to ensure reliable operation. Note that capacitor manufacturers’ ripple cur- rent ratings are often based on only 2000 hours (3 months) lifetime at rated temperature. Further derating of the input capacitor ripple current beyond the manufacturer’s speci- fication is recommended to extend the useful life of the circuit. Lower operating temperature has the largest effect on capacitor longevity. APPLICATIO S I FOR ATIO |
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