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LTC1625IGN Datenblatt(PDF) 11 Page - Linear Technology |
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LTC1625IGN Datenblatt(HTML) 11 Page - Linear Technology |
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11 / 24 page ![]() 11 LTC1625 APPLICATIONS INFORMATION The corresponding average current depends on the amount of ripple current. Lower inductor values (higher ∆IL) will reduce the load current at which Burst Mode operation begins. The output voltage ripple can increase during Burst Mode operation if ∆IL is substantially less than IBURST. This will primarily occur when the duty cycle is very close to unity (VIN is close to VOUT) or if very large value inductors are chosen. This is generally only a concern in applications with VOUT ≥ 5V. At high duty cycles, a skipped cycle causes the inductor current to quickly descend to zero. However, it takes multiple cycles to ramp the current back up to IBURST(PEAK). During this interval, the output capaci- tor must supply the load current and enough charge may be lost to cause significant droop in the output voltage. It is a good idea to keep ∆IL comparable to IBURST(PEAK). Otherwise, one might need to increase the output capaci- tance in order to reduce the voltage ripple or else disable Burst Mode operation by forcing continuous operation with the FCB pin. Fault Conditions: Current Limit and Output Shorts The LTC1625 current comparator can accommodate a maximum sense voltage of 150mV. This voltage and the sense resistance determine the maximum allowed peak inductor current. The corresponding output current limit is: I mV R I LIMIT DS ON T L =()( ) 150 1 2 () – ρ ∆ The current limit value should be checked to ensure that ILIMIT(MIN) > IO(MAX). The minimum value of current limit generally occurs with the largest VIN at the highest ambi- ent temperature, conditions which cause the highest power dissipation in the top MOSFET. Note that it is important to check for self-consistency between the assumed junction temperature of the top MOSFET and the resulting value of ILIMIT which heats the junction. Caution should be used when setting the current limit based upon RDS(ON) of the MOSFETs. The maximum current limit is determined by the minimum MOSFET on- resistance. Data sheets typically specify nominal and maximum values for RDS(ON), but not a minimum. A reasonable, but perhaps overly conservative, assumption is that the minimum RDS(ON) lies the same amount below the typical value as the maximum RDS(ON) lies above it. Consult the MOSFET manufacturer for further guidelines. The LTC1625 includes current foldback to help further limit load current when the output is shorted to ground. If the output falls by more than half, then the maximum sense voltage is progressively lowered from 150mV to 30mV. Under short-circuit conditions with very low duty cycle, the LTC1625 will begin skipping cycles in order to limit the short-circuit current. In this situation the bottom MOSFET RDS(ON) will control the inductor current trough rather than the top MOSFET controlling the inductor current peak. The short-circuit ripple current is deter- mined by the minimum on-time tON(MIN) of the LTC1625 (approximately 0.5 µs), the input voltage, and inductor value: ∆IL(SC) = tON(MIN) VIN/L. The resulting short-circuit current is: I mV R I SC DS ON BOT T LSC = ()( )+ 30 1 2 ()( ) () ρ ∆ Normally, the top and bottom MOSFETs will be of the same type. A bottom MOSFET with lower RDS(ON) than the top may be chosen if the resulting increase in short-circuit current is tolerable. However, the bottom MOSFET should never be chosen to have a higher nominal RDS(ON) than the top MOSFET. Inductor Core Selection Once the value for L is known, the type of inductor must be selected. High efficiency converters generally cannot afford the core loss found in low cost powdered iron cores, forcing the use of more expensive ferrite, molypermalloy or Kool M µ® cores. Actual core loss is independent of core size for a fixed inductor value, but it is very dependent on the inductance selected. As inductance increases, core losses go down. Unfortunately, increased inductance requires more turns of wire and therefore copper losses will increase. Kool M µ is a registered trademark of Magnetics, Inc. |
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