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LTC4012-1 数据表(PDF) 21 Page - Linear Technology |
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LTC4012-1 数据表(HTML) 21 Page - Linear Technology |
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21 / 28 page ![]() 21 4012f LTC4012/ LTC4012-1/LTC4012-2 The output capacitor shown across the battery and ground must also absorb PWM output ripple current. The general formula for this capacitor current is: I V V V Lf RMS BAT BAT CLP PWM = ⎛ ⎝⎜ ⎞ ⎠⎟ 029 1 1 .• • – • For example, IRMS = 0.22A with: VBAT = 12.6V VCLP = 19V L1 = 10μH fPWM = 550kHz High capacity ceramic capacitors (20μF or more) available from a variety of manufacturers can be used for input/out- put capacitors. Other alternatives include OS-CON and POSCAP capacitors from Sanyo. Low ESR solid tantalum capacitors have high ripple cur- rent rating in a relatively small surface mount package, but exercise caution when using tantalum for input or output bulk capacitors. High input surge current can be created when the adapter is hot-plugged to the charger or when a battery is connected to the charger. Solid tan- talum capacitors have a known failure mechanism when subjected to very high surge currents. Select tantalum capacitors that have high surge current ratings or have been surge tested. EMI considerations usually make it desirable to minimize ripple current in battery leads. Adding Ferrite beads or inductors can increase battery impedance at the nominal 550KHz switching frequency. Switching ripple current splits between the battery and the output capacitor in inverse relation to capacitor ESR and the battery impedance. If the ESR of the output capacitor is 0.2 Ω and the battery impedance is raised to 4 Ω with a ferrite bead, only 5% of the current ripple will flow to the battery. Inductor Selection Higher switching frequency generally results in lower efficiency because of MOSFET gate charge losses, but it allows smaller inductor and capacitor values to be used. A primary effect of the inductor value L1 is the amplitude of ripple current created. The inductor ripple current ΔIL decreases with higher inductance and PWM operating frequency: ΔI V V V Lf L BAT BAT CLP PWM = ⎛ ⎝ ⎜ ⎞ ⎠ ⎟ •– • 1 1 Accepting larger values of ΔIL allows the use of low in- ductance, but results in higher output voltage ripple and greater core losses. Lower charge currents generally call for larger inductor values. The LTC4012 limits maximum instantaneous peak inductor current during every PWM cycle. To avoid unstable switch waveforms, the ripple current must satisfy: ΔI mV R I L SENSE MAX < ⎛ ⎝ ⎜ ⎞ ⎠ ⎟ 2 150 •– so choose: L V f mV R I CLP PWM SENSE MAX 1 0 125 150 > ⎛ ⎝⎜ ⎞ ⎠⎟ .• •– A reasonable starting point for setting ripple current is ΔIL = 0.4 • IMAX. The voltage compliance of internal LTC4012 circuits also imposes limits on ripple current. Select RIN (in Figure 1) to avoid average current errors in high ripple designs. The following equation can be used for guidance: RI μA R RI μA SENSE L IN SENSE L •• ΔΔ 50 20 ≤≤ APPLICATIONS INFORMATION |
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