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LTC4100 数据表(PDF) 40 Page - Linear Technology |
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LTC4100 数据表(HTML) 40 Page - Linear Technology |
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40 / 48 page ![]() LTC1760 40 1760fa Calculating IC Power Dissipation The power dissipation of the LTC1760 is dependent upon the gate charge of QTG and QBG.(Refer to Typical Application). The gate charge is determined from the manufacturer’s data sheet and is dependent upon both the gate voltage swing and the drain voltage swing of the FET. PD = (VDCIN – VVCC) • fOSC • (QTG + QBG) + VDCIN • IDCIN_CHG – VVCC • (ISAFETY1 + ISAFETY2) where: IDCIN_CHG, ISAFETY1, ISAFETY2 are defined in the previous section. Example: VVCC = 5.2V, VDCIN = 19V, fOSC = 345kHz, QTG = QBG = 15nC, IDCIN_CHG = 2.62mA, ISAFETY1 = ISAFETY2 = 218μA. PD = 190mW VSET/ISET Capacitors Capacitor C7 is used to filter the delta-sigma modulation frequency components to a level which is essentially DC. Acceptable voltage ripple at ISET is about 10mVP-P. Since the period of the delta-sigma switch closure, TΔΣ, is about 10μs and the internal IDAC resistor, RSET, is 18.77k, the ripple voltage can be approximated by: ΔV ISET = V REF •T Δ∑ R SET •C7 Then the equation to extract C7 is: C7 = V REF •T Δ∑ ΔV ISET •RSET = 0.8/0.01/18.77k(10μs) ≅ 0.043μF In order to prevent overshoot during start-up transients the time constant associated with C7 must be shorter than the time constant of C5 at the ITH pin. If C7 is increased to improve ripple rejection, then C5 should be increased proportionally and charger response time to average cur- rent variation will degrade. Capacitors CB1 and CB2 are used to filter the VDAC delta- sigma modulation frequency components to a level which is essentially DC. CB2 is the primary filter capacitor and CB1 is used to provide a zero in the response to cancel the pole associated with CB2. Acceptable voltage ripple at VSET is about 10mVP-P. Since the period of the delta- sigma switch closure, TΔΣ, is about 11μs and the internal VDAC resistor, RVSET, is 7.2kΩ, the ripple voltage can be approximated by: ΔV VSET = V REF •T Δ∑ R VSET CB1||CB2 () Then the equation to extract CB1 || CB2 is: C B1||CB2 = V REF •T Δ∑ R VSET ΔVVSET CB2 should be 10× to 20× CB1 to divide the ripple voltage present at the charger output. Therefore CB1 = 0.01μF and CB2 = 0.1μF are good starting values. In order to prevent overshoot during start-up transients the time constant as- sociated with CB2 must be shorter than the time constant of C5 at the ITH pin. If CB2 is increased to improve ripple rejection, then C5 should be increased proportionally and charger response time to voltage variation will degrade. Input and Output Capacitors In the 4A Lithium Battery Charger (Typical Application section), the input capacitor (CIN) is assumed to absorb all input switching ripple current in the converter, so it must have adequate ripple current rating. Worst-case RMS ripple current will be equal to one half of output charging current. Actual capacitance value is not critical. Solid tantalum low ESR capacitors have high ripple current rating in a relatively small surface mount package, but caution must be used when tantalum capacitors are used for input or output bypass. High input surge currents can be created when the adapter is hot-plugged to the charger or when a battery is connected to the charger. Solid tantalum capaci- tors have a known failure mechanism when subjected to very high turn-on surge currents. Only Kemet T495 series of “Surge Robust” low ESR tantalums are rated for high surge conditions such as battery to ground. APPLICATIONS INFORMATION |
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