
Irms = Vin
Vout x (Vin ± Vout)
Iload x
CMIN = ('Vt)2 - ('It x Re)2
'Vt -
L x ©
§
©
§
Vout x Re
2
LM26001
,
LM26001-Q1
www.ti.com
SNVS430I –MAY 2006–REVISED MARCH 2015
Where ΔVt is the allowed voltage excursion during a load transient, and ΔIt is the maximum expected load
transient. If the total ESR is too high, the load transient requirement cannot be met, no matter how large the
output capacitance. If the ESR criteria for ripple voltage and transient excursion cannot be met, more capacitors
should be used in parallel. For non-ceramic capacitors, the minimum output capacitance is of secondary
importance, and is determined only by the load transient requirement.
If there is not enough capacitance, the output voltage excursion will exceed the maximum allowed value even if
the maximum ESR requirement is met. The minimum capacitance is calculated as follows:
(14)
It is assumed the total ESR, Re, is no greater than ReMAX. Also, it is assumed that L has already been selected.
Generally speaking, the output capacitance requirement decreases with Re, ΔIt, and L. A typical value greater
than 100 µF works well for most applications.
8.2.2.4 Input Capacitor
In a switching converter, very fast switching pulse currents are drawn from the input rail. Therefore, input
capacitors are required to reduce noise, EMI, and ripple at the input to the LM26001. Capacitors must be
selected that can handle both the maximum ripple RMS current at highest ambient temperature as well as the
maximum input voltage. The equation for calculating the RMS input ripple current is shown below:
(15)
For noise suppression, a ceramic capacitor in the range of 1.0 µF to 10 µF should be placed as close as possible
to the VIN pin.
A larger, high ESR input capacitor should also be used. This capacitor is recommended for damping input
voltage spikes during power-on and for holding up the input voltage during transients. In low input voltage
applications, line transients may fall below the UVLO threshold if there is not enough input capacitance. Both
tantalum and electrolytic type capacitors are suitable for the bulk capacitor. However, large tantalums may not be
available for high input voltages and their working voltage must be derated by at least 2X.
8.2.2.5 Bootstrap
The drive voltage for the internal switch is supplied via the BOOT pin. This pin must be connected to a ceramic
capacitor, Cboot, from the switch node, shown as C4 in the typical application. The LM26001 provides the VDD
voltage internally, so no external diode is needed. A maximum value of 0.1 uF is recommended for Cboot.
Values smaller than 0.01 uF may result in insufficient hold up time for the drive voltage and increased power
dissipation.
During low Vin operation, when the on-time is extended, the bootstrap capacitor is at risk of discharging. If the
Cboot capacitor is discharged below approximately 2.5V, the LM26001 enters a high frequency re-charge mode.
The Cboot cap is re-charged via the LG synchronous FET shown in the block diagram. Switching returns to
normal when the Cboot cap has been recharged.
8.2.2.6 Catch Diode
When the internal switch is off, output current flows through the catch diode. Alternately, when the switch is on,
the diode sees a reverse voltage equal to Vin. Therefore, the important parameters for selecting the catch diode
are peak current and peak inverse voltage. The average current through the diode is given by:
IDAVE = Iload x (1-D) (16)
Where D is the duty cycle, defined as Vout/Vin. The catch diode conducts the largest currents during the lowest
duty cycle. Therefore IDAVE should be calculated assuming maximum input voltage. The diode should be rated to
handle this current continuously. For over-current or short circuit conditions, the catch diode should be rated to
handle peak currents equal to the peak current limit.
The peak inverse voltage rating of the diode must be greater than maximum input voltage.
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