LTC3622/
LTC3622-2/LTC3622-23/5
16
Rev D
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resistance of COUT. ΔILOAD also begins to charge or dis-
charge COUT generating a feedback error signal used by the
regulator to return VOUT to its steady state value. During
this recovery time, VOUT can be monitored for overshoot
or ringing that indicates a stability problem.
The initial output voltage step may not be within the band-
width of the feedback loop, so the standard second order
overshoot/DC ratio cannot be used to determine phase
margin. In addition, a feedforward capacitor can be added
to improve the high frequency response, shown in Figure 2.
Capacitor CFF provides phase lead by creating a high fre-
quency zero with R2, which improves the phase margin.
The output voltage settling behavior is related to the stabil-
ity of the closed-loop system and demonstrates the actual
overall supply performance. For a detailed explanation of
optimizing the compensation components, including a
review of control loop theory, refer to Application Note 76.
In some applications, a more severe transient can be caused
by switching in loads with large (>1µF) input capacitors.
The discharge input capacitors are effectively put in parallel
with COUT, causing a rapid drop in VOUT. No regulator can
deliver enough current to prevent this problem if the switch
connecting to load has low resistance and is driven quickly.
The solution is to limit the turn-on speed of the load switch
driver. A Hot Swap controller is designed specifically for
this purpose and usually incorporates current limiting,
short-circuit protection and soft-starting.
Efficiency Considerations
The percent efficiency of a switching regulator is equal to
the output power divided by the input power times 100%.
It is often useful to analyze individual losses to determine
what is limiting the efficiency and which change would
produce the most improvement. Percent efficiency can
be expressed as:
% Efficiency = 100% – (L1 + L2 + L3 + …)
where L1, L2 etc. are the individual losses as a percent-
age of input power. Although all dissipative elements in
the circuit produce losses, three main sources usually
account for most of the losses in LTC3622 circuit: 1) I2R
losses, 2) switching and biasing losses, 3) other losses.
APPLICATIONS INFORMATION
1. I2R losses are calculated from the DC resistances of the
internal switches, RSW, and external inductor, RL. In
continuous mode, the average output current flows
through inductor L but is “chopped” between the
internal top and bottom power MOSFETs. Thus, the
series resistance looking into the SW pin is a function
of both top and bottom MOSFET RDS(ON) and the duty
cycle (DC) as follows:
RSW =(RDS(ON)TOP)(DC)+(RDS(ON)BOT)(1 – DC)
The RDS(ON) for both the top and bottom MOSFETs
can be obtained from the Typical Performance Char-
acteristics curves. Thus to obtain I2R losses:
I2R Losses = IOUT2(RSW + RL)
2. The switching current is the sum of the MOSFET driver
and control currents. The power MOSFET driver cur-
rent results from switching the gate capacitance of the
power MOSFETs. Each time a power MOSFET gate is
switched from low to high to low again, a packet of
charge dQ moves from VIN to ground. The resulting
dQ/dt is a current out of VIN that is typically much
larger than the DC control bias current. In continuous
mode, IGATECHG = fOSC(QT + QB), where QT and QB are
the gate charges of the internal top and bottom power
MOSFETs and fOSC is the switching frequency. The
power loss is thus:
Switching Loss = IGATECHG • VIN
The gate charge loss is proportional to VIN and fOSC
and thus their effects will be more pronounced at
higher supply voltages and higher frequencies.
3. Other “hidden” losses such as transition loss and cop-
per trace and internal load resistances can account
for additional efficiency degradations in the overall
power system. It is very important to include these
“system” level losses in the design of a system. Transi-
tion loss arises from the brief amount of time the top
power MOSFET spends in the saturated region during
switch node transitions. The LTC3622 internal power
devices switch quickly enough that these loses are not
significant compared to other sources. These losses
plus other losses, including diode conduction losses
during dead time and inductor core losses, generally
account for less than 2% total additional loss.