MAX8622
cy and lower ripple currents for the same output power
as compared to DCM operation. The capacitive switch-
ing losses in the switch are minimal at the boundary of
DCM and CCM operation. The primary inductance for
the transformer is therefore estimated based on the
assumption that the MAX8622 is operating close to this
boundary for highest efficiency and minimum charge
time.
The MAX8622 has an on-time limit (tON(MAX)) of typical-
ly 25µs. Assuming the default current limit (ILIMIT) of
1.6A, the maximum value of primary inductance for a
1.8V minimum input and a 1.6A primary current limit is
given by:
The boundary of DCM/CCM operation is determined by
monitoring the secondary valley current. The secondary
current-sensing circuit in the MAX8622 has a blanking
time of about 150ns. This implies a minimum off-time
tOFF(MIN) of 250ns for the MAX8622 to have adequate
time to sense the secondary valley current. Since the
minimum discharge time occurs at the target output
voltage VOUT(MAX), the minimum secondary induc-
tance LSEC(MIN) is given by:
where N is the transformer turns ratio. This in turn implies
a minimum primary inductance LPRI(MIN) given by:
For a typical turns ratio of 15 (see the Transformer Turns
Ratio section), the LPRI(MIN) is calculated to be 3µH.
Choose a value between LPRI(MIN) and LPRI(MAX)
based on other considerations for the leakage induc-
tance and the transformer capacitance. A transformer
with a primary inductance of 6µH is recommended for
most applications.
Leakage Inductance
A particularly important transformer parameter is leak-
age inductance. In a practical transformer construction,
all windings cannot be equally well-coupled to the core
because of physical separation. If the primary induc-
tance is high, the transformer may need multiple wind-
ings for the primary. A small amount of energy is stored
between the windings and this energy is represented
as leakage inductance. If the primary inductance is too
small, the primary windings may not cover the width of
the core and result in poor coupling to the secondary.
This also increases the leakage inductance.
Leakage inductance does not participate in the primary
to secondary energy transfer. Since the leakage induc-
tance does not find a path for the current built up dur-
ing the switch on-time, it results in voltage spikes and
ringing at the drain of the MAX8622 power switch (LX),
when it turns off. The MAX8622 internal switch is
designed to be robust to withstand these voltage
spikes; however, voltage overshoot should be mini-
mized because it reduces total efficiency. Leakage
inductance also delays the transfer of power from input
to output causing an increase in charge time.
In addition, transformer secondary leakage inductance
may couple with the reverse recovery current of the
output rectifier diode to cause ringing when the diode
turns off. The transformer secondary leakage induc-
tance and the capacitance of the rectifier determine
this resonant frequency. There is typically very little loss
in the resonant circuit, so this network can generate
many cycles of ringing after the spike. The ringing can
therefore affect the peak primary current-sense signal
used by the MAX8622. The transformer secondary
leakage inductance is a function of the primary leakage
inductance.
Care should be taken during transformer design while
using techniques such as sandwiching the secondary
between two primary windings to minimize leakage
inductance. This can cause high winding-to-winding
capacitance, reduce the efficiency of the circuit, and
increase the charge time.
Transformer Secondary Capacitance
The total capacitance of the secondary should be mini-
mized for both efficient and proper operation. Since the
secondary of the transformer undergoes large voltage
swings, capacitance on the secondary is a significant
detriment to efficiency. This capacitance is reflected on
the primary as an effective capacitance proportional to
the square of the transformer turns ratio. It therefore
dominates the resulting capacitance on the primary.
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