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LT1725
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Output Impedance Error
An additional error source is caused by transformer sec-
ondary current flow through the real life nonzero imped-
ances of the output rectifier, transformer secondary and
output capacitor. Because the secondary current only
flows during the off portion of the duty cycle, the effective
output impedance equals the “DC” lumped secondary
impedance times the inverse of the off duty cycle. If the
output load current remains relatively constant, or, in less
critical applications, the error may be judged acceptable
and the feedback resistor divider ratio adjusted for nomi-
nal expected error. In more demanding applications, out-
put impedance error may be minimized by the use of the
load compensation function (see Load Compensation).
MINIMUM LOAD CONSIDERATIONS
The LT1725 generally provides better low load perfor-
mance than previous generation switcher/controllers uti-
lizing indirect output voltage sensing techniques.
Specifically, it contains circuitry to detect flyback pulse
“collapse,” thereby supporting operation well into discon-
tinuous mode. Nevertheless, there still remain constraints
to ultimate low load operation. These relate to the mini-
mum switch on time and the minimum enable time.
Discontinuous mode operation will be assumed in the
following theoretical derivations.
As outlined in the Operation section, the LT1725 utilizes a
minimum output switch on time, t
ON
. This value can be
combined with expected V
IN
and switching frequency to
yield an expression for minimum delivered power.
Minimum Power
f
L
Vt
VI
PRI
IN ON
OUT OUT
=
()
=
1
2
2
This expression then yields a minimum output current
constraint:
I
f
LV
Vt
OUT MIN
PRI OUT
IN ON()
=
()
1
2
2
where
f = switching frequency
L
PRI
= transformer primary side inductance
V
IN
= input voltage
V
OUT
= output voltage
t
ON
= output switch minimum on time
An additional constraint has to do with the minimum
enable time. The LT1725 derives its output voltage infor-
mation from the flyback pulse. If the internal minimum
enable time pulse extends beyond the flyback pulse, loss
of regulation will occur. The onset of this condition can be
determined by setting the width of the flyback pulse equal
to the sum of the flyback enable delay, t
ED
, plus the
minimum enable time, t
EN
. Minimum power delivered to
the load is then:
Minimum Power
f
L
Vtt
VI
SEC
OUT EN ED
OUT OUT
=
+
()
[]
=
1
2
2
Which yields a minimum output constraint:
I
fV
L
tt
OUT MIN
OUT
SEC
ED EN()
=
+
()
1
2
2
where
f = switching frequency
L
SEC
= transformer secondary side inductance
V
OUT
= output voltage
t
ED
= enable delay time
t
EN
= minimum enable time
Note that generally, depending on the particulars of input
and output voltages and transformer inductance, one of
the above constraints will prove more restrictive. In other
words, the minimum load current in a particular applica-
tion will be either “output switch minimum on time”
constrained, or “minimum flyback pulse time” constrained.
(A final note—L
PRI
and L
SEC
refer to transformer induc-
tance as seen from the primary or secondary side respec-
tively. This general treatment allows these expressions to
be used when the transformer turns ratio is nonunity.)
APPLICATIO S I FOR ATIO
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LT1725
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APPLICATIO S I FOR ATIO
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MAXIMUM LOAD/SHORT-CIRCUIT CONSIDERATIONS
The LT1725 is a current mode controller. It uses the V
C
node voltage as an input to a current comparator which
turns off the output switch on a cycle-by-cycle basis as
this peak current is reached. The internal clamp on the V
C
node, nominally 2.5V, then acts as an output switch peak
current limit.
This 2.5V at the V
C
pin corresponds to a value of 250mV
at the I
SENSE
pin, when the (ON) switch duty cycle is less
than 40%. For a duty cycle above 40%, the internal slope
compensation mechanism lowers the effective I
SENSE
voltage limit. For example, at a duty cycle of 80%, the
nominal I
SENSE
voltage limit is 220mV. This action be-
comes the switch current limit specification. Maximum
available output power is then determined by the switch
current limit, which is somewhat duty cycle dependent
due to internal slope compensation action.
Overcurrent conditions are handled by the same mecha-
nism. The output switch turns on, the peak current is
quickly reached and the switch is turned off. Because the
output switch is only on for a small fraction of the available
period, power dissipation is controlled.
Loss of current limit is possible under certain conditions.
Remember that the LT1725 normally exhibits a minimum
switch on time, irrespective of current trip point. If the duty
cycle exhibited by this minimum on time is greater than the
ratio of secondary winding voltage (referred-to-primary)
divided by input voltage, then peak current will not be
controlled at the nominal value, and will cycle-by-cycle
ratchet up to some higher level. Expressed mathemati-
cally, the requirement to maintain short-circuit control is:
tf
VI R
VN
ON
F SC SEC
IN SP
<
+
()
where
t
ON
= output switch minimum on time
f = switching frequency
I
SC
= short-circuit output current
V
F
= output diode forward voltage at I
SC
R
SEC
= resistance of transformer secondary
V
IN
= input voltage
N
SP
= secondary-to-primary turns ratio ( N
SEC
/N
PRI
)
Trouble is typically only encountered in applications with
a relatively high product of input voltage times secondary-
to-primary turns ratio and/or a relatively long minimum
switch on time. (Additionally, several real world effects such
as transformer leakage inductance, AC winding losses, and
output switch voltage drop combine to make this simple
theoretical calculation a conservative estimate.)
THERMAL CONSIDERATIONS
Care should be taken to ensure that the worst-case input
voltage condition does not cause excessive die tempera-
tures. The 16-lead SO package is rated at 100°C/W, and
the 16-lead GN at 110°C/W.
Average supply current is simply the sum of quiescent
current given in the specifications section plus gate drive
current. Gate drive current can be computed as:
I
G
= f • Q
G
where
Q
G
= total gate charge
f = switching frequency
(Note: Total gate charge is more complicated than C
GS
• V
G
as it is frequently dominated by Miller effect of the C
GD
.
Furthermore, both capacitances are nonlinear in practice.
Fortunately, most MOSFET data sheets provide figures
and graphs which yield the total gate charge directly per
operating conditions.) Nearly all gate drive power is dissi-
pated in the IC, except for a small amount in the external
gate series resistor, so total IC dissipation may be com-
puted as:
P
D(TOTAL)
= V
CC
(I
Q
+ • f • Q
G
), where
I
Q
= quiescent current (from specifications)
Q
G
= total gate charge
f = switching frequency
V
CC
= LT1725 supply voltage
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LT1725
1725fa
SWITCH NODE CONSIDERATIONS
For maximum efficiency, gate drive rise and fall times are
made as short as practical. To prevent radiation and high
frequency resonance problems, proper layout of the
components connected to the IC is essential, especially
the power paths (primary and secondary). B field (mag-
netic) radiation is minimized by keeping MOSFET leads,
output diode, and output bypass capacitor leads as short
as possible. E field radiation is kept low by minimizing the
length and area of all similar traces. A ground plane
should always be used under the switcher circuitry to
prevent interplane coupling.
The high speed switching current paths are shown sche-
matically in Figure 8. Minimum lead length in these paths
are essential to ensure clean switching and minimal EMI.
The path containing the input capacitor, transformer pri-
mary and MOSFET, and the path containing the trans-
former secondary, output diode and output capacitor
contain “nanosecond” rise and fall times. Keep these
paths as short as possible.
APPLICATIO S I FOR ATIO
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GATE DRIVE RESISTOR CONSIDERATIONS
The gate drive circuitry internal to the LT1725 has been
designed to have as low an output impedance as practi-
cally possible—only a few ohms. A strong L/C resonance
is potentially presented by the inductance of the path
leading to the gate of the power MOSFET and its overall
gate capacitance. For this reason the path from the GATE
package pin to the physical MOSFET gate should be kept
as short as possible, and good layout/ground plane prac-
tice used to minimize the parasitic inductance.
An explicit series gate drive resistor may be useful in some
applications to damp out this potential L/C resonance
(typically tens of MHz). A minimum value of perhaps
several ohms is suggested, and higher values (typically a
few tens of ohms) will offer increased damping. However,
as this resistor value becomes too large, gate voltage rise
time will increase to unacceptable levels, and efficiency
will suffer due to the sluggish switching action.
Figure 8. High Speed Current Switching Paths
+
+
PGND
GATE
1725 F08
GATE
DISCHARGE
PATH
PRIMARY
POWER
PATH
SECONDARY
POWER
PATH
V
CC
V
CC
V
IN
+

LT1725IGN#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators General Purpose Iso Fly Cntr
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