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LT1737CS データシート(PDF) 16 Page - Linear Technology

部品番号 LT1737CS
部品情報  High Power Isolated Flyback Controller
PDF  28 Pages
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メーカー  LINER [Linear Technology]
ホームページ  http://www.linear.com
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LT1737CS データシート(HTML) 16 Page - Linear Technology

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16
LT1737
1737f
this frequency the sense resistor will behave like an
inductor.
Several techniques can be used to tame this potential
parasitic inductance problem. First, any resistor used for
current sensing purposes must be of an inherently non-
inductive construction. Mounting this resistor directly
above an unbroken ground plane and minimizing its
ground side connection will serve to absolutely minimize
parasitic inductance. In the case of low valued sense
resistors, these may be implemented as a parallel combi-
nation of several resistors for the thermal considerations
cited above. The parallel combination will help to lower the
parasitic inductance. Finally, it may be necessary to place
a “pole” between the current sense resistor and the
LT1737 ISENSE pin to undo the action of the inductive zero
(see Figure 5). A value of 51
Ωissuggestedfortheresistor,
while the capacitor is selected empirically for the particular
application and layout. Using good high frequency mea-
surement techniques, the ISENSE pin waveform may be
observed directly with an oscilloscope while the capacitor
value is varied.
APPLICATIO S I FOR ATIO
GATE
PARASITIC
INDUCTANCE
CCOMP
RSENSE
LP
1737 F05
51
PGND
SGND
ISENSE
f =
RSENSE
2
πLP
SENSE RESISTOR ZERO AT:
f =
1
2
π(51Ω)CCOMP
COMPENSATING POLE AT:
CCOMP =
LP
RSENSE(51Ω)
FOR CANCELLATION:
Figure 5
SOFT-START FUNCTION
The LT1737 contains an optional soft-start function that is
enabled by connecting an explicit external capacitor be-
tween the SFST pin and ground. Internal circuitry prevents
the control voltage at the VC pin from exceeding that on the
SFST pin.
The soft-start function is enagaged whenever VCC power
is removed, or as a result of either undervoltage lockout
or thermal (overtemperature) shutdown. The SFST node
is then discharged rapidly to roughly a VBE above ground.
(Remember that the VC pin control node switching
threshold is deliberately set at a VBE plus several hundred
millivolts.) When this condition is removed, a nominal
40
µA current acts to charge up the SFST node towards
roughly 3V. So, for example, a 0.1
µF soft-start capacitor
will place a 0.4V/ms limit on the ramp rate at the VC node.
UVLO PIN FUNCTION
The UVLO pin effects both undervoltage lockout and
shutdown functions. This is accomplished by using differ-
ent voltage thresholds for the two functions—the shut-
down function is at roughly a VBE above ground (0.75V at
25
°C, large temperature variation), while the UVLO func-
tion is at nearly a bandgap voltage (1.25V, fairly stable with
temperature). An external resistor divider between the
input supply and ground can then be used to achieve a
user-programmable undervoltage lockout (see Figure 6a).
An additional feature of this pin is that there is a change in
the input bias current at this pin as a function of the state
of the internal UVLO comparator. As the pin is brought
above the UVLO threshold, the bias current sourced by the
part increases. This positive feedback effects a hysteresis
band for reliable switching action. Note that the size of the
hysteresis is proportional to the Thevenin impedance of
the external UVLO resistor divider network, which makes
it user programmable. As a rough rule of thumb, each 4k
or so of impedance generates about 1% of hysteresis.
(This is based on roughly 1.25V for the threshold and 3
µA
for the bias current shift.)
Even in good quality ground plane layouts, it is common
for the switching node (MOSFET drain) to couple to the
UVLO pin with a stray capacitance of several
thousandths
of a pF. To ensure proper UVLO action, a 100pF capacitor
is recommended from this pin to ground as shown in
Figure 6b. This will typically reduce the coupled noise to
a few millivolts. The UVLO filter capacitor should not be
made much larger than a few hundred pF, however, as the
hysteresis action will become too slow. In cases where
further filtering is required, e.g., to attenuate high speed
supply ripple, the topology in Figure 6c is recommended.
Resistor R1 has been split into two equal parts. This
provides a node for effecting capacitor filtering of high
speed supply ripple, while leaving the UVLO pin node
impedance relatively unchanged at high frequency.



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