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LT3439 Datasheet(PDF) 7 Page - Linear Technology

Part # LT3439
Description  Slew Rate Controlled Ultralow Noise1A Isolated DC/DC Transformer Driver
PDF  12 Pages
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Manufacturer  LINER [Linear Technology]
Direct Link  http://www.linear.com
Logo LINER - Linear Technology

LT3439 Datasheet(HTML) 7 Page - Linear Technology

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LT3439
sn3439 3439fs
Oscillator SYNC
The oscillator can be synchronized to an external clock.
Set the RC timing components for an oscillator frequency
10% below the desired sync frequency.
It is recommended that the SYNC pin be driven with a
square wave that has an amplitude greater than 2V, a pulse
width greater than 1
µs and a rise time less than 500ns. The
rising edge of the sync waveform triggers the change in
the state of the outputs.
Slew Rate Setting
Setting the LT3439 maximum slew rate is easy. The
external resistor to ground on the RSL pin sets the maxi-
mum slew rate. To determine the maximum slew rate
connect a 50k resistor pot with a 3.4k series resistance to
the RSL pin. Start at the lowest resistance setting and
increase the pot until the noise level meets your require-
ments. Note that slower slewing waveforms will lower the
power supply efficiency. Consult Linear Technology Appli-
cation Note 70, “A Monolithic Switching Regulator with
100
µV Output Noise” for recommended noise measure-
ment techniques.
Shutdown
The SHDN pin is used to shut down the part. Grounding
this pin will disable all internal circuitry.
Increasing the SHDN voltage above the turn-on threshold,
approximately 1.3V, will enable the part. At the turn-on
threshold approximately 20
µA of current is sourced out of
the pin. This current, in conjunction with the Thevenin
resistance on the pin, sets up the amount of hysteresis.
This allows the user to set the turn-on voltage of the supply
and the start-up hysteresis with a resistor divider. The
hysteresis can be used to prevent the part from shutting
down due to input voltage sag from an initial high current
draw. When the SHDN pin is greater than 2.1V, the
hysteresis current is reduced to zero.
In addition to the current hysteresis, there is also approxi-
mately 35mV of voltage hysteresis on the SHDN pin.
If a resistor divider is used to set the turn on threshold the
resistors are determined by the following equations:
APPLICATIO S I FOR ATIO
V
RR
R
V
ON
AB
B
SHDN
=
+


•
SHDN
RA
RB
3439 AI01
VIN
VON is the input voltage at which the supply will turn on and
VSHDN is the SHDN pin turn-on threshold, typically 1.3V.
VR
V
RR
I
HYST
A
SHDN
AB
SHDN
=
∆
+


•
||
VHYST is the actual hysteresis voltage seen at the input
voltage. ISHDN is the current hysteresis sourced by the IC
at the turn-on threshold, typically 20
µA. ∆VSHDN is the
voltage hysteresis seen at the SHDN pin at the turn-on
threshold, typically 35mV.
The resistors can be calculated as follows:
R
VV
V
V
IV
R
VV
V
V
IV
V
A
HYST
SHDN
ON
SHDN
SHDN
SHDN
B
HYST
SHDN
ON
SHDN
SHDN
ON
SHDN
=
∆
()
=
∆
()
()
•–
•
•
•–
•
•–
For example if the turn-on voltage was to be set at 5V with
0.5V of hysteresis:
R
VV
V
mV
AV
k
R
VV
V
mV
AV
V
k
A
B
= ()
µ
=
= ()
µ
()
=
05
13
5
35
20
1 3
18 27
05
13
5
35
20
5
1 3
642
.• .–
•
•.
.
.• .–
•
•– .
.
The nearest 1% values would be 18.2k and 6.49k.
A resistor in series with the SHDN pin could further change
hysteresis without changing the turn-on voltage.
Thermal Considerations
Decreasing the noise by lowering the slew rate of the
output switches does not come for free. Lower slew rates



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