7
LT1777
BLOCK DIAGRA
W
V
C
V
BG
LOGIC
FEEDBACK
AMP
SWDR
I
1
V
IN
V
D
V
SW
I
2
1777 BD
R1
V
B
V
BG
R
SENSE
I
SWON
OSC
SYNC
SHDN
V
CC
SGND
FB
BIAS
I
COMP
I
g
m
dV/dt
LIMITER
±dI/dt
LIMITER
Q2
Q1
4
3
12
7
14
13
5
6
10
OUTPUT STAGE SI PLIFIED SCHE ATIC
WW
+
Q3Q2
R1
C1
Q4
Q6
SWITCH ON
SIGNAL
Q1
Q5
R2
V
SW
V
OUT
V
IN
L
SENSE
L
MAIN
R3
NOTE: R3 = R4
R4
1777 SS
V
D
I
1
I
8
LT1777
OPERATIO
U
The LT1777 is a current mode step-down switcher regu-
lator IC designed for low noise operation. The Block
Diagram shows an overall view of the system. The indi-
vidual blocks are straightforward and similar to those
found in traditional designs, including: Internal Bias Regu-
lator, Oscillator, Logic, and Feedback Amplifier. The novel
portion includes a specialized Output Switch section in-
cluding circuits to limit the dI/dt and dV/dt switching rates.
The LT1777 operates much the same as traditional current
mode switchers, the major difference being its specialized
output switch section. Due to space constraints, this
discussion will not reiterate the basics of current mode
switcher/controllers and the “buck” topology. A good
source of information on these topics is Application Note
AN19.
A straightforward output stage is provided by current
source I
1
driving the base of PNP transistor Q2. The
collector of Q2 in turn drives the base of NPN output device
Q1. The considerable base/collector capacitance of PNP
Q2 acts to limit dV/dt rate during switch turn-on. However,
when the switch is to be turned off, the only natural limit
to voltage slew rate would be the collector/base capaci-
tance of Q1 providing drive for the same device. While
dependent upon output load level and Q1’s β, the turn-off
voltage slew rate would be typically much faster than the
turn-on rate. To limit the voltage slew rate on switch turn-
off, an extra function is supplied. This is denoted by the
block labeled “–dV/dt Limiter.”
The details of the –dV/dt Limiter can be seen in the Output
Stage Simplified Schematic. Transistors Q3 and Q4 are
connected in a Darlington configuration whose input is
coupled with small-valued capacitor C1 to the V
IN
supply
rail. The product of negative voltage slew rate times this
capacitor value equals current, and when this current
through emitter/base resistor R1 exceeds a diode drop, Q3
and then Q4 turn on supplying base drive to output device
Q1 to limit –dV/dt rate.
In addition to voltage rates, the current slew rate also
needs to be controlled for reduced noise behavior. This is
provided by the section in the Block Diagram labeled
±dI/dt Limiter.” The details of this circuit can be seen in
the Output Stage Simplified Schematic. Note that an extra,
small-valued inductor, termed the “sense inductor” has
been added to the classic buck topology. As this inductor
is external to the LT1777, its value can be chosen by the
user allowing for optimization on a per application basis.
Operation of the current slew limiter is as follows: The
product of the sense inductor times the dI/dt through it
generates a voltage according to the well known formula
V = (L)(dI/dt). The remainder of the circuit is configured
such that when the voltage across the sense inductor
reaches ±2V
BE
, drive current will be supplied or removed
as necessary to limit current slew rate. The actual sensing
is performed between the output node labeled V
SW
and a
new node labeled V
D
.
In the case of switch turn-on, current drive is provided by
PNP Q2. If the voltage at V
SW
reaches 2V
BE
above that at
V
D
, transistor Q5 turns on and removes a portion of Q2’s
drive from Q1’s base. Similarly for turn-off, as the V
SW
node goes 2V
BE
below V
D
, transistor Q6 then turns on to
drive Q1’s base as needed. The net effect is that of limiting
the switch node dI/dt in both directions at a rate inversely
proportional to the external sense inductor value.
9
LT1777
APPLICATIONS INFORMATION
WUU
U
external sense inductor to set a maximum allowed dI/dt
rate. This attenuates the highest frequency components of
generated B field RFI. Minimal lead length in the path is
also essential to minimize generated RFI.
A second potential source of magnetic RFI is the main
(power) inductor. Fortunately, the natural triangular be-
havior of the current waveform in the main inductor tends
to generate magnetic field energy concentrated in the
fundamental and lower harmonics. Nevertheless, the rela-
tively intense magnetic field present in the main inductor
can cause coupling problems, especially if the main induc-
tor is of an open construction type. So called rod or barrel
inductors may be the physically smallest and most effec-
tive types, but their magnetic field extends far beyond the
device itself. Closed type inductors, toroids for example,
contain the magnetic field nearly completely. These are
generally preferred for low noise behavior.
The sense inductor sees a much more rapid current slew
rate than does the main inductor. However the sense
inductor is physically smaller and of much lower induc-
tance than the main inductor. These factors tend to reduce
its propensity to generate magnetic interference prob-
lems. Nevertheless, more sensitive applications can opt
for a closed type magnetic construction on the sense
inductor.
Basics of Low Noise Operation
Switching power supply circuits are often preferred over
linear topologies for their improved efficiency (P
OUT
/ P
IN
).
However, their typically rapid voltage and current slew
rates often cause “radio frequency” interference prob-
lems, commonly referred to as “RFI”. The LT1777 is
designed to provide a less aggressive voltage slew rate
and a user-programmable current slew rate to eliminate
the highest frequency harmonics of RFI emissions. These
highest frequency components are typically the most
troublesome. Optimum behavior is obtained by a combi-
nation of proper circuit design, which includes passive
component selection, and proper printed circuit board
layout technique.
There are two types of RFI emissions, i.e.,
conducted
and
radiated
. Conducted interference travels directly through
“wires”, as opposed to radiated interference, which travels
through the air. Conducted RFI can be created by a
switching power supply at its input voltage supply node,
its output node(s) or both. It is typically caused by pulsatile
current flow through the residual high frequency imped-
ance (ESR) of bypass capacitors.
Radiated interference can be of two types: electric (E field)
or magnetic (B field). E field interference is caused by stray
capacitance coupling of the node(s) which swing rapidly
over a large voltage excursion. In the LT1777, this in-
cludes the V
SW
and V
D
nodes. E field radiation is kept low
by minimizing the length and area of all traces connected
to these nodes. A ground plane should always be used
under the switcher circuitry to prevent interplane cou-
pling. Although these nodes swing over a voltage range
roughly equal to the input voltage, the limited dV/dt rate of
the LT1777 reduces the highest frequency components of
the generated E field RFI.
B field RFI is simply coupling of high frequency magnetic
fields generated by the offending circuitry. High frequency
magnetic fields are created by relatively rapidly changing
currents, and the high speed current switching path in the
LT1777 is shown schematically in Figure 1. This includes
the input capacitor, output switch, sense inductor and
output diode. Normal switching supply operation requires
a rapid switching of current back and forth between the
output switch and output diode. The LT1777 uses the
+
+
LT1777
V
IN
C1
D1
V
OUT
1777 F01
C2
L
SENSE
L
MAIN
Figure 1. High Speed Current Switching Paths
Selecting Sense Inductor
The LT1777 uses an external sense inductor to set a
theoretical limit for current ramp rate according to the
formula:
Max dI dt
V
L
BE
SENSE
/ =
2

LT1777IS#PBF

Mfr. #:
Manufacturer:
Analog Devices / Linear Technology
Description:
Switching Voltage Regulators L N Buck Sw Reg
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