LT1777C [Linear]

Low Noise Step-Down Switching Regulator; 低噪声降压型开关稳压器
LT1777C
型号: LT1777C
厂家: Linear    Linear
描述:

Low Noise Step-Down Switching Regulator
低噪声降压型开关稳压器

稳压器 开关
文件: 总24页 (文件大小:272K)
中文:  中文翻译
下载:  下载PDF数据表文档文件
LT1777  
Low Noise Step-Down  
Switching Regulator  
U
FEATURES  
DESCRIPTIO  
TheLT®1777isaBuck(step-down)regulatordesignedfor  
noise sensitive applications. It contains a dI/dt limiting  
circuit programmed via a small external inductor in the  
switchingpath.Internalcircuitryalsogeneratescontrolled  
dV/dt ramp rates.  
Programmable dI/dt Limit  
Internally Limited dV/dt  
High Input Voltage: 48V Max  
700mA Peak Switch Rating  
True Current Mode Control  
100kHz Fixed Operating Frequency  
The monolithic die includes all oscillator, control and  
protection circuitry. The part can accept operating input  
voltages as high as 48V, and contains an output switch  
rated at 700mA peak current. Current mode control offers  
excellent dynamic input supply rejection and short-circuit  
protection. The internal control circuitry is normally pow-  
ered via the VCC pin, thereby minimizing power drawn  
directly from the VIN supply (see Applications Informa-  
tion). The fused-lead SO16 package and 100kHz switch-  
ing frequency allow for minimal PC board area  
Synchronizable to 250kHz  
Low Supply Current in Shutdown: 30µA  
Low Thermal Resistance 16-Pin SO Package  
U
APPLICATIO S  
Automotive Cellular and GPS Receivers  
Telecom Power Supplies  
Industrial Instrument Power Supplies  
requirements.  
, LTC and LT are registered trademarks of Linear Technology Corporation.  
U
TYPICAL APPLICATIO  
Low Noise 5V Step-Down Supply  
VSW Switching Waveforms  
V
IN  
24V  
10  
+
39µF  
63V  
V
IN  
3
4
SHDN  
LT1777  
SYNC  
V
CC  
100pF  
VSW  
VOLTAGE  
10V/DIV  
1µH*  
220µH  
V
OUT  
12  
14  
6
V
5V  
SW  
5
400mA  
+
V
V
D
C
100µF  
10V  
36.5k  
1%  
13  
MBRS1100  
FB  
100pF 12k  
2200pF  
SGND  
VSW  
CURRENT  
200mA/DIV  
7
12.1k  
1%  
1777 TA01  
*PROGRAMS dI/dT  
1777 TA02  
500ns/DIV  
1
LT1777  
W W  
U W  
W
U
/O  
ABSOLUTE MAXIMUM RATINGS  
PACKAGE RDER I FOR ATIO  
(Note 1)  
Supply Voltage ....................................................... 48V  
Switch Voltage (VIN – VSW) (Note 4) ...................... 51V  
SHDN, SYNC Pin Voltage.......................................... 7V  
VCC Pin Voltage ...................................................... 30V  
FB Pin Voltage ........................................................ 3.0V  
Operating Junction Temperature Range  
LT1777C............................................... 0°C to 125°C  
LT1777I ........................................... 40°C to 125°C  
Storage Temperature Range ................ 65°C to 150°C  
Lead Temperature (Soldering, 10 sec)................. 300°C  
ORDER PART  
TOP VIEW  
NUMBER  
GND*  
NC  
1
2
3
4
5
6
7
8
16  
15  
14  
13  
12  
11  
10  
9
GND*  
NC  
LT1777CS  
LT1777IS  
SHDN  
V
C
V
CC  
FB  
V
D
SYNC  
NC  
V
SW  
SGND  
GND*  
V
IN  
*FOUR CORNER PINS ARE  
FUSED TO INTERNAL DIE  
ATTACH PADDLE FOR HEAT  
SINKING. CONNECT THESE  
FOUR PINS TO EXPANDED PC  
LANDS FOR PROPER HEAT  
SINKING.  
GND*  
S PACKAGE  
16-LEAD PLASTIC SO  
TJMAX = 125°C, θJA = 50°C/W*  
Consult factory for Military grade parts.  
ELECTRICAL CHARACTERISTICS  
The denotes specifications which apply over the full operating temperature range, otherwise specifications are at TJ = 25°C.  
VIN = 24V, VSW Open, VCC = 5V, VC = 1.4V unless otherwise noted.  
SYMBOL  
PARAMETER  
CONDITIONS  
MIN  
TYP  
MAX  
UNITS  
Power Supplies  
V
Minimum Input Voltage  
6.7  
620  
2.5  
7.0  
7.4  
V
V
IN(MIN)  
I
I
V
V
V
Supply Current  
Supply Current  
Dropout Voltage  
V = 0V  
800  
900  
µA  
µA  
VIN  
IN  
C
V = 0V  
C
3.5  
4.5  
mA  
mA  
VCC  
CC  
V
(Note 2)  
2.8  
30  
3.1  
V
VCC  
CC  
Shutdown Mode I  
V
= 0V  
SHDN  
50  
75  
µA  
µA  
VIN  
Feedback Amplifier  
V
Reference Voltage  
1.225  
1.215  
1.240  
1.255  
1.265  
V
V
REF  
I
FB Pin Input Bias Current  
600  
650  
1500  
nA  
IN  
g
Feedback Amplifier Transconductance  
I = ±10µA  
400  
200  
1000  
1500  
µmho  
µmho  
m
C
I
, I  
Feedback Amplifier Source or Sink Current  
60  
45  
100  
2.0  
170  
220  
µA  
µA  
SRC SNK  
V
Feedback Amplifier Clamp Voltage  
Reference Voltage Line Regulation  
Voltage Gain  
V
%/V  
V/V  
CL  
12V V 48V  
0.01  
IN  
200  
600  
2
LT1777  
ELECTRICAL CHARACTERISTICS  
The denotes specifications which apply over the full operating temperature range, otherwise specifications are at TJ = 25°C.  
IN = 24V, VSW Open, VCC = 5V, VC = 1.4V unless otherwise noted.  
V
SYMBOL PARAMETER CONDITIONS  
Output Switch  
MIN  
TYP  
MAX  
UNITS  
R
Output Switch On Voltage  
Switch Current Limit  
I
= 0.5A  
SW  
1.0  
0.70  
1.3  
1.5  
1.0  
V
A
ON  
I
(Note 3)  
0.55  
0.6  
LIM  
Output dl/dt Sense Voltage  
V
V
2.0  
Current Amplifier  
Control Pin Threshold  
Duty Cycle = 0%  
0.9  
1.1  
2
1.25  
V
Control Voltage to Switch Transconductance  
A/V  
Timing  
f
Switching Frequency  
90  
85  
100  
90  
110  
115  
kHz  
kHz  
Maximum Switch Duty Cycle  
85  
%
Sync Function  
Minimum Sync Amplitude  
1.5  
40  
2.2  
V
kHz  
kΩ  
Synchronization Range  
SYNC Pin Input R  
130  
250  
SHDN Pin Function  
V
Shutdown Mode Threshold  
0.5  
V
V
SHDN  
0.2  
0.8  
Upper Lockout Threshold  
Lower Lockout Threshold  
Shutdown Pin Current  
Switching Action On  
Switching Action Off  
1.260  
1.245  
V
V
I
V
V
= 0V  
= 1.25V  
12  
2.5  
20  
10  
µA  
µA  
SHDN  
SHDN  
SHDN  
Note 1: Absolute Maximum Ratings are those values beyond which the life  
of a device may be impaired.  
Note 4: During normal operation the V pin may fly as much as 3V  
below ground. However, the LT1777 may not be used in an inverting  
DC/DC configuration.  
SW  
Note 2: Control circuitry powered from V  
.
CC  
Note 3: Switch current limit is DC trimmed and tested in production.  
Inductor dI/dt rate will cause a somewhat higher current limit in actual  
application.  
3
LT1777  
U W  
TYPICAL PERFOR A CE CHARACTERISTICS  
Minimum Input Voltage  
vs Temperature  
Switch On Voltage  
vs Switch Current  
7.4  
7.2  
7.0  
6.8  
6.6  
6.4  
6.2  
6.0  
1.50  
1.25  
1.00  
0.75  
0.50  
0.25  
0
25°C  
55°C  
125°C  
50  
TEMPERATURE (°C)  
100 125  
–50 –25  
0
25  
75  
400  
SWITCH CURRENT (mA)  
600 700  
0
100 200 300  
500  
1777 G01  
1777 G02  
Switch Current Limit  
vs Duty Cycle  
SHDN Pin Shutdown Threshold  
vs Temperature  
1000  
800  
600  
400  
200  
0
900  
800  
700  
600  
500  
400  
300  
200  
T
= 25°C  
A
0
10 20 30 40 50 60 70 80 90 100  
50  
TEMPERATURE (°C)  
100 125  
–50 –25  
0
25  
75  
DUTY CYCLE (%)  
1777 G03  
1777 G04  
SHDN Pin Lockout Thresholds  
vs Temperature  
SHDN Pin Current vs Voltage  
5
0
1.30  
1.28  
1.26  
1.24  
1.22  
1.20  
UPPER THRESHOLD  
LOWER THRESHOLD  
–5  
–10  
–15  
–20  
25°C  
125°C  
–55°C  
0
1
2
3
4
5
–50 –25  
0
25  
50  
TEMPERATURE (°C)  
75  
100 125  
SHDN PIN VOLTAGE (V)  
1777 G05  
1777 G06  
4
LT1777  
U W  
TYPICAL PERFOR A CE CHARACTERISTICS  
Switching Frequency  
vs Temperature  
Minimum Synchronization  
Voltage vs Temperature  
106  
104  
102  
100  
98  
2.25  
2.00  
1.75  
1.50  
1.25  
1.00  
0.75  
96  
94  
50  
TEMPERATURE (°C)  
100 125  
50  
TEMPERATURE (°C)  
100 125  
–50 –25  
0
25  
75  
–50 –25  
0
25  
75  
1777 G07  
1777 G08  
Output dI/dt Sense Voltage  
vs Temperature  
VC Pin Switching Threshold,  
Clamp Voltage vs Temperature  
2.0  
1.8  
1.6  
1.4  
1.2  
1.0  
0.8  
0.6  
2.2  
2.0  
1.8  
1.6  
1.4  
1.2  
1.0  
0.8  
CLAMP  
VOLTAGE  
SWITCHING  
THRESHOLD  
50  
TEMPERATURE (°C)  
100 125  
–50 –25  
0
25  
50  
75  
100 125  
–50 –25  
0
25  
75  
TEMPERATURE (°C)  
1777 G09  
1777 G10  
Error Amplifier Transconductance  
vs Temperature  
Feedback Amplifier Output  
Current vs FB Pin Voltage  
100  
50  
750  
700  
650  
600  
550  
500  
450  
400  
25°C  
125°C  
–55°C  
0
–50  
–100  
–150  
1.1  
1.2  
1.3  
1.4  
1.5  
–50 –25  
0
25  
50  
TEMPERATURE (°C)  
75  
100 125  
1.0  
FB PIN VOLTAGE (V)  
1777 G11  
1777 G12  
5
LT1777  
U
U
U
PIN FUNCTIONS  
GND (Pins 1, 8, 9, 16): These corner package pins are  
mechanically connected to the die paddle and thus aid in  
conducting away internally generated heat. As these are  
electrically connected to the die substrate, they must be  
held at ground potential. A direct connection to the local  
ground plane is recommended.  
removed or supplied accordingly to limit dI/dt (see Appli-  
cations Information).  
V
SW (Pin 6): This is the emitter node of the output switch  
and has large currents flowing through it. Keep the traces  
to the switching components as short as possible to  
minimize electromagnetic radiation and voltage spikes.  
NC (Pins 2, 11, 15): Package Pins 2, 11 and 15 are  
unconnected.  
SGND (Pin 7): This is the device signal ground pin. The  
internal reference and feedback amplifier are referred to it.  
Keep the ground path connection to the FB divider and the  
VC compensation capacitor free of large ground currents.  
SHDN (Pin 3): When pulled below the shutdown mode  
threshold, nominally 0.5V, this pin turns off the regulator  
and reduces VIN input current to a few tens of microam-  
peres (shutdown mode).  
VIN (Pin 10): This is the high voltage supply pin for the  
outputswitch.Italsosuppliespowertotheinternalcontrol  
circuitry during start-up conditions or if the VCC pin is left  
open. A high quality bypass capacitor which meets the  
input ripple current requirements is needed here (see  
Applications Information).  
Whenthispinisheldabovetheshutdownmodethreshold,  
but below the lockout threshold, the part will be opera-  
tional with the exception that output switching action will  
be inhibited (lockout mode). A user-adjustable undervolt-  
age lockout can be implemented by driving this pin from  
an external resistor divider to VIN. This action is logically  
“ANDed” with the internal UVLO, nominally set at 6.7V,  
such that minimum VIN can be increased above 6.7V, but  
not decreased (see Applications Information).  
SYNC (Pin 12): Pin to synchronize internal oscillator to  
external frequency reference. It is directly logic compat-  
ible and can be driven with any signal between 10% and  
90% duty cycle. The sync function is internally disabled if  
the FB pin voltage is low enough to cause oscillator  
slowdown. If unused, this pin should be grounded.  
If unused, this pin should be left open. However, the high  
impedance nature of this pin renders it susceptible to  
coupling from the VSW node, so a small capacitor to  
ground, typically 100pF or so is recommended when the  
pin is left open.  
FB (Pin 13): This is the inverting input to the feedback  
amplifier. The noninverting input of this amplifier is inter-  
nally tied to the 1.24V reference. This pin also slows down  
the frequency of the internal oscillator when its voltage is  
abnormally low, e.g. 2/3 of normal or less. This feature  
helps maintain proper short-circuit protection. Coupling  
from high speed noise to this pin can cause irregular  
operation. (See Switch Node Considerations section.)  
VCC: (Pin 4): Pin to power the internal control circuitry  
from the switching supply output. Proper use of this pin  
enhances overall power supply efficiency. During start-up  
conditions, internal control circuitry is powered directly  
from VIN. If the output capacitor is located more than an  
inch from the VCC pin, a separate 0.1µF bypass capacitor  
to ground may be required right at the pin.  
VC (Pin 14): This is the control voltage pin which is the  
output of the feedback amplifier and the input of the  
currentcomparator.Frequencycompensationoftheover-  
all loop is effected by placing a capacitor (or in most cases  
a series R/C combination) between this node and ground.  
Coupling from high speed noise to this pin can cause  
irregular operation. (See Switch Node Considerations  
section.)  
VD (Pin 5): This pin is used in conjunction with a small  
external sense inductor to limit power path dI/dt. The  
senseinductorisplacedbetweentheVSW outputnodeand  
the cathode of the freewheeling (power) diode, and the VD  
pin is connected to the diode. As the voltage across the  
inductor reaches ±2VBE, drive to the output transistor is  
6
LT1777  
W
BLOCK DIAGRA  
V
V
IN  
CC  
4
10  
R1  
R
SENSE  
V
B
SHDN  
3
BIAS  
V
BG  
dV/dt  
LIMITER  
I
COMP  
SWDR  
SWON  
Q2  
SYNC  
12  
OSC  
LOGIC  
Q1  
SGND  
7
V
SW  
6
5
V
C
I
1
14  
I
FEEDBACK  
AMP  
FB  
13  
V
D
±dI/dt  
LIMITER  
g
m
I
2
I
V
BG  
1777 BD  
W
W
OUTPUT STAGE SI PLIFIED SCHE ATIC  
V
IN  
C1  
Q2  
Q3  
R1  
Q4  
R2  
Q6  
Q1  
L
V
SENSE  
SW  
L
MAIN  
SWITCH ON  
SIGNAL  
I
V
1
I
OUT  
+
R3  
Q5  
R4  
V
D
NOTE: R3 = R4  
1777 SS  
7
LT1777  
U
OPERATIO  
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  
foundintraditionaldesigns,including:InternalBiasRegu-  
lator, Oscillator, Logic, and Feedback Amplifier. The novel  
portion includes a specialized Output Switch section in-  
cludingcircuitstolimitthedI/dtanddV/dtswitchingrates.  
coupled with small-valued capacitor C1 to the VIN supply  
rail. The product of negative voltage slew rate times this  
capacitor value equals current, and when this current  
throughemitter/baseresistorR1exceedsadiodedrop,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 ±2VBE, drive current will be supplied or removed  
as necessary to limit current slew rate. The actual sensing  
is performed between the output node labeled VSW and a  
new node labeled VD.  
TheLT1777operatesmuchthesameastraditionalcurrent  
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 I1 driving the base of PNP transistor Q2. The  
collectorofQ2inturndrivesthebaseofNPNoutputdevice  
Q1. The considerable base/collector capacitance of PNP  
Q2actstolimitdV/dtrateduringswitchturn-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.”  
In the case of switch turn-on, current drive is provided by  
PNP Q2. If the voltage at VSW reaches 2VBE above that at  
VD, transistor Q5 turns on and removes a portion of Q2’s  
drive from Q1’s base. Similarly for turn-off, as the VSW  
node goes 2VBE below VD, 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.  
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  
8
LT1777  
U
W U U  
APPLICATIONS INFORMATION  
external sense inductor to set a maximum allowed dI/dt  
rate. Thisattenuatesthehighestfrequencycomponentsof  
generated B field RFI. Minimal lead length in the path is  
also essential to minimize generated RFI.  
Basics of Low Noise Operation  
Switching power supply circuits are often preferred over  
linear topologies for their improved efficiency (POUT/ PIN).  
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.  
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  
fundamentalandlowerharmonics. Nevertheless, therela-  
tively intense magnetic field present in the main inductor  
cancausecouplingproblems,especiallyifthemaininduc-  
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.  
There are two types of RFI emissions, i.e., conducted and  
radiated. Conducted interference travels directly through  
“wires”,asopposedtoradiatedinterference,whichtravels  
through the air. Conducted RFI can be created by a  
switching power supply at its input voltage supply node,  
itsoutputnode(s)orboth.Itistypicallycausedbypulsatile  
current flow through the residual high frequency imped-  
ance (ESR) of bypass capacitors.  
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.  
Radiated interference can be of two types: electric (E field)  
ormagnetic(Bfield).Efieldinterferenceiscausedbystray  
capacitance coupling of the node(s) which swing rapidly  
over a large voltage excursion. In the LT1777, this in-  
cludes the VSW and VD 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.  
LT1777  
+
L
SENSE  
L
V
IN  
MAIN  
C1  
V
OUT  
+
D1  
C2  
1777 F01  
Figure 1. High Speed Current Switching Paths  
B field RFI is simply coupling of high frequency magnetic  
fieldsgeneratedbytheoffendingcircuitry. Highfrequency  
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  
Selecting Sense Inductor  
The LT1777 uses an external sense inductor to set a  
theoretical limit for current ramp rate according to the  
formula:  
2VBE  
LSENSE  
Max dI/dt =  
9
LT1777  
U
W U U  
APPLICATIONS INFORMATION  
Deciding upon a value for the sense inductor involves  
Asanexample,amaximuminputvoltageof36V,anoutput  
voltage of 5V and a main inductor value of 220µH yields a  
maximum suggested sense inductor value of 3.5µH.  
evaluating the trade-off between overall efficiency (POUT  
/
PIN) and switch current slew rate. Larger sense inductors  
yield lower current slew rates which offer reduced high  
frequency RFI emissions, but at the expense of poorer  
efficiency.  
Circuit behavior versus sense inductor value is shown in  
the oscilloscope photos in Figure 2. The circuit and oper-  
ating conditions are similar to the Typical Application on  
the first page of this data sheet with the exception that the  
sense inductor is allowed to assume the series of values:  
0µH, 0.47µH, 1µH and 2.2µH. Figure 2a shows a close-up  
of the leading edge (turn-on) of the current waveform.  
Values of 0µH and 0.47µH are found to yield a dI/dt of  
about 2.2A/µs, while 1µH yields 1.4A/µs and 2.2µH yields  
0.6A/µs. Figure2bshowsthetrailingedge(turn-off)ofthe  
The question is “What is the allowed range of values for a  
sense inductor in a given application?” There is really no  
minimum limit to the sense inductor, i.e., its value is  
allowed to be zero. (In other words, the physical sense  
inductor ceases to exist and is replaced by a short circuit.)  
This will yield the highest efficiency possible in a given  
situation. Although an explicit current slew rate no longer  
exists, the naturally less aggressive nature of the LT1777  
will often yield quieter supply operation than other stan-  
dard switching regulators.  
As far as the maximum allowable value for the sense  
inductor, this is dictated by the current ramp rate in the  
main inductor during the conventional part of the switch-  
ing cycle. It is generally overconservative to limit the  
switch current slew rate to that exhibited by the main  
inductor. This would potentially yield a triangular current  
waveform. Efficiency would be greatly reduced at little  
further gain in noise performance. Stated mathematically,  
maximum slew rate in the main inductor occurs at maxi-  
mum input voltage as:  
1777 F02a  
200ns/DIV  
(a) Leading Edge  
Max VIN VOUT  
LMAIN  
dI  
dt  
=
The sense inductor experiences 2VBE of applied voltage.  
Thisisperhaps1.0Vatamaximumhotcondition.Ifweuse  
an additional factor of two to be conservative, this yields  
a maximum sense inductor value as follows:  
Max VIN VOUT  
LMAIN  
0.5V  
LSENSE  
1777 F02b  
200ns/DIV  
=
or,  
(b) Trailing Edge  
0.5V  
Max VIN VOUT  
Max LSENSE = LMAIN  
Figure 2. VSW Node Current Behavior vs LSENSE Value.  
LSENSE = 0µH, 0.47µH, 1.0µH and 2.2µH  
10  
LT1777  
U
W U U  
APPLICATIONS INFORMATION  
current waveform. The four sense inductor values of 0µH,  
0.47µH, 1µH and 2.2µH yield dI/dt rates of roughly  
4.5A/µs, 2.2A/µs, 1.4A/µs and 0.6A/µs, respectively.  
Harmonic Behavior  
TheLT1676isahighefficiencycousintotheLT1777. An  
additional set of oscilloscope photographs in Figure 3  
show the leading edge and trailing edge of the current  
waveform when this part is substituted for the LT1777.  
(No sense inductor is used with the LT1676.) The leading  
and trailing edges of the LT1676 current waveform are  
much faster than that of the LT1777, even when the  
LT1777 uses a sense inductor of 0µH. The 10% to 90%  
rise time/fall time is on the order of 10ns to 20ns, too fast  
to measure accurately at the horizontal sweep rate of  
200ns/DIV.  
Thesephotosshowthatthereisaminimumeffectivevalue  
for sense inductance, which is 0.47µH for a typical part at  
room temperature as shown. This value inductor has a  
small effect on the trailing edge rate, but essentially no  
effect on the rising edge. Minimum effective sense induc-  
tance value means that inductors much smaller than this  
valuewillhavesubstantiallythesameperformanceaszero  
inductance, such that these inductors serve no useful  
purpose.  
In summary,  
While this time-based analysis demonstrates that the  
current waveform of the LT1777 is quieter than standard  
high efficiency buck converters, some users may prefer to  
see a direct comparison on a frequency domain basis.  
Figures 4a, 4b, and 4c show a spectral analysis of the  
currentwaveforms.Thehorizontalaxisis2MHz/DIV(0MHz  
to 20MHz), and the vertical axis is 10dB/DIV. All photos  
were taken with VIN = 24V and VOUT = 5V at 400mA. Figure  
4a is of the LT1676 and is for comparison purposes.  
Figures 4b and 4c are of the LT1777 with a sense inductor  
of 0µH and 2.2µH, respectively. A decrease in high fre-  
quency energy is seen when going from the LT1676 to the  
LT1777 with no sense inductor, and a further improve-  
mentwitha2.2µHsenseinductor. Forexample, at10MHz,  
the LT1777 shows an improvement of about –10dB with  
0µH and perhaps 25dB with 2.2µH.  
1. The LT1777 uses an external sense inductor to set a  
theoretical limit for current ramp rate according to the  
formula:  
2VBE  
LSENSE  
Max dI/dt =  
2. Allowable range for the sense inductor runs from a  
minimum of 0 to a maximum of:  
0.5V  
Max VIN VOUT  
Max LSENSE = LMAIN  
3. Theminimumeffectiveinductorsizeistypically0.47µH.  
1777 F03a  
1777 F03b  
200ns/DIV  
200ns/DIV  
(a) Leading Edge  
(b) Trailing Edge  
Figure 3. LT1676 Current Behavior for Comparison Purposes Only  
11  
LT1777  
U
W U U  
APPLICATIONS INFORMATION  
voltage of 12V, and then 36V. Once again the circuit is the  
Typical Application shown on the first page of this data  
sheet, with an output load of 400mA.  
Figure 5a, with VIN of 12V, shows a relatively rectangular  
voltagewaveform.Thelimitedvoltageslewratestillallows  
for nearly vertical switching edges, so little power is  
wasted. A positive-going step before the leading edge and  
a negative-going step after the trailing edge can be seen.  
Theseareevidenceoftheinternalcurrentlimitingcircuitry  
at work.  
1777 F04a  
0MHz to 20MHz (2MHz/DIV)  
(a) LT1676 for Comparison  
Figure 5b, with VIN of 36V, shows a substantially  
nonrectangular waveform. The limited voltage slew rate is  
clearly evident as transitions take a few hundred nanosec-  
onds. Efficiency (POUT/PIN) is reduced as a result of the  
slower transitions. For comparison purposes, the oscillo-  
scopephotoinFigure6showstheperformanceofthehigh  
efficiency LT1676. Voltage transitions are well under  
100ns and the waveform appears quite rectangular.  
1777 F04b  
0MHz to 20MHz (2MHz/DIV)  
(b) LT1777 with LSENSE = 0µH  
GND  
1777 F05a  
1µs/DIV  
(a) VIN = 12V  
1777 F04c  
0MHz to 20MHz (2MHz/DIV)  
(c) LT1777 with LSENSE = 2.2µH  
Figure 4. Spectral Analysis of Current Waveforms in  
Figures 2 and 3. (VIN = 24V, VOUT = 5V, IOUT = 400mA)  
Voltage Waveform Behavior  
Unlike current behavior, voltage slew rate of the LT1777 is  
not adjustable by the user. No component selection or  
other action is required. Nevertheless, it is instructive to  
examine typical behavior. The oscilloscope photos in  
Figure 5 show the VSW voltage waveform with an input  
GND  
1777 F05b  
500ns/DIV  
(b) VIN = 36V  
Figure 5. VSW Node Voltage Behavior  
12  
LT1777  
U
W U U  
APPLICATIONS INFORMATION  
through the main inductor has most of its energy concen-  
trated in the fundamental and lower harmonics.) Toroidal  
style inductors, many available in surface mount configu-  
ration, offer a reduced external magnetic field, generally at  
an increase in cost and physical size. Although custom  
design is always a possibility, most potential LT1777 ap-  
plicationscanbehandledbythearrayofstandard, off-the-  
shelf inductor products offered by the major suppliers.  
GND  
1777 F06  
Selecting Bypass Capacitors  
500ns/DIV  
Figure 6. LT1676 VSW Node Voltage Behavior  
for Comparison Purposes Only, VIN = 36V  
The basic topology as shown in the Typical Application on  
the first page uses two bypass capacitors, one for the VIN  
input supply and one for the VOUT output supply.  
Selecting Main Inductor  
User selection of an appropriate output capacitor is rela-  
tivelyeasy,asthiscapacitorseesonlytheACripplecurrent  
in the inductor L1. As the LT1777 is designed for buck or  
step-down applications, output voltage will nearly always  
be compatible with tantalum type capacitors, which are  
generally available in ratings up to 35V or so. These  
tantalumtypesoffergoodvolumetricefficiency, andmany  
areavailablewithspecifiedESRperformance.Theproduct  
ofinductorACripplecurrentandoutputcapacitorESRwill  
manifestitselfaspeak-to-peakvoltagerippleontheoutput  
node. (Note: If this ripple becomes too large, heavier  
control loop compensation, at least at the switching fre-  
quency, may be required on the VC pin.)  
There are several parameters to consider when selecting  
a main inductor. These include inductance value, peak  
current rating (to avoid core saturation), DC resistance,  
construction type, physical size, and of course, cost.  
Once the inductance value is decided, inductor peak  
current rating and resistance need to be considered. Here,  
the inductor peak current rating refers to the onset of  
saturation in the core material, although manufacturers  
sometimes specify a “peak current rating” which is de-  
rived from a worst-case combination of core saturation  
andself-heatingeffects.Inductorwindingresistancealone  
limits the inductor’s current carrying capability as the I2R  
power threatens to overheat the inductor. Remember to  
include the condition of output short circuit, if applicable.  
Although the peak current rating of the inductor can be  
exceeded in short-circuit operation, as core saturation per  
se is not destructive to the core, excess resistive self-  
heating is still a potential problem.  
The input bypass capacitor can present a more difficult  
choice. In a typical application e.g., 24VIN to 5VOUT  
,
relatively heavy VIN current is drawn by the power switch  
for only a small portion of the oscillator period (low ON  
duty cycle). The resulting RMS ripple current, for which  
the capacitor must be rated, can be several times the DC  
average VIN current. The straightforward choice for a low  
volume, surface mountable electrolytic capacitor with  
good ESR/ripple current ratings is a tantalum type. How-  
ever, worst-case (high) input voltage coupled with stan-  
dard capacitor voltage derating may exceed the 35V or so  
for which tantalum capacitors are generally available.  
Relatively bulky “high frequency” aluminum electrolytic  
types, specifically constructed and rated for switching  
supply applications, may then be the only choice.  
The final inductor selection is generally based on cost,  
which usually translates into choosing the smallest physi-  
cal size part which meets the desired inductance value,  
resistance and current carrying capability. An additional  
factor to consider is that of physical construction. Briefly  
stated, “open” inductors built on a rod- or barrel-shaped  
core generally offer the smallest physical size and lowest  
cost. However their open construction does not contain  
the resulting magnetic field, and they may not be accept-  
able in RFI-sensitive applications. (A mitigating factor is  
that, as mentioned previously, the AC current passing  
Additionally, it may be advantageous to parallel the input  
and output capacitors with 0.1µF ceramic bypass capaci-  
13  
LT1777  
U
W U U  
APPLICATIONS INFORMATION  
tors. Their relatively low ESR in the mid-MHz region can  
The solution to this dilemma is to slow down the oscillator  
when the FB pin voltage is abnormally low thereby indicat-  
ing some sort of short-circuit condition. Figure 7 shows  
the typical response of oscillator frequency vs FB pin  
voltage. Oscillator frequency is normal until FB voltage  
dropstoabouthalfofitsnormalvalue. Belowthispointthe  
oscillator frequency decreases linearly down to a limit of  
about25kHz.Thisloweroscillatorfrequencyduringshort-  
circuit conditions can then maintain control with the  
effective minimum on time.  
further attenuate high speed glitches.  
Maximum Load/Short-Circuit Considerations  
The LT1777 is a current mode controller. It uses the VC  
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 VC  
node, nominally 2.0V, then acts as an output switch peak  
current limit. This action becomes the switch current limit  
specification. The maximum available output power is  
then determined by the switch current limit.  
A further potential problem with short-circuit operation  
might occur if the user were operating the part with its  
oscillator slaved to an external frequency source via the  
SYNC pin. However, the LT1777 has circuitry to automati-  
cally disable the sync function when the oscillator is  
slowed down due to abnormally low FB voltage.  
A potential controllability problem could occur under  
short-circuit conditions. If the power supply output is  
short circuited, the feedback amplifier responds to the low  
output voltage by raising the control voltage, VC, to its  
peak current limit value. Ideally, the output switch would  
be turned on, and then turned off as its current exceeded  
thevalueindicatedbyVC.However,thereisfiniteresponse  
time involved in both the current comparator and turn-off  
of the output switch. These result in a minimum on time  
tON(MIN). When combined with the large ratio of VIN to  
(VF + I • R), the diode forward voltage plus inductor I • R  
voltage drop, the potential exists for a loss of control.  
Expressed mathematically the requirement to maintain  
control is:  
120  
100  
R
= 22k  
TH  
80  
60  
R
= 10k  
R
= 4.7k  
TH  
TH  
40  
20  
0
LT1777  
FB  
R
TH  
0
0.25  
0.50  
0.75  
1.00  
1.25  
VF +I•R  
FB DIVIDER THEVENIN VOLTAGE (V)  
f t  
( )(  
)
ON  
VIN  
1777 F07  
Figure 7. Oscillator Frequency vs FB Divider  
Thevenin Voltage and Impedance  
where:  
f = switching frequency  
tON = switch on time  
Feedback Divider Considerations  
VF = diode forward voltage  
VIN = Input voltage  
AnLT1777applicationtypicallyincludesaresistivedivider  
betweenVOUT andground, thecenternodeofwhichdrives  
the FB pin to the reference voltage VREF. This establishes  
a fixed ratio between the two resistors, but a second  
degree of freedom is offered by the overall impedance  
level of the resistor pair. The most obvious effect this has  
is one of efficiency—a higher resistance feedback divider  
will waste less power and offer somewhat higher effi-  
ciency, especially at light load.  
I • R = inductor I • R voltage drop  
If this condition is not observed, the current will not be  
limited at IPK, but will cycle-by-cycle ratchet up to some  
higher value. Using the nominal LT1777 clock frequency  
of 100kHz, a VIN of 48V and a (VF + I • R) of say, 0.7V, the  
maximum tON to maintain control would be approximately  
140ns, an unacceptably short time.  
14  
LT1777  
U
W U U  
APPLICATIONS INFORMATION  
However, remember that oscillator slowdown to achieve  
short-circuit protection (discussed above) is dependent  
on FB pin behavior, and this in turn, is sensitive to FB node  
external impedance. The graph in Figure 7 shows the  
typical relationship between FB pin voltage, driving im-  
pedance and oscillator frequency. This shows that as  
feedbacknetworkimpedanceincreasesbeyond10k,com-  
plete oscillator slowdown is not achieved, and short-  
circuitprotectionmaybecompromised. Andasapractical  
matter, the product of FB pin bias current and larger FB  
network impedances will cause increasing output voltage  
error. (Nominal cancellation for 10k of FB Thevenin im-  
pedance is included internally.)  
suggested. Operate the proposed power supply over the  
applicable input voltage and load current ranges. Measure  
the input power and output power, and calculate the  
difference as “lost power.” This measured lost power  
minus estimated inductor and diode dissipation yields a  
figure for internal LT1777 dissipation. Fortunately, as  
LT1777 internal dissipation dominates total lost power,  
inductor and diode power need not be estimated very  
accurately.InductorpowermaybeestimatedasI2Rwhere  
I is the load current and R is the DC resistance of the  
inductor. (Loss in the sense inductor is usually so small  
that only the main inductor must be considered.) Diode  
power may be estimated as 1/2 • VF• I • DC, where VF is the  
diode forward voltage, I is the load current and DC is the  
duty cycle percentage when the diode is conducting.  
Thermal Considerations  
Care should be taken to ensure that the worst-case input  
voltage and load current conditions do not cause exces-  
sive die temperatures. The SO16 package is rated at  
50°C/W when the four corner package pins are connected  
to a good ground plane. (These corner pins are internally  
fused to the die paddle for improved thermal perfor-  
mance.) Die junction temperature is then a function of  
ambient temperature and internal dissipation as follows:  
Frequency Compensation  
Loop frequency compensation is performed by connect-  
ing a capacitor, or in most cases a series R/C, from the  
output of the error amplifier (VC pin) to ground. Proper  
loop compensation may be obtained by empirical meth-  
ods as described in detail in Application Note AN19.  
Briefly, this involves applying a load transient and observ-  
ing the dynamic response over the expected range of VIN  
and ILOAD values.  
TJ = TA + θJA • PINT  
Total internally dissipated power is composed of three  
parts, quiescent power, DC switch loss and AC switch  
loss. The AC switch loss will often dominate the total  
dissipation, and this is unfortunately difficult to estimate  
accurately.  
As a practical matter, a second small capacitor, directly  
from the VC pin to ground is generally recommended to  
attenuate capacitive coupling from the VSW and VD pins. A  
typical value for this capacitor is 100pF. (See Switch Node  
Considerations).  
Two options are suggested to the potential user. The first  
is to observe the graphical data presented in the Typical  
Applications section. Internal LT1777 dissipation vs load  
current is given for output voltages of 5V and 3.3V, with  
input voltages of 12V, 24V and 36V, and with sense  
inductors of 0µH, 1µH, and 2.2µH (Figures 9 and 11).  
While it is true that the user’s ultimate circuit may use  
somewhat different passive components than the ex-  
amples given, it turns out that internal IC dissipation is not  
very sensitive to these changes.  
Switch Node Considerations  
InspiteofthefactthattheLT1777isalownoiseconverter,  
it is still possible for the part to cause problems by  
“coupling to itself.” Specifically, this can occur if the VSW  
pin is allowed to capacitively couple in an uncontrolled  
manner to the part’s high impedance nodes, i.e., SHDN,  
SYNC, VC and FB. This can cause erratic operation such as  
odd/even cycle behavior, pulse width “nervousness”, im-  
proper output voltage and/or premature current limit  
action.  
In cases where the user’s potential circuit differs signifi-  
cantly from the examples given, an empirical method is  
15  
LT1777  
U
W U U  
APPLICATIONS INFORMATION  
As an example, assume that the capacitance between the  
VSW nodeandahighimpedancepinnodeis0.1pF,andthat  
the high impedance node in question exhibits a capaci-  
tance of 1pF to ground. Also assume a “typical” 36VIN to  
5VOUT application. Due to the large voltage excursion at  
the VSW node, this will couple a 3.5V(!) transient to the  
high impedance pin, causing abnormal operation. An  
explicit 100pF capacitor added to the node will reduce the  
amplitude of the disturbance to more like 35mV (although  
settling time will increase).  
Specific pin recommendations are as follows:  
SHDN: If unused, add a 100pF capacitor to ground.  
SYNC: Ground if unused.  
VC: Add a capacitor directly to ground in addition to the  
explicit compensation network. A value of one-tenth of  
the main compensation capacitor is recommended, up  
to a maximum of 100pF.  
FB: Assuming the VC pin is handled properly, this pin  
usually requires no explicit capacitor of its own, but  
keep this node physically small to minimize stray  
capacitance.  
16  
LT1777  
U
TYPICAL APPLICATIONS  
Basic 5V Output Application  
output current should not present a problem, though.) As  
shown, the SHDN and SYNC pins are unused, however  
either(orboth)canbeoptionallydrivenbyexternalsignals  
as desired.  
Figure 8 shows a basic application that produces 5V at up  
to 500mA IOUT. Efficiency and Internal Power Dissipation  
graphs are shown in Figure 9 for input voltages of 12V,  
24V and 36V, and for sense inductor values of 0µH, 1µH  
and 2.2µH. Be aware that continuous operation at the  
combination of high input voltage, large sense inductor  
and high output current may not be possible due to  
thermal constraints. (Brief transients in input voltage or  
Thedataasshownwereperformedusinganoff-the-shelf  
Coilcraft DO3316-224 as the main inductor. This is a  
cost-effective inductor using an open style of construc-  
tion. For a toroidal style inductor, the Coiltronics  
CTX250-4 or similar may be substituted.  
V
IN  
10  
10V TO 40V  
+
C1  
39µF  
63V  
C6  
0.1µF  
V
IN  
3
4
L1  
SHDN  
LT1777  
SYNC  
V
CC  
0µH TO 2.2µH  
C5  
100pF  
L2  
(SEE BELOW)  
220µH  
12  
14  
6
V
OUT  
V
SW  
5V  
5
+
C2  
100µF  
10V  
R1  
36.5k  
1%  
V
V
D
C
C7  
0.1µF  
13  
D1  
C4  
100pF  
R3  
12k  
C3  
2200pF  
FB  
SGND  
R2  
12.1k  
1%  
7
C1: PANASONIC HFQ ELECTROLYTIC  
C2: AVX D CASE TPSD107M010R0080  
C3, C4, C5: NPO OR X7R  
L1: SENSE INDUCTOR CAN VARY FROM 0µH TO 2.2µH  
AS PER APPLICATION. GRAPHICAL DATA TAKEN WITH:  
1µH = D01608C-102, COILCRAFT OR SIMILAR  
1777 F08  
C6, C7: Z5U  
2.2µH = D01608C-222, COILCRAFT OR SIMILAR (SEE TEXT)  
D1: MOTOROLA 100V, 1A SMD SCHOTTKY  
MBRS1100  
L2: COILCRAFT D03316-224 OR SIMILAR (SEE TEXT)  
Figure 8. Basic 5V Output Application  
17  
LT1777  
U
TYPICAL APPLICATIONS  
Efficiency  
Internal Dissipation  
90  
1.4  
1.2  
1.0  
0.8  
0.6  
0.4  
0.2  
0
L
=
V
V
T
= 12V  
= 5V  
SENSE  
0µH  
V
V
T
= 12V  
OUT  
= 25°C  
IN  
IN  
= 5V  
OUT  
80  
70  
60  
50  
40  
30  
20  
= 25°C  
A
A
1µH  
2.2µH  
L
=
SENSE  
2.2µH  
VIN = 12V  
1µH  
0µH  
1
10  
100  
1000  
10  
1000  
100  
(mA)  
I
I
(mA)  
OUT  
LOAD  
1777 F09a  
1777 F09b  
90  
80  
70  
60  
50  
40  
30  
20  
1.4  
1.2  
1.0  
0.8  
0.6  
0.4  
0.2  
0
L
=
V
= 24V  
OUT  
= 25°C  
V
V
A
= 24V  
OUT  
= 25°C  
SENSE  
IN  
IN  
L
=
SENSE  
0µH  
2.2µH  
V
= 5V  
= 5V  
T
A
T
1µH  
1µH  
0µH  
2.2µH  
VIN = 24V  
1
10  
100  
1000  
10  
1000  
100  
(mA)  
I
I
(mA)  
OUT  
LOAD  
1777 F09c  
1777 F09d  
90  
80  
70  
60  
50  
40  
30  
20  
1.4  
1.2  
1.0  
0.8  
0.6  
0.4  
0.2  
0
L
=
V
= 36V  
OUT  
= 25°C  
V
= 36V  
IN  
OUT  
SENSE  
IN  
2.2µH  
V
= 5V  
V
= 5V  
L
=
SENSE  
0µH  
T
A
T = 25°C  
A
1µH  
0µH  
1µH  
VIN = 36V  
2.2µH  
1
10  
100  
1000  
10  
1000  
100  
I
(mA)  
I
(mA)  
OUT  
LOAD  
1777 F09e  
1777 F09f  
Figure 9. Efficiency and LT1777 Internal Dissipation for the Basic 5V Output Application  
18  
LT1777  
U
TYPICAL APPLICATIONS  
Basic 3.3V Output Application  
dissipation is largely determined by input voltage, load  
current and sense inductor, and is only a weak function of  
output voltage.  
Figure 10 shows a circuit similar to the previous example,  
but modified for a 3.3V output. Once again, Efficiency and  
Internal Power Dissipation graphs are shown in Figure 11  
for input voltages of 12V, 24V and 36V, and for sense  
inductor values of 0µH, 1µH and 2.2µH. It is interesting to  
note that internal LT1777 dissipation is very close to the  
5V example. This confirms the fact that internal LT1777  
The data as shown were performed using an off-the-shelf  
Coilcraft DO3316-154 as the main inductor. This is a cost-  
effective inductor using an open style of construction. For  
a toroidal style inductor, the Coiltronics CTX150-4 or  
similar may be substituted.  
V
IN  
10  
10V TO 40V  
+
C1  
39µF  
63V  
C6  
0.1µF  
V
IN  
3
4
L1  
SHDN  
LT1777  
SYNC  
V
CC  
0µH TO 2.2µH  
C5  
100pF  
L2  
(SEE BELOW)  
150µH  
12  
14  
6
V
OUT  
V
SW  
3.3V  
5
+
C2  
100µF  
10V  
R1  
20k  
1%  
V
C
V
D
C7  
0.1µF  
13  
D1  
C4  
100pF  
R3  
12k  
C3  
2200pF  
FB  
SGND  
R2  
12.1k  
1%  
7
C1: PANASONIC HFQ ELECTROLYTIC  
C2: AVX D CASE TPSD107M010R0080  
C3, C4, C5: NPO OR X7R  
L1: SENSE INDUCTOR CAN VARY FROM 0µH TO 2.2µH  
AS PER APPLICATION. GRAPHICAL DATA TAKEN WITH:  
1µH = D01608C-102, COILCRAFT OR SIMILAR  
1777 F10  
C6, C7: Z5U  
2.2µH = D01608C-222, COILCRAFT OR SIMILAR (SEE TEXT)  
D1: MOTOROLA 100V, 1A SMD SCHOTTKY  
MBRS1100  
L2: COILCRAFT D03316-154 OR SIMILAR (SEE TEXT)  
Figure 10. Basic 3.3V Output Application  
19  
LT1777  
U
TYPICAL APPLICATIONS  
Efficiency  
Internal Dissipation  
90  
1.4  
1.2  
1.0  
0.8  
0.6  
0.4  
0.2  
0
V
V
T
= 12V  
= 3.3V  
= 25°C  
V
V
T
= 12V  
= 3.3V  
= 25°C  
IN  
OUT  
A
IN  
OUT  
A
L
=
SENSE  
0µH  
80  
70  
60  
50  
40  
30  
20  
1µH  
2.2µH  
L
=
SENSE  
2.2µH  
VIN = 12V  
1µH  
0µH  
1
10  
100  
1000  
10  
1000  
100  
(mA)  
I
(mA)  
I
LOAD  
OUT  
1777 F11a  
1777 F11b  
90  
80  
70  
60  
50  
40  
30  
20  
1.4  
1.2  
1.0  
0.8  
0.6  
0.4  
0.2  
0
L
=
V
V
T
= 24V  
OUT  
= 25°C  
V
= 24V  
OUT  
SENSE  
IN  
IN  
2.2µH  
= 3.3V  
V
= 3.3V  
L
=
SENSE  
0µH  
T = 25°C  
A
A
1µH  
0µH  
1µH  
VIN = 24V  
2.2µH  
1
10  
100  
1000  
10  
1000  
100  
(mA)  
I
(mA)  
I
LOAD  
OUT  
1777 F11c  
1777 F11d  
90  
80  
70  
60  
50  
40  
30  
20  
1.4  
1.2  
1.0  
0.8  
0.6  
0.4  
0.2  
0
L
=
V
= 36V  
OUT  
= 25°C  
V
V
T
= 36V  
OUT  
= 25°C  
SENSE  
IN  
IN  
2.2µH  
V
T
= 3.3V  
= 3.3V  
A
A
1µH  
0µH  
L
=
SENSE  
0µH  
VIN = 36V  
1µH  
2.2µH  
1
10  
100  
1000  
10  
1000  
100  
(mA)  
I
(mA)  
I
LOAD  
OUT  
1777 F11e  
1777 F11f  
Figure 11. Efficiency and LT1777 Internal Dissipation for the Basic 3.3V Output Application  
20  
LT1777  
U
TYPICAL APPLICATIONS  
Optional Input/Output Filtering  
output voltage at 50mV/DIV, and the lower waveform is a  
DC-coupled representation of current into the node at  
50mA/DIV. Input voltage ripple is seen to decrease from  
100mVP-P toperhaps10mVP-P.Ripplecurrentisalsoseen  
to decrease dramatically. (This improvement in AC ripple  
current actually affects radiated magnetic noise.)  
When minimum conducted noise is required, it is often  
advantageous to add an explicit input and/or output filter  
to the topology. This can be a cost-effective way to reduce  
conducted noise on the input or output node by an order  
of magnitude or more. The exact details involved are a bit  
lengthy, so the user is referred to the thorough treatments  
in Application Notes AN19 and AN44. However, an ex-  
ample will be given to illustrate the principles involved.  
The next pair of scope photos in Figure 14 show an  
AC-coupled version of the output node at 2mV/DIV.  
Voltagerippleisseentobeoriginallyabout12mVP-P, with  
most of the energy in the lowest harmonics. After the  
addition of a 4.7µH inductor and a second 100µF output  
Figure 12 shows the previous “Basic 5V Output Applica-  
tion” modified with an additional input inductor and an  
output L/C combination. The dramatic improvement in  
noise performance is seen in the accompanying oscillo-  
scope photos shown in Figures 13 and 14. Operating  
conditions are VIN = 24V, IOUT = 400mA. The pair of scope  
photos in Figure 13 show the response at the input node,  
beforeandaftertheadditional33µHinductorisadded.The  
upper waveform shows an AC-coupled version of the  
capacitor, ripple is about 200µVP-P  
.
Theseinputandoutputinductorrequirementsaretypically  
not very difficult to achieve, and inexpensive open style  
DO1608C types were used in this example. Once again,  
more costly closed-construction style inductors may be  
employed, but these are usually not necessary, as the AC  
fields generated by these inductors are typically small.  
L3  
33µH  
V
IN  
10  
+
V
IN  
3
4
SHDN  
LT1777  
SYNC  
V
CC  
L4  
4.7µH  
12  
14  
6
V
V
OUT  
SW  
5
+
+
C8  
V
V
D
C
13  
100µF  
10V  
D1  
FB  
SGND  
7
ADDITIONAL FILTER COMPONENTS  
L3: COILCRAFT D01608C-333 OR SIMILAR  
L4: COILCRAFT D01608C-472 OR SIMILAR  
C8: AVX D CASE TPSD107M010R0080  
1777 F12  
Figure 12. Basic 5V Application with Optional Input/Output Filters  
VIN NODE VOLTAGE  
AC COUPLED  
50mV/DIV  
VIN NODE VOLTAGE  
AC COUPLED  
50mV/DIV  
VIN NODE CURRENT  
DC COUPLED  
50mA/DIV  
V
IN NODE CURRENT  
DC COUPLED  
50mA/DIV  
GND, CH2  
GND, CH2  
1777 F13a  
1777 F13b  
2µs/DIV  
2µs/DIV  
(a) Before Input Inductor  
(b) After Input Inductor  
Figure 13. Input Node Ripple  
21  
LT1777  
U
TYPICAL APPLICATIONS  
VOUT NODE  
AC COUPLED  
2mV/DIV  
VOUT NODE  
AC COUPLED  
2mV/DIV  
1777 F13a  
1777 F14b  
2µs/DIV  
2µs/DIV  
(a) Before Output Filter  
(b) After Output Filter  
Figure 14. Output Node Ripple  
User Programmable Undervoltage Lockout  
Behaviorisasfollows:Normaloperationisobservedatthe  
nominal input voltage of 24V. As the input voltage is  
decreasedtoroughly18V, switchingactionwillstop, VOUT  
will drop to zero, and the LT1777 will draw its VIN and VCC  
quiescent currents from the VIN supply. At a lower input  
voltage, typically 10V or so at 25°C, the voltage on the  
SHDNpinwilldroptotheshutdownthreshold,andthepart  
will draw its shutdown current only from the VIN rail. The  
resistive divider of R4 and R5 will continue to draw power  
from VIN. (The user should be aware that while the SHDN  
pin lockout threshold is relatively accurate including  
temperature effects, the SHDN pin shutdown threshold is  
morecoarse, andexhibitsconsiderablymoretemperature  
drift. Nevertheless the shutdown threshold will always be  
well below the lockout threshold.)  
Figure 15 uses a resistor divider between VIN and ground  
to drive the SHDN node. This is a simple, cost-effective  
way to add a user-programmable undervoltage lockout  
(UVLO) function. Resistor R5 is chosen to have approxi-  
mately 200µA through it at the nominal SHDN pin lockout  
threshold of roughly 1.25V. The somewhat arbitrary value  
of 200µA was chosen to be significantly above the SHDN  
pin input current to minimize its error contribution, but  
significantly below the typical 2.5mA the LT1777 draws in  
lockout mode. Resistor R4 is then chosen to yield this  
same 200µA, less 2.5µA, with the desired VIN UVLO volt-  
age minus 1.25V across it. (The 2.5mA factor is an allow-  
ance to minimize error due to SHDN pin input current.)  
V
IN  
R4  
84.5k  
1%  
LT1777  
SHDN  
R5  
6.19k  
1%  
C5  
100pF  
1777 F15  
Figure 15. User Programmable UVLO  
22  
LT1777  
U
Dimensions in inches (millimeters) unless otherwise noted.  
S Package  
PACKAGE DESCRIPTION  
16-Lead Plastic Small Outline (Narrow 0.150)  
(LTC DWG # 05-08-1610)  
0.386 – 0.394*  
(9.804 – 10.008)  
16  
15  
14  
13  
12  
11  
10  
9
0.150 – 0.157**  
0.228 – 0.244  
(3.810 – 3.988)  
(5.791 – 6.197)  
5
7
8
1
2
3
4
6
0.010 – 0.020  
(0.254 – 0.508)  
× 45°  
0.053 – 0.069  
(1.346 – 1.752)  
0.004 – 0.010  
(0.101 – 0.254)  
0.008 – 0.010  
(0.203 – 0.254)  
0° – 8° TYP  
0.050  
(1.270)  
BSC  
0.014 – 0.019  
(0.355 – 0.483)  
TYP  
0.016 – 0.050  
(0.406 – 1.270)  
S16 1098  
*DIMENSION DOES NOT INCLUDE MOLD FLASH. MOLD FLASH  
SHALL NOT EXCEED 0.006" (0.152mm) PER SIDE  
**DIMENSION DOES NOT INCLUDE INTERLEAD FLASH. INTERLEAD  
FLASH SHALL NOT EXCEED 0.010" (0.254mm) PER SIDE  
Information furnished by Linear Technology Corporation is believed to be accurate and reliable.  
However, no responsibility is assumed for its use. Linear Technology Corporation makes no represen-  
tationthattheinterconnectionofitscircuitsasdescribedhereinwillnotinfringeonexistingpatentrights.  
23  
LT1777  
U
TYPICAL APPLICATION  
Minimum PC Board Size Application  
circuit is capable of delivering up to 300mA at 5V, from  
input voltages as high as 28V. The only disadvantage is  
that due to the increased resistance in the inductor, the  
circuitisnolongercapableofwithstandingindefiniteshort  
circuits to ground. The LT1777 will still current limit at its  
nominal ILIM value, but this will overheat the inductor.  
Momentary short circuits of a few seconds or less can still  
be tolerated.  
Thepreviouslydescribedbasicapplicationsemploypower  
path parts which are capable of delivering the full rated  
input supply voltage and output current capabilities of the  
LT1777. A substantial improvement in printed circuit  
board area requirements can be achieved with the circuit  
shown below. This uses a physically smaller and less  
costlypower inductorand atantaluminputcapacitor. This  
Minimum PC Board Area Application  
V
IN  
10V TO 28V  
10  
+
C1  
22µF  
35V  
C6  
0.1µF  
V
IN  
3
4
L1  
SHDN  
LT1777  
SYNC  
V
CC  
0µH TO 2.2µH  
C5  
100pF  
L2  
(SEE BELOW)  
200µH  
12  
14  
6
V
OUT  
5V  
V
SW  
5
+
C2  
100µF  
10V  
R1  
36.5k  
1%  
V
C
V
D
C7  
0.1µF  
13  
D1  
C4  
100pF  
R3  
12k  
C3  
2200pF  
FB  
SGND  
R2  
12.1k  
1%  
7
C1: AVX E CASE TPSE226M035R0300  
C2: AVX D CASE TPSD107M010R0080  
C3, C4, C5: NPO OR X7R  
L1: SENSE INDUCTOR CAN VARY FROM 0µH TO 2.2µH  
AS PER APPLICATION. SEE PREVIOUS SCHEMATICS  
FOR EXAMPLES  
1777 TA03  
C6, C7: Z5U  
L2: COILCRAFT CTX200-1 OR SIMILAR  
D1: MOTOROLA 100V, 1A SMD SCHOTTKY  
MBRS1100  
RELATED PARTS  
PART NUMBER  
LT1076  
DESCRIPTION  
COMMENTS  
Integrated 2A Switch, V Up to 46V  
IN  
Push-Pull Design for Low Noise Isolated Supplies  
Ultralow Noise Regulator for Boost Topologies  
Output Up to 1.25A, Integrated Switch, SO-8 Package  
Fixed Frequency 550kHz Operation, MSOP Package  
100kHz, 2A Step-Down Switching Regulator  
Ultralow Noise 1A Switching Regulator  
Ultralow Noise 2A Switching Regulator  
200kHz, 1.5A Step-Down Switching Regulator  
LT1533  
LT1534  
LT1576  
LTC1622  
LTC1624  
Low V Step-Down DC/DC Controller  
High Efficiency SO-8 DC/DC Controller  
IN  
200kHz Operation, V from 3.5V to 36V, SO-8 Package  
IN  
LT1676/LT1776 Wide Input Range, High Efficiency, Step-Down Voltage Regulator 7.4V to 60V Input, 100/200kHz Operation, 700mA Internal Switch  
1777f LT/TP 0899 4K • PRINTED IN USA  
LinearTechnology Corporation  
1630 McCarthy Blvd., Milpitas, CA 95035-7417  
24  
LINEAR TECHNOLOGY CORPORATION 1999  
(408)432-1900 FAX:(408)434-0507 www.linear-tech.com  

相关型号:

LT1777CS

Low Noise Step-Down Switching Regulator
Linear

LT1777CS#PBF

LT1777 - Low Noise Step-Down Switching Regulator; Package: SO; Pins: 16; Temperature Range: 0°C to 70°C
Linear

LT1777CS#TR

LT1777 - Low Noise Step-Down Switching Regulator; Package: SO; Pins: 16; Temperature Range: 0°C to 70°C
Linear

LT1777CS#TRPBF

暂无描述
Linear

LT1777I

Low Noise Step-Down Switching Regulator
Linear

LT1777IS

Low Noise Step-Down Switching Regulator
Linear

LT1777IS#PBF

LT1777 - Low Noise Step-Down Switching Regulator; Package: SO; Pins: 16; Temperature Range: -40°C to 85°C
Linear

LT1777IS#TR

LT1777 - Low Noise Step-Down Switching Regulator; Package: SO; Pins: 16; Temperature Range: -40°C to 85°C
Linear

LT1777IS#TRPBF

LT1777 - Low Noise Step-Down Switching Regulator; Package: SO; Pins: 16; Temperature Range: -40°C to 85°C
Linear

LT1780

Low Power 5V RS232 Dual Driver/Receiver with 【15kV ESD Protection
Linear

LT17801IN

Transceiver
ETC

LT1780CN

Low Power 5V RS232 Dual Driver/Receiver with 【15kV ESD Protection
Linear