LTC1929IG [Linear]

2-Phase, High Efficiency, Synchronous Step-Down Switching Regulator; 2相,高效率,同步降压型开关稳压器
LTC1929IG
型号: LTC1929IG
厂家: Linear    Linear
描述:

2-Phase, High Efficiency, Synchronous Step-Down Switching Regulator
2相,高效率,同步降压型开关稳压器

稳压器 开关式稳压器或控制器 电源电路 开关式控制器 光电二极管
文件: 总24页 (文件大小:236K)
中文:  中文翻译
下载:  下载PDF数据表文档文件
Final Electrical Specifications  
LTC1929  
2-Phase, High Efficiency,  
Synchronous Step-Down  
Switching Regulator  
August 1999  
U
DESCRIPTIO  
FEATURES  
The LTC®1929 is a 2-phase, single output, synchronous  
step-down current mode switching regulator controller  
that drives N-channel external power MOSFET stages in a  
phase-lockable fixed frequency architecture. The 2-phase  
controller drives its two output stages out of phase at  
frequencies up to 300kHz to minimize the RMS ripple  
currents in both input and output capacitors. The 2-phase  
techniqueeffectivelymultipliesthefundamentalfrequency  
by two, improving transient response while operating  
each channel at an optimum frequency for efficiency.  
Thermal design is also simplified.  
2-Phase Single Output Controller  
Reduces Required Input Capacitance and Power  
Supply Induced Noise  
Current Mode Control Ensures Current Sharing  
Phase-Lockable Fixed Frequency: 150kHz to 300kHz  
True Remote Sensing Differential Amplifier  
OPTI-LOOPTM Compensation Improves Transient  
Response  
±1% Output Voltage Accuracy  
Wide VIN Range: 4V to 36V Operation  
Very Low Dropout Operation: 99% Duty Cycle  
Adjustable Soft-Start Current Ramping  
Internal Current Foldback  
Short-Circuit Shutdown Timer with Defeat Option  
Overvoltage Soft-Latch Eliminates Nuisance Trips  
Available in 28-Lead SSOP Package  
An internal differential amplifier provides true remote  
sensing of the regulated supply’s positive and negative  
output terminals as required by high current applications.  
The RUN/SS pin provides soft-start and a defeatable,  
timed, latched short-circuit shutdown to shut down both  
channels. Internal foldback current limit provides protec-  
tion for the external sychronous MOSFETs in the event of  
an output fault. OPTI-LOOP compensation allows the  
transient response to be optimized over a wide range of  
output capacitance and ESR values.  
U
APPLICATIO S  
Desktop Computers  
Internet/Network Servers  
Large Memory Arrays  
DC Power Distribution Systems  
, LTC and LT are registered trademarks of Linear Technology Corporation.  
OPTI-LOOP is a trademark of Linear Technology Corporation.  
U
TYPICAL APPLICATIO  
10  
V
IN  
5V TO 28V  
10µF ×4  
35V  
CERAMIC  
0.1µF  
S
V
TG1  
BOOST1  
SW1  
IN  
S
0.47µF  
0.1µF  
LTC1929  
RUN/SS  
L1  
1µH  
0.002Ω  
S
BG1  
D1  
PGND  
+
1000pF  
SENSE1  
SENSE1  
S
I
TH  
10k  
100pF  
TG2  
BOOST2  
SW2  
S
S
S
SGND  
V
OUT  
0.47µF  
1.6V/40A  
L2  
1µH  
S
S
8.06k  
0.002Ω  
S
V
BG2  
D2  
DIFFOUT  
S
EAIN  
INTV  
CC  
+
C
10µF  
OUT  
+
V
OS  
SENSE2  
SENSE2  
1000µF ×2  
8.06k  
+
4V  
V
OS  
C
: T510E108K004AS  
OUT  
L1, L2: CEPH149-1ROMC  
1929 TA01  
Figure 1. High Current 2-Phase Step-Down Converter  
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.  
1
LTC1929  
W W U W  
U
W
U
ABSOLUTE AXI U RATI GS  
(Note 1)  
PACKAGE/ORDER I FOR ATIO  
TOP VIEW  
ORDER PART  
NUMBER  
Input Supply Voltage (VIN).........................36V to 0.3V  
Topside Driver Voltages (BOOST1,2).........42V to 0.3V  
Switch Voltage (SW1, 2) .............................36V to 5 V  
SENSE1+, SENSE2+, SENSE1,  
1
2
NC  
28  
27  
26  
25  
24  
23  
22  
21  
20  
19  
18  
17  
16  
15  
RUN/SS  
+
TG1  
SENSE1  
LTC1929CG  
LTC1929IG  
3
SW1  
BOOST1  
SENSE1  
4
EAIN  
PLLFLTR  
PLLIN  
SENSE2Voltages........................ (1.1)INTVCC to 0.3V  
5
V
IN  
EAIN, VOS+, VOS, EXTVCC, INTVCC,  
6
BG1  
RUN/SS, AMPMD Voltages..........................7V to 0.3V  
Boosted Driver Voltage (BOOST-SW) ..........7V to 0.3V  
PLLFLTR, PLLIN, VDIFFOUT Voltages .... INTVCC to 0.3V  
ITH Voltage................................................2.7V to 0.3V  
Peak Output Current <1µs(TGL1,2, BG1,2)................ 3A  
INTVCC RMS Output Current................................ 50mA  
Operating Ambient Temperature Range  
LTC1929C.................................................. 0°C to 85°C  
LTC1929I .............................................. 40°C to 85°C  
Junction Temperature (Note 2)............................. 125°C  
Storage Temperature Range ................. 65°C to 150°C  
Lead Temperature (Soldering, 10 sec).................. 300°C  
7
EXTV  
CC  
NC  
8
INTV  
CC  
I
TH  
9
PGND  
BG2  
SGND  
10  
11  
12  
13  
14  
V
DIFFOUT  
BOOST2  
SW2  
V
V
OS  
OS  
+
TG2  
SENSE2  
SENSE2  
+
AMPMD  
G PACKAGE  
28-LEAD PLASTIC SSOP  
TJMAX = 125°C, θJA = 95°C/W  
Consult factory for Military grade parts.  
The denotes the specifications which apply over the full operating  
ELECTRICAL CHARACTERISTICS  
temperature range, otherwise specifications are at TA = 25°C. VIN = 15V, VRUN/SS = 5V unless otherwise noted.  
SYMBOL  
PARAMETER  
CONDITIONS  
MIN  
TYP  
MAX  
UNITS  
Main Control Loop  
V
V
Regulated Feedback Voltage  
Maximum Current Sense Threshold  
Feedback Current  
(Note 3); I Voltage = 1.2V  
0.792  
65  
0.800  
75  
0.808  
85  
V
mV  
nA  
EAIN  
TH  
V
= 5V  
SENSEMAX  
INEAIN  
SENSE  
I
(Note 3)  
–5  
50  
V
Output Voltage Load Regulation  
(Note 3)  
LOADREG  
Measured in Servo Loop; I Voltage = 0.7V  
Measured in Servo Loop; I Voltage = 2V  
0.05  
0.1  
0.3  
0.5  
%
%
TH  
TH  
V
V
Reference Voltage Line Regulation  
Output Overvoltage Threshold  
Undervoltage Lockout  
V
= 3.6V to 30V (Note 3)  
IN  
0.002  
0.86  
3.5  
%/V  
V
REFLNREG  
OVL  
Measured at V  
0.84  
3
0.88  
4
EAIN  
UVLO  
V
Ramping Down  
V
IN  
TH  
TH  
g
g
Transconductance Amplifier g  
I
I
= 1.2V; Sink/Source 5µA; (Note 3)  
3
mmho  
V/mV  
m
m
Transconductance Amplifier Gain  
= 1.2V; (g xZ ; No Ext Load); (Note 3)  
1.5  
mOL  
m
L
I
Input DC Supply Current  
Normal Mode  
Shutdown  
(Note 4)  
Q
EXTV Tied to V ; V  
= 5V  
470  
20  
µA  
µA  
CC  
OUT OUT  
V
V
V
V
= 0V  
40  
1.9  
4.0  
RUN/SS  
I
Soft-Start Charge Current  
RUN/SS Pin ON Threshold  
RUN/SS Pin Latchoff Arming  
RUN/SS Discharge Current  
= 1.9V  
–1.2  
1.5  
µA  
V
RUN/SS  
RUN/SS  
RUN/SS  
RUN/SS  
V
V
Rising  
1.0  
0.5  
RUN/SS  
RUN/SSLO  
SCL  
Rising from 3V  
4.1  
V
I
Soft Short Condition V  
= 0.5V;  
2.0  
µA  
EAIN  
V
= 4.5V  
RUN/SS  
2
LTC1929  
The denotes the specifications which apply over the full operating  
ELECTRICAL CHARACTERISTICS  
temperature range, otherwise specifications are at TA = 25°C. VIN = 15V, VRUN/SS = 5V unless otherwise noted.  
SYMBOL  
PARAMETER  
CONDITIONS  
= 0.5V  
MIN  
TYP  
1.6  
MAX  
UNITS  
µA  
I
I
Shutdown Latch Disable Current  
Total Sense Pins Source Current  
Maximum Duty Factor  
V
5
SDLHO  
SENSE  
EAIN  
Each Channel: V  
In Dropout  
– = V + + = 0V  
SENSE1 , 2  
60  
99.5  
µA  
SENSE1 , 2  
DF  
MAX  
98  
%
Top Gate Transition Time:  
Rise Time  
Fall Time  
TG1, 2 t  
TG1, 2 t  
C
C
= 3300pF  
= 3300pF  
30  
40  
90  
90  
ns  
ns  
r
f
LOAD  
LOAD  
Bottom Gate Transition Time:  
Rise Time  
Fall Time  
BG1, 2 t  
BG1, 2 t  
C
C
= 3300pF  
= 3300pF  
30  
20  
90  
90  
ns  
ns  
r
f
LOAD  
LOAD  
TG/BG t  
Top Gate Off to Bottom Gate On Delay  
Synchronous Switch-On Delay Time  
1D  
C
C
= 3300pF Each Driver  
= 3300pF Each Driver  
90  
90  
ns  
ns  
LOAD  
LOAD  
BG/TG t  
Bottom Gate Off to Top Gate On Delay  
Top Switch-On Delay Time  
2D  
Internal V Regulator  
CC  
V
V
V
V
V
Internal V Voltage  
6V < V < 30V; V = 4V  
EXTVCC  
4.8  
4.5  
5.0  
0.2  
120  
4.7  
0.2  
5.2  
1.0  
V
%
INTVCC  
CC  
IN  
INT  
INTV Load Regulation  
I
I
I
I
= 0 to 20mA; V  
= 4V  
EXTVCC  
LDO  
LDO  
CC  
CC  
CC  
CC  
CC  
EXT  
EXTV Voltage Drop  
= 20mA; V  
= 5V  
240  
mV  
V
CC  
EXTVCC  
EXTV Switchover Voltage  
= 20mA, EXTV Ramping Positive  
EXTVCC  
LDOHYS  
CC  
CC  
EXTV Switchover Hysteresis  
= 20mA, EXTV Ramping Negative  
V
CC  
CC  
Oscillator and Phase-Locked Loop  
f
f
f
Nominal Frequency  
Lowest Frequency  
Highest Frequency  
PLLIN Input Resistance  
V
V
V
= 1.2V  
= 0V  
200  
110  
270  
220  
140  
310  
50  
250  
170  
350  
kHz  
kHz  
kHz  
kΩ  
NOM  
LOW  
HIGH  
PLLFLTR  
PLLFLTR  
PLLFLTR  
2.4V  
R
PLLIN  
I
Phase Detector Output Current  
Sinking Capability  
Sourcing Capability  
PLLFLTR  
f
f
< f  
> f  
15  
15  
µA  
µA  
PLLIN  
PLLIN  
OSC  
OSC  
R
Controller 2-Controller 1 Phase  
180  
Deg  
RELPHS  
Differential Amplifier/Op Amp Gain Block (Note 5)  
A
Gain  
Differential Amp Mode  
Differential Amp Mode; 0V < V < 5V  
0.995  
46  
1
1.005  
V/V  
dB  
DA  
CMRR  
Common Mode Rejection Ratio  
Input Resistance  
Input Offset Voltage  
55  
80  
DA  
CM  
R
Differential Amp Mode; Measured at V + Input  
kΩ  
mV  
IN  
OS  
V
Op Amp Mode; V = 2.5V; V = 5V;  
DIFFOUT  
6
OS  
CM  
I
= 1mA  
DIFFOUT  
I
Input Bias Current  
Op Amp Mode  
30  
200  
nA  
V/mV  
V
B
A
V
Open Loop DC Gain  
Op Amp Mode; 0.7V V  
< 10V  
DIFFOUT  
5000  
OL  
Common Mode Input Voltage Range  
Common Mode Rejection Ratio  
Power Supply Rejection Ratio  
Maximum Output Current  
Maximum Output Voltage  
Gain-Bandwidth Product  
Slew Rate  
Op Amp Mode  
0
3
CM  
CMRR  
Op Amp Mode; 0V < V < 3V  
70  
70  
10  
10  
90  
90  
35  
11  
2
dB  
OA  
CM  
PSRR  
Op Amp Mode; 6V < V < 30V  
dB  
OA  
IN  
I
Op Amp Mode; V  
= 0V  
mA  
V
CL  
DIFFOUT  
DIFFOUT  
DIFFOUT  
V
Op Amp Mode; I  
Op Amp Mode; I  
= 1mA  
= 1mA  
O(MAX)  
GBW  
SR  
MHz  
V/µs  
Op Amp Mode; R = 2k  
5
L
3
LTC1929  
ELECTRICAL CHARACTERISTICS  
Note 1: Absolute Maximum Ratings are those values beyond which the  
Note 3: The LTC1929 is tested in a feedback loop that servos V to a  
ITH  
life of a device may be impaired.  
specified voltage and measures the resultant V  
.
EAIN  
Note 2: T is calculated from the ambient temperature T and power  
Note 4: Dynamic supply current is higher due to the gate charge being  
delivered at the switching frequency. See Applications Information.  
J
A
dissipation P according to the following formulas:  
D
LTC1929CG: T = T + (P • 95°C/W)  
Note 5: When the AMPMD pin is high, the IC pins are connected directly to  
the internal op amp inputs. When the AMPMD pin is low, internal MOSFET  
switches connect four 40k resistors around the op amp to create a  
standard unity-gain differential amp.  
J
A
D
U
U
U
PI FU CTIO S  
RUN/SS (Pin 1): Combination of Soft-Start, Run Control  
Input and Short-Circuit Detection Timer. A capacitor to  
groundatthispinsetstheramptimetofullcurrentoutput.  
Forcing this pin below 0.8V causes the IC to shut down all  
internal circuitry. All functions are disabled in shutdown.  
SENSE1+, SENSE2+ (Pins 2,14): The (+) Input to the  
Differential Current Comparators. The ITH pin voltage and  
built-in offsets between SENSEand SENSE+ pins in  
conjunction with RSENSE set the current trip threshold.  
SGND (Pin 9): Signal Ground, common to both control-  
lers, must be routed separately from the input switched  
current ground path to the common (–) terminal(s) of the  
COUT capacitor(s).  
VDIFFOUT (Pin 10): Output of a Differential Amplifier that  
provides true remote output voltage sensing. This pin  
normally drives an external resistive divider that sets the  
output voltage.  
VOS, VOS+ (Pins 11, 12): Inputs to an Operational Ampli-  
fier. Internal precision resistors capable of being elec-  
tronically switched in or out can configure it as a differen-  
tial amplifier or an uncommitted Op Amp.  
SENSE1, SENSE2(Pins 3, 13): The (–) Input to the  
Differential Current Comparators.  
EAIN (Pin 4): Input to the Error Amplifier that compares  
thefeedbackvoltagetotheinternal0.8Vreferencevoltage.  
This pin is normally connected to a resistive divider from  
the output of the differential amplifier (DIFFOUT).  
AMPMD (Pin 15): This Logic Input pin controls the  
connections of internal precision resistors that configure  
the operational amplifier as a unity-gain differential ampli-  
fier.  
PLLFLTR (Pin 5): The Phase-Locked Loop’s Low Pass  
Filter is tied to this pin. Alternatively, this pin can be driven  
with an AC or DC voltage source to vary the frequency of  
the internal oscillator.  
TG2, TG1 (Pins 16, 27): High Current Gate Drives for Top  
N-Channel MOSFETS. These are the outputs of floating  
drivers with a voltage swing equal to INTVCC superim-  
posed on the switch node voltage SW.  
PLLIN (Pin 6): External Synchronization Input to Phase  
Detector. This pin is internally terminated to SGND with  
50k. The phase-locked loop will force the rising top gate  
signal of controller 1 to be synchronized with the rising  
edge of the PLLIN signal.  
SW2, SW1 (Pins 17, 26): Switch Node Connections to  
Inductors. Voltage swing at these pins is from a Schottky  
diode (external) voltage drop below ground to VIN.  
BOOST2, BOOST1 (Pins 18, 25): Bootstrapped Supplies  
to the Topside Floating Drivers. Capacitors are connected  
between the Boost and Switch pins, and Schottky diodes  
are tied between the Boost and INTVCC pins.  
NC (Pins 7, 28): Not connected.  
ITH (Pin 8): Error Amplifier Output and Switching Regula-  
torCompensationPoint.Bothcurrentcomparator’sthresh-  
oldsincreasewiththiscontrolvoltage. Thenormalvoltage  
range of this pin is from 0V to 2.4V  
BG2, BG1 (Pins 19, 23): Voltage Swing High Current Gate  
Drives for Bottom Synchronous N-Channel MOSFETS.  
Voltage swing at these pins is from ground to INTVCC.  
4
LTC1929  
U
U
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PI FU CTIO S  
PGND(Pin20):DriverPowerGround.Connectstosources  
of bottom N-channel MOSFETS and the (–) terminals of  
CIN.  
EXTVCC (Pin 22): External Power Input to an Internal  
Switch . This switch closes and supplies INTVCC, bypass-  
ing the internallow dropout regulator whenever EXTVCC is  
higher than 4.7V. See EXTVCC Connection in the Applica-  
tions Information section. Do not exceed 7V on this pin  
INTVCC (Pin 21): Output of the Internal 5V Linear Low  
Dropout Regulator and the EXTVCC Switch. The driver and  
control circuits are powered from this voltage source.  
Decouple to power ground with a 1µF ceramic capacitor  
placed directly adjacent to the IC and minimum of 4.7µF  
additional tantalum or other low ESR capacitor.  
and ensure VEXTVCC VINTVCC  
.
VIN (Pin24):MainSupplyPin.Shouldbecloselydecoupled  
to the IC’s signal ground pin.  
U
U W  
FU CTIO AL DIAGRA  
PLLIN  
INTV  
V
IN  
CC  
PHASE DET  
F
IN  
50k  
PLLLPF  
D
C
DUPLICATE FOR  
SECOND CHANNEL  
B
BOOST  
TG  
R
C
LP  
B
DROP  
OUT  
DET  
+
CLK1  
CLK2  
TOP  
BOT  
C
IN  
LP  
OSCILLATOR  
BOT  
FORCE BOT  
SW  
S
R
Q
Q
SWITCH  
LOGIC  
INTV  
CC  
BG  
PGND  
+
V
V
OS  
SHDN  
A1  
+
OS  
INTV  
CC  
I1  
L
+
+
+
SENSE  
SENSE  
30k  
30k  
4(V  
FB  
)
C
OUT  
R
SENSE  
AMPMD  
DIFFOUT  
SLOPE  
COMP  
0V POSITION  
45k  
45k  
2.4V  
V
OUT  
EAIN  
R1  
V
FB  
+
EA  
OV  
V
0.8V  
REF  
0.80V  
0.86V  
V
IN  
R2  
V
IN  
+
+
4.7V  
5V  
LDO  
REG  
C
C
V
IN  
I
TH  
EXTV  
INTV  
CC  
1.2µA  
SHDN  
4(V  
RUN  
SOFT  
START  
R
C
CC  
5V  
)
FB  
+
6V  
RUN/SS  
INTERNAL  
SUPPLY  
SGND  
C
SS  
1929 FBD  
5
LTC1929  
U
(Refer to Functional Diagram)  
OPERATIO  
Main Control Loop  
Low Current Operation  
The LTC1929 uses a constant frequency, current mode  
step-down architecture with inherent current sharing.  
During normal operation, the top MOSFET is turned on  
each cycle when the oscillator sets the RS latch, and  
turned off when the main current comparator, I1, resets  
the RS latch. The peak inductor current at which I1 resets  
the RS latch is controlled by the voltage on the ITH pin,  
which is the output of the error amplifier EA. The differen-  
tialamplifier,A1,producesasignalequaltothedifferential  
voltage sensed across the output capacitor but re-refer-  
ences it to the internal signal ground (SGND) reference.  
The EAIN pin receives a portion of this voltage feedback  
signal at the DIFFOUT pin which is compared to the  
internalreferencevoltagebytheEA.Whentheloadcurrent  
increases, it causes a slight decrease in the EAIN pin  
voltagerelative to the 0.8V reference, which in turn causes  
the ITH voltage to increase until the average inductor  
current matches the new load current. After the top  
MOSFET has turned off, the bottom MOSFET is turned on  
for the rest of the period.  
The LTC1929 operates in a continuous, PWM control  
mode. The resulting operation at low output currents  
optimizes transient response at the expense of substantial  
negative inductor current during the latter part of the  
period. The level of ripple current is determined by the  
inductor value, input voltage, output voltage, and fre-  
quency of operation.  
Frequency Synchronization  
The phase-locked loop allows the internal oscillator to be  
synchronized to an external source via the PLLIN pin. The  
output of the phase detector at the PLLFLTR pin is also the  
DC frequency control input of the oscillator that operates  
over a 140kHz to 310kHz range corresponding to a DC  
voltageinputfrom0Vto2.4V.Whenlocked,thePLLaligns  
the turn on of the top MOSFET to the rising edge of the  
synchronizingsignal.WhenPLLINisleftopen,thePLLFLTR  
pingoeslow,forcingtheoscillatortominimumfrequency.  
InputcapacitanceESRrequirementsandefficiencylosses  
are substantially reduced because the peak current drawn  
from the input capacitor is effectively divided by two and  
power loss is proportional to the RMS current squared. A  
two stage, single output voltage implementation can re-  
duce input path power loss by 75% and radically reduce  
the required RMS current rating of the input capacitor(s).  
The top MOSFET drivers are biased from floating boot-  
strap capacitor CB, which normally is recharged during  
each off cycle through an external Schottky diode. When  
VIN decreasestoavoltageclosetoVOUT,however,theloop  
may enter dropout and attempt to turn on the top MOSFET  
continuously. A dropout detector detects this condition  
and forces the top MOSFET to turn off for about 400ns  
every 10th cycle to recharge the bootstrap capacitor.  
INTVCC/EXTVCC Power  
Power for the top and bottom MOSFET drivers and most  
of the IC circuitry is derived from INTVCC. When the  
EXTVCC pin is left open, an internal 5V low dropout  
regulator supplies INTVCC power. If the EXTVCC pin is  
taken above 4.7V, the 5V regulator is turned off and an  
internalswitchisturnedonconnectingEXTVCC toINTVCC.  
This allows the INTVCC power to be derived from a high  
efficiency external source such as the output of the regu-  
lator itself or a secondary winding, as described in the  
Applications Information section. An external Schottky  
diode can be used to minimize the voltage drop from  
EXTVCC to INTVCC in applications requiring greater than  
the specified INTVCC current. Voltages up to 7V can be  
applied to EXTVCC for additional gate drive capability.  
The main control loop is shut down by pulling Pin 1 (RUN/  
SS) low. Releasing RUN/SS allows an internal 1.2µA  
current source to charge soft-start capacitor CSS. When  
CSS reaches1.5V,themaincontrolloopisenabledwiththe  
ITH voltageclampedatapproximately30%ofitsmaximum  
value. As CSS continues to charge, ITH is gradually re-  
leased allowing normal operation to resume. When the  
RUN/SS pin is low, all LTC1929 functions are shut down.  
IfVOUT hasnotreached70%ofitsnominalvaluewhenCSS  
has charged to 4.1V, an overcurrent latchoff can be  
invoked as described in the Applications Information  
section.  
6
LTC1929  
U
(Refer to Functional Diagram)  
OPERATIO  
Differential Amplifier  
Short-Circuit Detection  
This amplifier provides true differential output voltage  
sensing. Sensing both VOUT+ and VOUTbenefits regula-  
tion in high current applications and/or applications hav-  
ing electrical interconnection losses. The AMPMD pin  
allows selection of internal, precision feedback resistors  
for high common mode rejection differencing applica-  
tions, or direct access to the actual amplifier inputs  
withouttheseinternalfeedbackresistorsforotherapplica-  
tions. The AMPMD pin is grounded to connect the internal  
precisionresistorsinaunity-gaindifferencingapplication,  
or tied to the INTVCC pin to bypass the internal resistors  
and make the amplifier inputs directly available. The  
amplifier is a unity-gain stable, 2MHz gain-bandwidth,  
>120dB open-loop gain design. The amplifier has an  
output slew rate of 5V/µs and is capable of driving capaci-  
tive loads with an output RMS current typically up to  
25mA. The amplifier is not capable of sinking current and  
therefore must be resistively loaded to do so.  
The RUN/SS capacitor is used initially to limit the inrush  
current from the input power source. Once the controllers  
have been given time, as determined by the capacitor on  
the RUN/SS pin, to charge up the output capacitors and  
provide full load current, the RUN/SS capacitor is then  
usedasashort-circuittimeoutcircuit.Iftheoutputvoltage  
falls to less than 70% of its nominal output voltage the  
RUN/SS capacitor begins discharging assuming that the  
output is in a severe overcurrent and/or short-circuit  
condition. If the condition lasts for a long enough period  
as determined by the size of the RUN/SS capacitor, the  
controller will be shut down until the RUN/SS pin voltage  
is recycled. This built-in latchoff can be overidden by  
providing a current >5µA at a compliance of 5V to the  
RUN/SS pin. This current shortens the soft-start period  
but also prevents net discharge of the RUN/SS capacitor  
during a severe overcurrent and/or short-circuit condi-  
tion.Foldbackcurrentlimitingisactivatedwhentheoutput  
voltage falls below 70% of its nominal level whether or not  
the short-circuit latchoff circuit is enabled.  
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ThebasicLTC1929applicationcircuitisshowninFigure 1  
on the first page. External component selection is driven  
by the load requirement, and begins with the selection of  
RSENSE1, 2. Once RSENSE1, 2 are known, L1 and L2 can be  
chosen. Next, the power MOSFETs and D1 and D2 are  
selected. The operating frequency and the inductor are  
chosen based mainly on the amount of ripple current.  
Finally, CIN is selected for its ability to handle the input  
ripple current (that PolyPhaseTM operation minimizes) and  
COUT is chosen with low enough ESR to meet the output  
ripplevoltageandloadstepspecifications(alsominimized  
with PolyPhase). Current mode architecture provides in-  
herent current sharing between output stages. The circuit  
showninFigure 1canbeconfiguredforoperationuptoan  
input voltage of 28V (limited by the external MOSFETs).  
mum threshold of 75mV/RSENSE and an input common  
mode range of SGND to 1.1( INTVCC). The current com-  
parator threshold sets the peak inductor current, yielding  
a maximum average output current IMAX equal to the peak  
value less half the peak-to-peak ripple current, IL.  
Allowing a margin for variations in the LTC1929 and  
external component values yields:  
R
SENSE = 2(50mV/IMAX  
)
Operating Frequency  
The LTC1929 uses a constant frequency, phase-lockable  
architecture with the frequency determined by an internal  
capacitor. This capacitor is charged by a fixed current plus  
an additional current which is proportional to the voltage  
applied to the PLLFLTR pin. Refer to Phase-Locked Loop  
and Frequency Synchronization in the Applications Infor-  
mation section for additional information.  
RSENSE Selection For Output Current  
RSENSE1, 2 are chosen based on the required output  
current. The LTC1929 current comparator has a maxi-  
PolyPhase is a registered trademark of Linear Technology Corporation.  
7
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A graph for the voltage applied to the PLLFLTR pin vs  
frequency is given in Figure 2. As the operating frequency  
isincreasedthegatechargelosseswillbehigher,reducing  
efficiency (see Efficiency Considerations). The maximum  
switching frequency is approximately 310kHz.  
In a 2-phase converter, the net ripple current seen by the  
output capacitor is much smaller than the individual  
inductor ripple currents due to the ripple cancellation. The  
details on how to calculate the net output ripple current  
can be found in Application Note 77.  
Figure 3 shows the net ripple current seen by the output  
capacitors for the 1- and 2-phase configurations. The  
outputripplecurrentisplottedforafixedoutputvoltageas  
the duty factor is varied between 10% and 90% on the  
x-axis. The output ripple current is normalized against the  
inductor ripple current at zero duty factor. The graph can  
be used in place of tedious calculations, simplifying the  
design process.  
2.5  
2.0  
1.5  
1.0  
0.5  
0
Accepting larger values of IL allows the use of low  
inductances, butcanresultinhigheroutputvoltageripple.  
A reasonable starting point for setting ripple current is IL  
=0.4(IOUT)/2,whereIOUT isthetotalloadcurrent.Remem-  
ber, the maximum IL occurs at the maximum input  
voltage. The individual inductor ripple currents are deter-  
mined by the inductor, input and output voltages.  
1.0  
120  
170  
220  
270  
320  
OPERATING FREQUENCY (kHz)  
1929 F02  
Figure 2. Operating Frequency vs VPLLFLTR  
Inductor Value Calculation and Output Ripple Current  
1-PHASE  
2-PHASE  
0.9  
0.8  
The operating frequency and inductor selection are inter-  
related in that higher operating frequencies allow the use  
of smaller inductor and capacitor values. So why would  
anyone ever choose to operate at lower frequencies with  
larger components? The answer is efficiency. A higher  
frequency generally results in lower efficiency because of  
MOSFET gate charge and transition losses. In addition to  
this basic tradeoff, the effect of inductor value on ripple  
current and low current operation must also be consid-  
ered. The PolyPhase approach reduces both input and  
output ripple currents while optimizing individual output  
stagestorunatalowerfundamentalfrequency,enhancing  
efficiency.  
0.7  
0.6  
0.5  
0.4  
0.3  
0.2  
0.1  
0
0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9  
DUTY FACTOR (V /V  
)
OUT IN  
1929 F03  
Figure 3. Normalized Output Ripple Current vs  
Duty Factor [IRMS 0.3 (IO(P–P))]  
Theinductorvaluehasadirecteffectonripplecurrent.The  
inductor ripple current IL per individual section, N,  
decreases with higher inductance or frequency and in-  
Inductor Core Selection  
Once the values for L1 and L2 are known, the type of  
inductor must be selected. High efficiency converters  
generally cannot afford the core loss found in low cost  
powdered iron cores, forcing the use of more expensive  
ferrite, molypermalloy, or Kool Mµ® cores. Actual core  
loss is independent of core size for a fixed inductor value,  
creases with higher VIN or VOUT  
:
VOUT  
fL  
VOUT  
V
IN  
IL =  
1−  
where f is the individual output stage operating frequency.  
Kool Mµ is a registered trademark of Magnetics, Inc.  
8
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but it is very dependent on inductance selected. As induc-  
tance increases, core losses go down. Unfortunately,  
increased inductance requires more turns of wire and  
therefore copper losses will increase.  
VOUT  
V
IN  
Main SwitchDuty Cycle =  
V – VOUT  
IN  
Synchronous SwitchDuty Cycle =  
Ferrite designs have very low core loss and are preferred  
at high switching frequencies, so design goals can con-  
centrate on copper loss and preventing saturation. Ferrite  
core material saturates “hard,” which means that induc-  
tance collapses abruptly when the peak design current is  
exceeded. This results in an abrupt increase in inductor  
ripple current and consequent output voltage ripple. Do  
not allow the core to saturate!  
V
IN  
The MOSFET power dissipations at maximum output  
current are given by:  
2
VOUT IMAX  
PMAIN  
=
1+ δ RDS(ON)  
+
(
)
V
IN  
2
Molypermalloy (from Magnetics, Inc.) is a very good, low  
losscorematerialfortoroids,butitismoreexpensivethan  
ferrite. A reasonable compromise from the same manu-  
facturer is Kool Mµ. Toroids are very space efficient,  
especially when you can use several layers of wire. Be-  
cause they lack a bobbin, mounting is more difficult.  
However, designs for surface mount are available which  
do not increase the height significantly.  
2
)
IMAX  
2
k V  
CRSS  
f
(
IN  
(
)( )  
2
V – VOUT IMAX  
IN  
PSYNC  
=
1+ δ RDS(ON)  
(
)
V
IN  
2
where δ is the temperature dependency of RDS(ON) and k  
is a constant inversely related to the gate drive current.  
Power MOSFET, D1 and D2 Selection  
Both MOSFETs have I2R losses but the topside N-channel  
equation includes an additional term for transition losses,  
which peak at the highest input voltage. For VIN < 20V the  
high current efficiency generally improves with larger  
MOSFETs, while for VIN > 20V the transition losses rapidly  
increasetothepointthattheuseofahigherRDS(ON)device  
with lower CRSS actual provides higher efficiency. The  
synchronous MOSFET losses are greatest at high input  
voltage when the top switch duty factor is low or during a  
short-circuit when the synchronous switch is on close to  
100% of the period.  
Two external power MOSFETs must be selected for each  
controller with the LTC1929: One N-channel MOSFET for  
the top (main) switch, and one N-channel MOSFET for the  
bottom (synchronous) switch.  
The peak-to-peak drive levels are set by the INTVCC volt-  
age. This voltage is typically 5V during start-up (see  
EXTVCC PinConnection).Consequently,logic-levelthresh-  
old MOSFETs must be used in most applications. The only  
exception is if low input voltage is expected (VIN < 5V);  
then, sublogic-level threshold MOSFETs (VGS(TH) < 3V)  
should be used. Pay close attention to the BVDSS specifi-  
cation for the MOSFETs as well; most of the logic-level  
MOSFETs are limited to 30V or less.  
The term (1 + δ) is generally given for a MOSFET in the  
form of a normalized RDS(ON) vs. Temperature curve, but  
δ = 0.005/°C can be used as an approximation for low  
voltage MOSFETs. CRSS is usually specified in the MOS-  
FET characteristics. The constant k = 1.7 can be used to  
estimate the contributions of the two terms in the main  
switch dissipation equation.  
SelectioncriteriaforthepowerMOSFETsincludetheON”  
resistance RDS(ON), reverse transfer capacitance CRSS  
,
input voltage, and maximum output current. When the  
LTC1929isoperatingincontinuousmodethedutyfactors  
for the top and bottom MOSFETs of each output stage are  
given by:  
TheSchottkydiodes,D1andD2showninFigure1conduct  
during the dead-time between the conduction of the two  
large power MOSFETs. This helps prevent the body diode  
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LTC1929  
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of the bottom MOSFET from turning on, storing charge  
during the dead-time, and requiring a reverse recovery  
periodwhichwouldreduceefficiency. A1Ato3A(depend-  
ing on output current) Schottky diode is generally a good  
compromise for both regions of operation due to the  
relatively small average current. Larger diodes result in  
additional transition losses due to their larger junction  
capacitance.  
These worst-case conditions are commonly used for  
design because even significant deviations do not offer  
much relief. Note that capacitor manufacturer’s ripple  
current ratings are often based on only 2000 hours of life.  
This makes it advisable to further derate the capacitor, or  
to choose a capacitor rated at a higher temperature than  
required. Several capacitors may also be paralleled to  
meet size or height requirements in the design. Always  
consult the capacitor manufacturer if there is any ques-  
tion.  
CIN and COUT Selection  
In continuous mode, the source current of each top  
It is important to note that the efficiency loss is propor-  
tional to the input RMS current squared and therefore a  
2-stage implementation results in 75% less power loss  
when compared to a single phase design. Battery/input  
protection fuse resistance (if used), PC board trace and  
connector resistance losses are also reduced by the re-  
ductionoftheinputripplecurrentina2-phasesystem.The  
requiredamountofinputcapacitanceisfurtherreducedby  
the factor, 2, due to the effective increase in the frequency  
of the current pulses.  
N-channel MOSFET is a square wave of duty cycle VOUT  
/
VIN. A low ESR input capacitor sized for the maximum  
RMS current must be used. The details of a close form  
equation can be found in Application Note 77. Figure 4  
shows the input capacitor ripple current for a 2-phase  
configuration with the output voltage fixed and input  
voltage varied. The input ripple current is normalized  
against the DC output current. The graph can be used in  
place of tedious calculations. The minimum input ripple  
currentcanbeachievedwhentheinputvoltageistwicethe  
output voltage. The minimum is not quite zero due to  
inductor ripple current.  
The selection of COUT is driven by the required effective  
series resistance (ESR). Typically once the ESR require-  
ment has been met, the RMS current rating generally far  
exceeds the IRIPPLE(P-P) requirements. The steady state  
output ripple (VOUT) is determined by:  
In the graph of Figure 4, the local maximum input RMS  
capacitor currents are reached when:  
VOUT 2k 1  
1
=
where k = 1, 2.  
VOUT ≈ ∆IRIPPLE ESR +  
V
4
IN  
16fCOUT  
Where f = operating frequency of each stage, COUT  
=
0.6  
0.5  
0.4  
0.3  
0.2  
0.1  
0
output capacitance and IRIPPLE = combined inductor  
ripple currents.  
The output ripple varies with input voltage since IL is a  
functionofinputvoltage.Theoutputripplewillbelessthan  
50mV at max VIN with IL = 0.4IOUT(MAX)/2 assuming:  
1-PHASE  
2-PHASE  
COUT required ESR < 4(RSENSE) and  
COUT > 1/(16f)(RSENSE  
)
The emergence of very low ESR capacitors in small,  
surface mount packages makes very physically small  
implementations possible. The ability to externally com-  
pensatetheswitchingregulatorloopusingtheITHpin(OPTI-  
LOOP compensation) allows a much wider selection of  
0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9  
DUTY FACTOR (V /V  
)
OUT IN  
1929 F04  
Figure 4. Normalized RMS Input Ripple Current vs  
Duty Factor for 1 and 2 Output Stages  
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output capacitor types. OPTI-LOOP compensation effec-  
tively removes constraints on output capacitor ESR. The  
impedance characteristics of each capacitor type are sig-  
nificantly different than an ideal capacitor and therefore  
require accurate modeling or bench evaluation during  
design.  
High input voltage applications in which large MOSFETs  
are being driven at high frequencies may cause the maxi-  
mum junction temperature rating for the LTC1929 to be  
exceeded. The supply current is dominated by the gate  
charge supply current, in addition to the current drawn  
from the differential amplifier output. The gate charge is  
dependent on operating frequency as discussed in the  
Efficiency Considerations section. The supply current can  
either be supplied by the internal 5V regulator or via the  
EXTVCC pin. When the voltage applied to the EXTVCC pin  
is less than 4.7V, all of the INTVCC load current is supplied  
by the internal 5V linear regulator. Power dissipation for  
the IC is higher in this case by (IIN)(VIN – INTVCC) and  
efficiency is lowered. The junction temperature can be  
estimated by using the equations given in Note 1 of the  
Electrical Characteristics. For example, the LTC1929 VIN  
current is limited to less than 24mA from a 24V supply:  
Manufacturers such as Nichicon, United Chemicon and  
Sanyoshouldbeconsideredforhighperformancethrough-  
hole capacitors. The OS-CON semiconductor dielectric  
capacitor available from Sanyo and the Panasonic SP  
surface mount types have the lowest (ESR)(size) product  
of any aluminum electrolytic at a somewhat higher price.  
An additional ceramic capacitor in parallel with OS-CON  
type capacitors is recommended to reduce the inductance  
effects.  
In surface mount applications, multiple capacitors may  
have to be paralleled to meet the ESR or RMS current  
handling requirements of the application. Aluminum elec-  
trolytic and dry tantalum capacitors are both available in  
surface mount configurations. New special polymer sur-  
face mount capacitors offer very low ESR also but have  
muchlowercapacitivedensityperunitvolume. Inthecase  
oftantalum,itiscriticalthatthecapacitorsaresurgetested  
for use in switching power supplies. Several excellent  
choices are the AVX TPS, AVX TPSV or the KEMET T510  
seriesofsurfacemounttantalums,availableincaseheights  
ranging from 2mm to 4mm. Other capacitor types include  
Sanyo OS-CON, Nichicon PL series and Sprague 595D  
series. Consultthemanufacturerforotherspecificrecom-  
mendations. A combination of capacitors will often result  
in maximizing performance and minimizing overall cost  
and size.  
TJ = 70°C + (24mA)(24V)(95°C/W) = 125°C  
Use of the EXTVCC pin reduces the junction temperature  
to:  
TJ = 70°C + (24mA)(5V)(95°C/W) = 81.4°C  
The input supply current should be measured while the  
controller is operating in continuous mode at maximum  
VIN and the power dissipation calculated in order to pre-  
vent the maximum junction temperature from being ex-  
ceeded.  
EXTVCC Connection  
The LTC1929 contains an internal P-channel MOSFET  
switch connected between the EXTVCC and INTVCC pins.  
When the voltage applied to EXTVCC rises above 4.7V, the  
internal regulator is turned off and the switch closes,  
connecting the EXTVCC pin to the INTVCC pin thereby  
supplying internal and MOSFET gate driving power. The  
switch remains closed as long as the voltage applied to  
EXTVCC remains above 4.5V. This allows the MOSFET  
driver and control power to be derived from the output  
during normal operation (4.7V < VEXTVCC < 7V) and from  
the internal regulator when the output is out of regulation  
(start-up, short-circuit). Do not apply greater than 7V to  
the EXTVCC pin and ensure that EXTVCC < VIN + 0.3V when  
using the application circuits shown.If an external voltage  
source is applied to the EXTVCC pin when the VIN supply is  
INTVCC Regulator  
An internal P-channel low dropout regulator produces 5V  
at the INTVCC pin from the VIN supply pin. The INTVCC  
regulator powers the drivers and internal circuitry of the  
LTC1929.TheINTVCC pinregulatorcansupplyupto50mA  
peak and must be bypassed to power ground with a  
minimum of 4.7µF tantalum or electrolytic capacitor. An  
additional 1µF ceramic capacitor placed very close to the  
IC is recommended due to the extremely high instanta-  
neous currents required by the MOSFET gate drivers.  
11  
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not present, a diode can be placed in series with the  
LTC1929’s VIN pin and a Schottky diode between the  
EXTVCCandtheVINpin,topreventcurrentfrombackfeeding  
VIN.  
inductive boost winding as shown in Figure 5a or the  
capacitive charge pump shown in Figure 5b. The charge  
pump has the advantage of simple magnetics.  
Topside MOSFET Driver Supply (CB,DB) (Refer to  
Functional Diagram)  
Significant efficiency gains can be realized by powering  
INTVCC from the output, since the VIN current resulting  
from the driver and control currents will be scaled by the  
ratio: (Duty Factor)/(Efficiency). For 5V regulators this  
means connecting the EXTVCC pin directly to VOUT. How-  
ever, for 3.3V and other lower voltage regulators, addi-  
tionalcircuitryisrequiredtoderiveINTVCC powerfromthe  
output.  
External bootstrap capacitors CB1 and CB2 connected to  
the BOOST1 and BOOST2 pins supply the gate drive  
voltages for the topside MOSFETs. Capacitor CB in the  
Functional Diagram is charged though diode DB from  
INTVCC whentheSWpinislow.WhenthetopsideMOSFET  
turns on, the driver places the CB voltage across the gate-  
sourceofthedesiredMOSFET.ThisenhancestheMOSFET  
and turns on the topside switch. The switch node voltage,  
The following list summarizes the four possible connec-  
tions for EXTVCC:  
SW, rises to VIN and the BOOST pin rises to VIN + VINTVCC  
.
1. EXTVCC left open (or grounded). This will cause INTVCC  
to be powered from the internal 5V regulator resulting in  
a significant efficiency penalty at high input voltages.  
The value of the boost capacitor CB needs to be 30 to 100  
times that of the total input capacitance of the topside  
MOSFET(s). ThereversebreakdownofDB mustbegreater  
than VIN(MAX).  
2. EXTVCC connected directly to VOUT. This is the normal  
connection for a 5V regulator and provides the highest  
efficiency.  
The final arbiter when defining the best gate drive ampli-  
tude level will be the input supply current. If a change is  
made that decreases input current, the efficiency has  
improved. If the input current does not change then the  
efficiency has not changed either.  
3. EXTVCC connected to an external supply. If an external  
supply is available in the 5V to 7V range, it may be used to  
powerEXTVCC providingitiscompatiblewiththeMOSFET  
gate drive requirements.  
Output Voltage  
4. EXTVCC connected to an output-derived boost network.  
For 3.3V and other low voltage regulators, efficiency gains  
can still be realized by connecting EXTVCC to an output-  
derived voltage which has been boosted to greater than  
4.7V but less than 7V. This can be done with either the  
The LTC1929 has a true remote voltage sense capablity.  
Thesensingconnectionsshouldbereturnedfromtheload  
back to the differential amplifier’s inputs through a com-  
mon, tightly coupled pair of PC traces. The differential  
+
OPTIONAL EXTV CONNECTION  
CC  
V
IN  
+
5V < V  
< 7V  
V
SEC  
+
C
IN  
IN  
C
IN  
V
IN  
BAT85  
0.22µF  
BAT85  
BAT85  
V
LTC1929  
IN  
1N4148  
V
TG1  
SEC  
TG1  
+
LTC1929  
N-CH  
VN2222LL  
R
1µF  
EXTV  
CC  
N-CH  
EXTV  
CC  
R
SENSE  
SENSE  
V
OUT  
V
SW1  
BG1  
SW1  
BG1  
OUT  
L1  
T1  
+
+
C
C
OUT  
OUT  
N-CH  
N-CH  
PGND  
PGND  
1929 F05b  
1929 F05a  
Figure 5a. Secondary Output Loop with EXTVCC Connection  
Figure 5b. Capacitive Charge Pump for EXTVCC  
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amplifier rejects common mode signals capacitively or  
inductively radiated into the feedback PC traces as well as  
ground loop disturbances. The differential amplifier out-  
put signal is divided down and compared with the internal  
precision 0.8V voltage reference by the error amplifier.  
required from the input power supply. If RUN/SS has been  
pulled all the way to ground there is a delay before starting  
of approximately:  
1.5V  
1.2µA  
tDELAY  
=
C
SS = 1.25s / µF CSS  
(
)
The differential amplifier can be used in either of two  
configurations according to the voltage applied to the  
AMPMD pin. The first configuration, with the connections  
illustrated in the Functional Diagram, utilizes a set of  
internalprecisionresistorstoenableprecisioninstrumen-  
tation-type measurement of the output voltage. This con-  
figuration is activated when the AMPMD pin is tied to  
ground. When the AMPMD pin is tied to INTVCC, the  
resistors are disconnected and the amplifier inputs are  
made directly available. The amplifier can then be used as  
a general purpose op amp. The amplifier has a 0V to 3V  
common mode input range limitation due to the internal  
switching of its inputs. The output is an NPN emitter  
follower without any internal pull-down current. A DC  
resistiveloadtogroundisrequiredinordertosinkcurrent.  
Theoutputwillswingfrom0Vto10V(VIN VDIFFOUT +2V).  
The time for the output current to ramp up is then:  
3V 1.5V  
1.2µA  
tIRAMP  
=
C
SS = 1.25s / µF CSS  
(
)
By pulling both RUN/SS controller pins below 0.8V the  
LTC1929isputintolowcurrentshutdown(IQ <40µA).The  
RUN/SS pins can be driven directly from logic as shown in  
Figure 6. Diode D1 in Figure 6 reduces the start delay but  
allows CSS to ramp up slowly providing the soft-start  
function. The RUN/SS pin has an internal 6V zener clamp  
(see Functional Diagram).  
Fault Conditions: Overcurrent Latchoff  
The RUN/SS pin also provides the ability to latch off the  
controllerswhenanovercurrentconditionisdetected.The  
RUN/SS capacitor, CSS, is used initially to limit the inrush  
current of both controllers. After the controllers have been  
started and been given adequate time to charge up the  
output capacitors and provide full load current, the RUN/  
SS capacitor is used for a short-circuit timer. If the output  
voltage falls to less than 70% of its nominal value, after  
CSS reaches 4.1V, CSS begins discharging on the assump-  
tion that the output is in an overcurrent condition. If the  
condition lasts for a long enough period as determined by  
the size of CSS, the controller will be shut down until the  
RUN/SS pin voltage is recycled. If the overload occurs  
during start-up, the time can be approximated by:  
Soft-Start/Run Function  
The RUN/SS pin provides three functions: 1) Run/Shut-  
down,2)soft-startand3)adefeatableshort-circuitlatchoff  
timer. Soft-start reduces the input power sources’ surge  
currents by gradually increasing the controller’s current  
limit ITH(MAX). The latchoff timer prevents very short,  
extreme load transients from tripping the overcurrent  
latch. A small pull-up current (>5µA) supplied to the RUN/  
SS pin will prevent the overcurrent latch from operating.  
The following explanation describes how the functions  
operate.  
An internal 1.2µA current source charges up the CSS  
capacitor. When the voltage on RUN/SS reaches 1.5V, the  
controllerispermittedtostartoperating.Asthevoltageon  
RUN/SS increases from 1.5V to 3.0V, the internal current  
T
LO1 (CSS • 0.6V)/(1.2µA) = 5 • 105 (CSS)  
If the overload occurs after start-up the voltage on the  
RUN/SS capacitor will continue charging and will provide  
additional time before latching off:  
limit is increased from 25mV/RSENSE to 75mV/RSENSE  
.
The output current limit ramps up slowly, taking an  
additional 1.4s/µF to reach full current. The output current  
thus ramps up slowly, reducing the starting surge current  
T
LO2 (CSS • 3V)/(1.2µA) = 2.5 • 106 (CSS)  
13  
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This built-in overcurrent latchoff can be overridden by  
providing a pull-up resistor, RSS, to the RUN/SS pin as  
shown in Figure 6. This resistance shortens the soft-start  
period and prevents the discharge of the RUN/SS capaci-  
tor during a severe overcurrent and/or short-circuit con-  
dition. When deriving the 5µA current from VIN as in the  
figure, current latchoff is always defeated. The diode  
connecting of this pull-up resistor to INTVCC, as in  
Figure 6, eliminates any extra supply current during shut-  
down while eliminating the INTVCC loading from prevent-  
ing controller start-up.  
Phase-Locked Loop and Frequency Synchronization  
The LTC1929 has a phase-locked loop comprised of an  
internal voltage controlled oscillator and phase detector.  
This allows the top MOSFET turn-on to be locked to the  
rising edge of an external source. The frequency range of  
the voltage controlled oscillator is ±50% around the  
center frequency fO. A voltage applied to the PLLFLTR pin  
of 1.2V corresponds to a frequency of approximately  
220kHz. The nominal operating frequency range of the  
LTC1929 is 140kHz to 310kHz.  
The phase detector used is an edge sensitive digital type  
which provides zero degrees phase shift between the  
external and internal oscillators. This type of phase detec-  
tor will not lock up on input frequencies close to the  
harmonics of the VCO center frequency. The PLL hold-in  
range, fH, is equal to the capture range, fC:  
Why should you defeat current latchoff? During the  
prototypingstageofadesign,theremaybeaproblemwith  
noise pickup or poor layout causing the protection circuit  
to latch off the controller. Defeating this feature allows  
troubleshooting of the circuit and PC layout. The internal  
short-circuit and foldback current limiting still remains  
active, thereby protecting the power supply system from  
failure. A decision can be made after the design is com-  
plete whether to rely solely on foldback current limiting or  
to enable the latchoff feature by removing the pull-up  
resistor.  
fH = fC = ±0.5 fO (150kHz-300kHz)  
The output of the phase detector is a complementary pair  
of current sources charging or discharging the external  
filter network on the PLLFLTR pin. A simplified block  
diagram is shown in Figure 7.  
The value of the soft-start capacitor CSS may need to be  
scaled with output voltage, output capacitance and load  
current characteristics. The minimum soft-start capaci-  
tance is given by:  
If the external frequency (fPLLIN) is greater than the oscil-  
lator frequency f0SC, current is sourced continuously,  
pulling up the PLLFLTR pin. When the external frequency  
is less than f0SC, current is sunk continuously, pulling  
down the PLLFLTR pin. If the external and internal fre-  
quencies are the same but exhibit a phase difference, the  
currentsourcesturnonforanamountoftimecorrespond-  
ing to the phase difference. Thus the voltage on the  
PLLFLTR pin is adjusted until the phase and frequency of  
the external and internal oscillators are identical. At this  
stable operating point the phase comparator output is  
open and the filter capacitor CLP holds the voltage. The  
LTC1929 PLLIN pin must be driven from a low impedance  
source such as a logic gate located close to the pin.  
CSS > (COUT )(VOUT)(10-4)(RSENSE  
)
The minimum recommended soft-start capacitor of CSS  
0.1µF will be sufficient for most applications.  
=
V
INTV  
IN  
CC  
R
3.3V OR 5V  
RUN/SS  
*
R
*
SS  
SS  
D1  
RUN/SS  
D1*  
C
SS  
The loop filter components (CLP, RLP) smooth out the  
current pulses from the phase detector and provide a  
stable input to the voltage controlled oscillator. The filter  
components CLP and RLP determine how fast the loop  
acquires lock. Typically RLP =10kand CLP is 0.01µF to  
0.1µF.  
C
SS  
*OPTIONAL TO DEFEAT OVERCURRENT LATCHOFF  
1929 F06  
Figure 6. RUN/SS Pin Interfacing  
14  
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If an application can operate close to the minimum on-  
time limit, an inductor must be chosen that has a low  
enough inductance to provide sufficient ripple amplitude  
to meet the minimum on-time requirement. As a general  
rule, keep the inductor ripple current of each phase equal  
2.4V  
R
LP  
10k  
PHASE  
DETECTOR  
C
LP  
EXTERNAL  
OSC  
PLLFLTR  
PLLIN  
DIGITAL  
PHASE/  
FREQUENCY  
DETECTOR  
to or greater than 15% of IOUT(MAX) at VIN(MAX)  
.
OSC  
50k  
Efficiency Considerations  
The percent efficiency of a switching regulator is equal to  
the output power divided by the input power times 100%.  
It is often useful to analyze individual losses to determine  
what is limiting the efficiency and which change would  
produce the most improvement. Percent efficiency can be  
expressed as:  
1929 F07  
Figure 7. Phase-Locked Loop Block Diagram  
Minimum On-Time Considerations  
%Efficiency = 100% – (L1 + L2 + L3 + ...)  
Minimum on-time tON(MIN) is the smallest time duration  
thattheLTC1929iscapableofturningonthetopMOSFET.  
It is determined by internal timing delays and the gate  
chargerequiredtoturnonthetopMOSFET.Lowdutycycle  
applications may approach this minimum on-time limit  
and care should be taken to ensure that  
whereL1, L2, etc. aretheindividuallossesasapercentage  
of input power.  
Although all dissipative elements in the circuit produce  
losses, four main sources usually account for most of the  
losses in LTC1929 circuits: 1) LTC1929 VIN current (in-  
cluding loading on the differential amplifier output),  
2) INTVCC regulator current, 3) I2R losses and 4) Topside  
MOSFET transition losses.  
VOUT  
tON MIN  
<
(
)
V f  
IN( )  
1) The VIN current has two components: the first is the  
DC supply current given in the Electrical Characteristics  
table, which excludes MOSFET driver and control cur-  
rents; the second is the current drawn from the differential  
amplifier output. VIN current typically results in a small  
(<0.1%) loss.  
Ifthedutycyclefallsbelowwhatcanbeaccommodatedby  
the minimum on-time, the LTC1929 will begin to skip  
cycles resulting in nonconstant frequency operation. The  
output voltage will continue to be regulated, but the ripple  
current and ripple voltage will increase.  
The minimum on-time for the LTC1929 is generally less  
than200ns.However,asthepeaksensevoltagedecreases  
the minimum on-time gradually increases. This is of  
particular concern in forced continuous applications with  
low ripple current at light loads. If the duty cycle drops  
below the minimum on-time limit in this situation, a  
significant amount of cycle skipping can occur with corre-  
spondingly larger current and voltage ripple.  
2) INTVCC current is the sum of the MOSFET driver and  
control currents. The MOSFET driver current results from  
switching the gate capacitance of the power MOSFETs.  
Each time a MOSFET gate is switched from low to high to  
low again, a packet of charge dQ moves from INTVCC to  
ground. The resulting dQ/dt is a current out of INTVCC that  
is typically much larger than the control circuit current. In  
continuous mode, IGATECHG = (QT + QB), where QT and QB  
are the gate charges of the topside and bottom side  
MOSFETs.  
15  
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SupplyingINTVCC powerthroughtheEXTVCC switchinput  
from an output-derived source will scale the VIN current  
required for the driver and control circuits by the ratio  
(Duty Factor)/(Efficiency). For example, in a 20V to 5V  
application, 10mA of INTVCC current results in approxi-  
mately 3mA of VIN current. This reduces the mid-current  
loss from 10% or more (if the driver was powered directly  
from VIN) to only a few percent.  
minimum of 20µF to 40µF of capacitance having a maxi-  
mum of 10mto 20mof ESR. The LTC1929 2-phase  
architecture typically halves this input capacitance re-  
quirement over competing solutions. Other losses includ-  
ing Schottky conduction losses during dead-time and  
inductor core losses generally account for less than 2%  
total additional loss.  
Checking Transient Response  
3) I2R losses are predicted from the DC resistances of the  
fuse (if used), MOSFET, inductor, current sense resistor,  
and input and output capacitor ESR. In continuous mode  
The regulator loop response can be checked by looking at  
the load transient response. Switching regulators take  
several cycles to respond to a step in DC (resistive) load  
current. When a load step occurs, VOUT shifts by an  
amount equal to ILOAD(ESR), where ESR is the effective  
seriesresistanceofCOUT(ILOAD)alsobeginstochargeor  
discharge COUT generating the feedback error signal that  
forces the regulator to adapt to the current change and  
return VOUT to its steady-state value. During this recovery  
time VOUT can be monitored for excessive overshoot or  
ringing, which would indicate a stability problem. The  
availability of the ITH pin not only allows optimization of  
control loop behavior but also provides a DC coupled and  
AC filtered closed loop response test point. The DC step,  
rise time, and settling at this test point truly reflects the  
closed loop response. Assuming a predominantly second  
order system, phase margin and/or damping factor can be  
estimated using the percentage of overshoot seen at this  
pin. The bandwidth can also be estimated by examining  
the rise time at the pin. The ITH external components  
shown in the Figure 1 circuit will provide an adequate  
starting point for most applications.  
the average output current flows through L and RSENSE  
,
but is “chopped” between the topside MOSFET and the  
synchronous MOSFET. If the two MOSFETs have approxi-  
mately the same RDS(ON), then the resistance of one  
MOSFET can simply be summed with the resistances of L,  
RSENSE and ESR to obtain I2R losses. For example, if each  
RDS(ON)=10m, RL=10m, and RSENSE=5m, then the  
total resistance is 25m. This results in losses ranging  
from 2% to 8% as the output current increases from 3A to  
15A per output stage for a 5V output, or a 3% to 12% loss  
per output stage for a 3.3V output. Efficiency varies as the  
inverse square of VOUT for the same external components  
and output power level. The combined effects of increas-  
ingly lower output voltages and higher currents required  
by high performance digital systems is not doubling but  
quadrupling the importance of loss terms in the switching  
regulator system!  
4) Transition losses apply only to the topside MOSFET(s),  
and only when operating at high input voltages (typically  
20V or greater). Transition losses can be estimated from:  
The ITH series RC-CC filter sets the dominant pole-zero  
loop compensation. The values can be modified slightly  
(from 0.2 to 5 times their suggested values) to maximize  
transient response once the final PC layout is done and the  
particular output capacitor type and value have been  
determined. The output capacitors need to be decided  
upon because the various types and values determine the  
loop feedback factor gain and phase. An output current  
pulse of 20% to 80% of full-load current having a rise time  
of<2µswillproduceoutputvoltageandITH pinwaveforms  
2
Transition Loss = (1.7) VIN IO(MAX) CRSS  
f
Other “hidden” losses such as copper trace and internal  
battery resistances can account for an additional 5% to  
10% efficiency degradation in portable systems. It is very  
important to include these “system” level losses in the  
design of a system. The internal battery and input fuse  
resistance losses can be minimized by making sure that  
CIN has adequate charge storage and a very low ESR at the  
switching frequency. A 25W supply will typically require a  
16  
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that will give a sense of the overall loop stability without  
breaking the feedback loop. The initial output voltage step  
resulting from the step change in output current may not  
bewithinthebandwidthofthefeedbackloop,sothissignal  
cannot be used to determine phase margin. This is why it  
isbettertolookattheIthpinsignalwhichisinthefeedback  
loop and is the filtered and compensated control loop  
response. The gain of the loop will be increased by  
increasing RC and the bandwidth of the loop will be  
increased by decreasing CC. If RC is increased by the same  
factor that CC is decreased, the zero frequency will be kept  
the same, thereby keeping the phase the same in the most  
critical frequency range of the feedback loop. The output  
voltage settling behavior is related to the stability of the  
closed-loop system and will demonstrate the actual over-  
all supply performance.  
Automotive Considerations: Plugging into the  
Cigarette Lighter  
As battery-powered devices go mobile, there is a natural  
interest in plugging into the cigarette lighter in order to  
conserveorevenrechargebatterypacksduringoperation.  
But before you connect, be advised: you are plugging into  
the supply from hell. The main battery line in an automo-  
bileisthesourceofanumberofnastypotentialtransients,  
including load-dump, reverse-battery, and double-bat-  
tery.  
Load-dump is the result of a loose battery cable. When the  
cablebreaksconnection,thefieldcollapseinthealternator  
can cause a positive spike as high as 60V which takes  
several hundred milliseconds to decay. Reverse-battery is  
just what it says, while double-battery is a consequence of  
tow truck operators finding that a 24V jump start cranks  
cold engines faster than 12V.  
A second, more severe transient is caused by switching in  
loads with large (>1µF) supply bypass capacitors. The  
dischargedbypasscapacitorsareeffectivelyputinparallel  
with COUT, causing a rapid drop in VOUT. No regulator can  
alter its delivery of current quickly enough to prevent this  
sudden step change in output voltage if the load switch  
resistance is low and it is driven quickly. If the ratio of  
CLOAD to COUT is greater than1:50, the switch rise time  
should be controlled so that the load rise time is limited to  
approximately 25 • CLOAD. Thus a 10µF capacitor would  
require a 250µs rise time, limiting the charging current to  
about 200mA.  
ThenetworkshowninFigure8isthemoststraightforward  
approach to protect a DC/DC converter from the ravages  
of an automotive battery line. The series diode prevents  
current from flowing during reverse-battery, while the  
transient suppressor clamps the input voltage during  
load-dump. Note that the transient suppressor should not  
conduct during double-battery operation, but must still  
clamptheinputvoltagebelowbreakdownoftheconverter.  
AlthoughtheLT1929hasamaximuminputvoltageof36V,  
most applications will be limited to 30V by the MOSFET  
BVDSS  
.
50A I RATING  
PK  
V
IN  
12V  
LTC1929  
TRANSIENT VOLTAGE  
SUPPRESSOR  
GENERAL INSTRUMENT  
1.5KA24A  
1929 F08  
Figure 8. Automotive Application Protection  
17  
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Design Example (Using Two Phases)  
The power dissipation on the topside MOSFET can be  
easily estimated. Using a Siliconix Si4420DY for example;  
RDS(ON) = 0.013, CRSS = 300pF. At maximum input  
voltage with Tj (estimated) = 110°C at an elevated ambient  
temperature:  
Asadesignexample,assumeVIN=5V(nominal),VIN = 5.5V  
(max), VOUT =1.8V, IMAX =20A, TA =70°Candf = 310kHz,  
RSENSE1 and RSENSE2 can immediately be calculated:  
RSENSE1 = RSENSE2 = 50mV/10A = 0.005Ω  
2
If L1 = L2 = 2µH the actual value of the ripple current for  
1.8V  
5.5V  
PMAIN  
=
10 1+ 0.005 110°C 25°C  
( )  
(
)(  
)
]
[
each channel, the following equation is used:  
2
) (  
0.013Ω + 1.7 5.5V 10A 300pF  
VOUT  
fL  
VOUT  
V
IN  
(
)(  
)
IL =  
1−  
310kHz = 0.65W  
(
)
The highest value of the ripple current occurs at the  
maximum input voltage:  
The worst-case power disipated by the synchronous  
MOSFET under normal operating conditions at elevated  
ambient temperature and estimated 50°C junction tem-  
perature rise is:  
1.8  
1.8  
5.5  
IL =  
1−  
1.95A  
310kHz 2µH  
(
)(  
)
2
) (  
5.5V 1.8V  
The ripple current for each inductor is 20% at maximum  
output current which is conservative.  
PSYNC  
=
10A 1.48 0.013Ω  
(
)(  
)
5.5V  
= 1.29W  
Next verify the minimum on-time of 200ns is not violated.  
The minimum on-time occurs at maximum VIN:  
Ashort-circuittogroundwillresultinafoldedbackcurrent  
of:  
VOUT  
1.8V  
tON MIN  
=
=
1µs  
(
)
200ns 5.5V  
(
)
25mV  
0.005Ω  
1
2
V
f
5.5V 310kHz  
IN MAX  
(
(
)
)
ISC  
=
+
= 5.28A  
2µH  
Since the output voltage is below 2.4V the output resistive  
divider will need to be sized to not only set the output  
voltage but also to absorb the sense pin current for both  
channels.  
The worst-case power disipated by the synchronous  
MOSFET under short-circuit conditions at elevated ambi-  
ent temperature and estimated 50°C junction temperature  
rise is:  
20k  
2
VOUT  
2.4V VOUT  
R1MIN  
=
(
)
2
) (  
5.5V 1.8V  
5.5V  
= 360mW  
PSYNC  
=
5.28A 1.48 0.013Ω  
(
)(  
)
1.8V  
2.4V 1.8V  
= 10k  
= 30k  
which is much less than normal, full-load conditions.  
Incidentally, since the load no longer dissipates power in  
the shorted condition, total system power dissipation is  
decreased by over 99%.  
Choosing 1% resistors; R1=13.2k and R2=16.5k yields an  
output voltage of 1.80V.  
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The duty factors when the peak RMS input current occurs  
is at D = 0.25 and D = 0.75 according to Figure 4. Calculate  
the worst-case required RMS current rating at the input  
voltage that produces a duty cycle nearest to the peak.  
PC Board Layout Checklist  
When laying out the printed circuit board, the following  
checklist should be used to ensure proper operation of the  
LTC1929. These items are also illustrated graphically in  
the layout diagram of Figure 11. Check the following in  
your layout:  
CIN will require an RMS current rating of:  
1) Are the signal and power grounds segregated? The  
LTC1929 signal ground pin should return to the (–) plate  
of COUT separately. The power ground returns to the  
sources of the bottom N-channel MOSFETs, anodes of the  
Schottky diodes, and (–) plates of CIN, which should have  
as short lead lengths as possible.  
2) Does the LTC1929 VOS+ pin connect to the (+) plate(s)  
of COUT? Does the LTC1929 VOSpin connect to the (–)  
plate(s) of COUT? The resistive divider R1, R2 must be  
connected between the VDIFFOUT and signal ground and  
anyfeedforwardcapacitoracrossR1shouldbeascloseas  
possible to the LTC1929.  
1.8 1 1 1.8  
5.5 2 2 5.5 2  
1
CINrequiredIRMS = 20A  
(
)
= 4.76ARMS  
The output capacitor ripple current is calculated by using  
the inductor ripple already calculated for each inductor  
andmultiplyingbythefactorobtainedfromFigure 3along  
with the calculated duty factor. The output ripple in con-  
tinuous mode will be highest at the maximum input  
voltage since the duty factor is <50%. The maximum  
output current ripple is:  
3)AretheSENSEandSENSE+ leadsroutedtogetherwith  
minimum PC trace spacing? The filter capacitors between  
SENSE+ and SENSEpin pairs should be as close as  
possible to the LTC1929. Ensure accurate current sensing  
with Kelvin connections.  
VOUT  
fL  
VOUT 0.33  
ICOUT  
=
1−  
at 33%D.F.  
V
IN  
0.66  
1.8V  
1.8V  
10.54  
ICOUTMAX  
=
5.5V  
310kHz 2µH  
(
)(  
)
4) Do the (+) plates of CIN connect to the drains of the  
topside MOSFETs as closely as possible? This capacitor  
provides the AC current to the MOSFETs. Keep the input  
currentpathformedbytheinputcapacitor,topandbottom  
MOSFETs, and the Schottky diode on the same side of the  
PC board in a tight loop to minimize conducted and  
radiated EMI.  
= 0.97A  
V
OUTRIPPLE = 20m0.97A = 19.4mVRMS  
(
)
An alternate calculation just uses the equation for output  
ripple current at D = 1.8V/5.5 = 0.33:  
5) Is the INTVCC 1µF ceramic decoupling capacitor con-  
nectedcloselybetweenINTVCC andthepowergroundpin?  
This capacitor carries the MOSFET driver peak currents. A  
small value is used to allow placement immediately adja-  
cent to the IC.  
12 0.33 10.33  
2 1.8V  
(
) (  
)
(
)
IRIPPLE  
=
310kHz 2µH  
12 0.33 + 1  
(
)
(
)
= 0.99A  
V
OUTRIPPLE = 20m0.99A = 19.7mVRMS  
6) Keep the switching nodes, SW1 (SW2), away from  
sensitive small-signal nodes. Ideally the switch nodes  
should be placed at the furthest point from the LTC1929.  
(
)
7)Usealowimpedancesourcesuchasalogicgatetodrive  
the PLLIN pin and keep the lead as short as possible.  
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The diagram in Figure 9 illustrates all branch currents in a  
2-phase switching regulator. It becomes very clear after  
studying the current waveforms why it is critical to keep  
the high-switching-current paths to a small physical size.  
High electric and magnetic fields will radiate from these  
“loops” just as radio stations transmit signals. The output  
capacitor ground should return to the negative terminal of  
the input capacitor and not share a common ground path  
with any switched current paths. The left half of the circuit  
gives rise to the “noise” generated by a switching regula-  
tor. The ground terminations of the sychronous MOSFETs  
and Schottky diodes should return to the bottom plate(s)  
of the input capacitor(s) with a short isolated PC trace  
since very high switched currents are present. A separate  
isolated path from the bottom plate(s) of the input  
capacitor(s) should be used to tie in the IC power ground  
pin (PGND) and the signal ground pin (SGND). This  
technique keeps inherent signals generated by high cur-  
rent pulses from taking alternate current paths that have  
finite impedances during the total period of the switching  
regulator.ExternalOPTI-LOOPcompensationallowsover-  
compensation for PC layouts which are not optimized but  
this is not the recommended design procedure.  
RMS current is calculated, higher effective duty factor  
results and the peak current levels are divided as long as  
the currents in each stage are balanced. Refer to Applica-  
tion Note 19 for a detailed description of how to calculate  
RMS current for the single stage switching regulator.  
Figures 3 and 4 help to illustrate how the input and output  
currents are reduced by using an additional phase. The  
input current peaks drop in half and the frequency is  
doubled for this 2-phase converter. The input capacity  
requirement is thus reduced theoretically by a factor of  
four! Ceramic input capacitors with their unbeatably low  
ESR characteristics can be used.  
Figure 4 illustrates the RMS input current drawn from the  
input capacitance vs the duty cycle as determined by the  
ratio of input and output voltage. The peak input RMS  
currentlevelofthesinglephasesystemisreducedby50%  
in a 2-phase solution due to the current splitting between  
the two stages.  
An interesting result of the 2-phase solution is that the VIN  
which produces worst-case ripple current for the input  
capacitor, VOUT = VIN/2, in the single phase design pro-  
duces zero input current ripple in the 2-phase design.  
The output ripple current is reduced significantly when  
compared to the single phase solution using the same  
inductance value because the VOUT/L discharge current  
term from the stage that has its bottom MOSFET on  
subtracts current from the (VIN - VOUT)/L charging current  
resultingfromthestagewhichhasitstopMOSFETon. The  
output ripple current is:  
Simplified Visual Explanation of How a 2-Phase  
Controller Reduces Both Input and Output RMS Ripple  
Current  
A multiphase power supply significantly reduces the  
amount of ripple current in both the input and output  
capacitors.TheRMSinputripplecurrentisdividedby,and  
the effective ripple frequency is multiplied up by the  
number of phases used (assuming that the input voltage  
isgreaterthanthenumberofphasesusedtimestheoutput  
voltage). The output ripple amplitude is also reduced by,  
and the effective ripple frequency is increased by the  
number of phases used. Figure 10 graphically illustrates  
the principle.  
12D 1D  
(
)
2VOUT  
fL  
IRIPPLE  
=
12D +1  
where D is duty factor.  
The input and output ripple frequency is increased by the  
number of stages used, reducing the output capacity  
The worst-case RMS ripple current for a single stage  
design peaks at twice the value of the output voltage . The  
worst-case RMS ripple current for a two stage design  
results in peaks at 1/4 and 3/4 of input voltage. When the  
requirements.WhenVIN isapproximatelyequalto2(VOUT  
)
as illustrated in Figures 3 and 4, very low input and output  
ripple currents result.  
20  
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L1  
SW1  
R
SENSE1  
D1  
V
V
OUT  
IN  
R
IN  
C
OUT  
+
+
C
R
L
IN  
L2  
SW2  
R
SENSE2  
D2  
BOLD LINES INDICATE  
HIGH, SWITCHING  
CURRENT LINES.  
KEEP LINES TO A  
MINIMUM LENGTH.  
1929 F09  
Figure 9. Instantaneous Current Path Flow in a Multiple Phase Switching Regulator  
SINGLE PHASE  
DUAL PHASE  
SW V  
SW1 V  
SW2 V  
I
CIN  
I
L1  
L2  
I
COUT  
I
I
CIN  
I
COUT  
RIPPLE  
1929 F10  
Figure 10. Single and 2-Phase Current Waveforms  
21  
LTC1929  
U
TYPICAL APPLICATIO S  
22  
LTC1929  
U
TYPICAL APPLICATIO S  
100  
90  
80  
70  
60  
50  
V
V
= 5V  
OUT  
IN  
= 1.6V  
0
5
10 15 20 25 30 35 40  
LOAD CURRENT (A)  
1929 TA04  
Figure 12. Efficiency Plot for Circuit of Figure 11  
U
PACKAGE DESCRIPTIO  
Dimensions in inches (millimeters) unless otherwise noted.  
G Package  
28-Lead Plastic SSOP (0.209)  
(LTC DWG # 05-08-1640)  
0.397 – 0.407*  
(10.07 – 10.33)  
28 27 26 25 24 23 22 21 20 19 18  
16 15  
17  
0.301 – 0.311  
(7.65 – 7.90)  
5
7
8
1
2
3
4
6
9 10 11 12 13 14  
0.205 – 0.212**  
(5.20 – 5.38)  
0.068 – 0.078  
(1.73 – 1.99)  
0° – 8°  
0.0256  
(0.65)  
BSC  
0.005 – 0.009  
(0.13 – 0.22)  
0.022 – 0.037  
(0.55 – 0.95)  
0.002 – 0.008  
(0.05 – 0.21)  
0.010 – 0.015  
(0.25 – 0.38)  
*DIMENSIONS DO NOT INCLUDE MOLD FLASH. MOLD FLASH  
SHALL NOT EXCEED 0.006" (0.152mm) PER SIDE  
**DIMENSIONS DO NOT INCLUDE INTERLEAD FLASH. INTERLEAD  
FLASH SHALL NOT EXCEED 0.010" (0.254mm) PER SIDE  
G28 SSOP 0694  
23  
LTC1929  
U
TYPICAL APPLICATIO  
L1  
1
28  
27  
26  
25  
24  
23  
22  
21  
20  
19  
18  
17  
16  
15  
1000pF  
0.005  
RUN/SS  
SENSE1  
SENSE1  
EAIN  
NC  
TG1  
2
+
0.1µF  
0.22µF  
D3  
M1  
M2  
3
D1  
MBRM  
140T3  
SW1  
13.2k  
4
BOOST1  
10Ω  
5
INTV  
CC  
PLLFLTR  
V
IN  
6
LTC1929  
C
OUT  
0.1µF  
PLLIN  
NC  
BG1  
33pF  
10k  
7
8
GND  
2X270µF  
2V  
220pF  
EXTV  
INTV  
CC  
22µF  
50V  
1µF,25V  
I
TH  
SGND  
CC  
4.7µF  
6.3V  
9
V
IN  
PGND  
BG2  
5V TO  
28V  
16.5k  
10  
11  
12  
13  
14  
V
V
V
DIFFOUT  
BOOST2  
SW2  
OS  
D2  
MBRM  
140T3  
D4  
0.22µF  
100pF  
+
OS  
+
SENSE2  
SENSE2  
TG2  
M3  
M4  
AMPMD  
0.005Ω  
1000pF  
V
OUT  
1.8V/20A  
L2  
D3, D4: CENTRAL CMDSH-3TR  
V
V
: 5V TO 28V  
MI – M4: FAIRCHILD FDS6680A  
L1 – L2: 2µH SUMIDA CEE125-2R1NC  
: PANASONIC EEFUEOD271R  
IN  
: 1.8V/20A  
OUT  
1929 TA02  
SWITCHING FREQUENCY = 310kHz  
C
OUT  
Figure 13. 1.8V/20A CPU Power Supply  
RELATED PARTS  
PART NUMBER  
LTC1438/LTC1439  
LTC1438-ADJ  
LTC1538-AUX  
LTC1539  
DESCRIPTION  
Dual High Efficiency Low Noise Synchronous Step-Down Switching Regulators POR, Auxiliary Regulator  
Dual Synchronous Controller with Auxiliary Regulator POR, External Feedback Divider  
Dual High Efficiency Low Noise Synchronous Step-Down Switching Regulator Auxiliary Regulator, 5V Standby  
Dual High Efficiency Low Noise Synchronous Step-Down Switching Regulator 5V Standby, POR, Low-Battery, Aux Regulator  
COMMENTS  
LTC1435/LTC1435A High Efficiency Synchronous Step-Down Switching Regulator  
Burst ModeTM Operation, 16-Pin Narrow SO  
Adaptive PowerTM Mode, 24-Pin SSOP  
Constant Frequency, Standby, 5V and 3.3V LDOs  
Expandable Up to 12 Phases, G-28, Up to 120A  
500kHz, 25MHz GBW  
LTC1436A-PLL  
LTC1628  
High Efficiency Low Noise Synchronous Step-Down Switching Regulator  
Dual High Efficiency, 2-Phase Synchronous Step-Down Switching Regulator  
PolyPhase High Efficiency Controller  
LTC1629  
LTC1702/LTC1703  
LTC1735  
Dual High Efficiency, 2-Phase Synchronous Step-Down Switching Regulator  
High Efficiency Synchronous Step-Down Controller  
Burst Mode Operation, 16-Pin Narrow SSOP,  
Fault Protection, 3.5V V 36V  
IN  
LTC1736  
High Efficiency Synchronous Step-Down Controller with 5-Bit VID  
Output Fault Protection, Power Good, GN-24,  
3.5V V 36V, 0.8V V  
6V  
IN  
OUT  
Adaptive Power and Burst Mode are trademarks of Linear Technology Corporation.  
1929i 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  

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