The NX2113 controller IC is a synchronous Buck controller IC designed for step down DC to DC converter
applications. Synchronous control operation replaces the
traditional catch diode with an Nch MOSFET resulting
in improved converter efficiency. The NX2113 controller
is optimized to convert bus voltages from 2V to 25V to
outputs as low as 0.8V voltage using Enable pin to
program the BUS voltage start up threshold. The NX2113
operates at 300kHz while 2113A is set at 600kHz
operation which together with less than 50 nS of dead
band provides an efficient and cost effective solution.
Other features of the device are:
Internal digital soft start; Vcc undervoltage lock out;
Output undervoltage protection with digital filter and shutdown capability via the enable pin.
Evaluation board available.
NX2113/2113A
PROGRAMMABLE BUS UVLO
PRELIMINARY DATA SHEET
Pb Free Product
FEATURES
n Synchronous Controller in 10 Pin Package
n Bus voltage operation from 2V to 25V
n Enable pin allows programmable BUS UVLO
n Less than 50 nS adaptive deadband
n Internal 300kHz for 2113 and 600kHz for 2113A
n Internal Digital Soft Start Function
n Separated power ground and analog ground for
extra noise filtering
n Pb-free and RoHS compliant
APPLICATIONS
n Graphic Card on board converters
n Memory Vcore or Vddq supply
n On board DC to DC such as12V, 5V to 3.3V, 2.5V or 1.8V
n Hard Disk Drive
ON
OFF
TYPICAL APPLICATION
C6
1uF
6
Vcc
PGnd
3
L2 1uH
1
5
BST
PVcc
Hdrv
SW
NX2113A
Ldrv
Gnd
11
10k 1%R1
C8
R9
1.2k
D1
2.2nF
C5
1uF
C7
0.1uF
2
10
4
M1
L1 1.5uH
M2
Cin
270uF,18mohm
Co
3x (220uF,12mohm)
Vout
+1.6V,10A
Vin
+12V
Vin
+5V
2N3904
R8
10k
R7
10k
C3
47uF
C9
1uF
R5
68k
R6
12.4k
C1
47pF
R3
10
C4
1uF
C2
2.7nF
R4
11k
R2
10k 1%
7
9
8
EN
Comp
Fb
Figure1 - Typical application of 2113A
Rev. 2.0
11/18/05
ORDERING INFORMATION
Device Temperature Package Frequency Pb-Free
NX2113CMTR 0 to 70oC MLPD-10L300kHz Yes
NX2113CUTR 0 to 70oC MSOP-10L300kHz Yes
NX2113ACMTR 0 to 70oC MLPD-10L600kHz Yes
NX2113ACUTR 0 to 70oC MSOP-10L600kHz Yes
1
Page 2
NX2113/2113A
θ≈52/
CW
CW
θ≈200/
3.4
ABSOLUTE MAXIMUM RATINGS
Vcc to GND & BST to SW voltage ................... 6.5V
BST to GND Voltage ...................................... 35V
Storage Temperature Range ............................. -65oC to 150oC
Operating Junction Temperature Range ............. -40oC to 125oC
CAUTION: Stresses above those listed in "ABSOLUTE MAXIMUM RATINGS", may cause permanent damage to
the device. This is a stress only rating and operation of the device at these or any other conditions above those
indicated in the operational sections of this specification is not implied.
PACKAGE INFORMATION
10-LEAD PLASTIC MSOP 10-LEAD PLASTIC MLPD
JA
PAD
(Gnd)
o
10
SW
9
Comp
8
Fb
7
EN
6
Vcc
BST
HDrv
PGnd/Gnd
LDrv
PVcc
JA
1
2
3
4
5
o
10
9
8
7
6
SW
Comp
Fb
EN
Vcc
PGnd
PVcc
BST
HDrv
LDrv
1
2
3
4
5
ELECTRICAL SPECIFICATIONS
Unless otherwise specified, these specifications apply over Vcc = 5V, and TA = 0 to 70oC. Typical values refer to T
= 25oC. Low duty cycle pulse testing is used which keeps junction and case temperatures equal to the ambient
PARAMETERSYMTest ConditionMinTYPMAXUnits
Reference Voltage
Ref VoltageV
REF
Ref Voltage line regulation0.4%
Supply Voltage(Vcc)
VCC Voltage RangeV
CC
VCC Supply Current (Static)ICC (Static) Outputs not switching 2.1mA
VCC Supply Current
(Dynamic)
Fall TimeTHdrv(Fall)V
Deadband TimeLdrv going Low to Hdrv
Tdead(L to
H)
BST-VSW
BST-VSW
going High, 10%-10%
=4.5V50ns
=4.5V50ns
ns30
Low Side Driver (CL=3300pF)
Output Impedance, Sourcing
R
(Ldrv) I=200mA1.1ohm
source
Current
Output Impedance, Sinking
R
(Ldrv) I=200mA0.5ohm
sink
Current
Rise TimeTLdrv(Rise)10% to 90%50ns
Fall TimeTLdrv(Fall)90% to 10%50ns
Deadband TimeTdead(H to L)SW going Low to Ldrv
30
ns
going High, 10% to 10%
Rev. 2.0
11/18/05
3
Page 4
PIN DESCRIPTIONS
PIN # PIN SYMBOL PIN DESCRIPTION
1BST
This pin supplies voltage to the high side driver. A high frequency
ceramic capacitor of 0.1 to 1 uF must be connected from this pin to SW pin.
NX2113/2113A
2HDRV
3PGND/Gnd
4LDRV
5PVcc
6Vcc
7EN
8FB
9COMP
High side MOSFET gate driver.
Power and analog ground pin. For MLPD package, analog ground and power ground
are separated, additional pad pin(11) is available for analog ground.
Low side MOSFET gate driver.
Ldrv supply voltage. A 1uF high frequency cap must be connected from this pin to
GND directly.
Voltage supply for the internal circuit as well as the low side MOSFET gate driver. A
1uF high frequency ceramic capacitor must be connected from this pin to GND pin.
Pull up this pin to Vcc for normal operation. Pulling this pin down below 1.25V
shuts down the controller and resets the soft start. This pin can also be used as
a UVLO detector for the bus voltage via a resistor divider.
This pin is the error amplifier inverting input. This pin is also connected to the output
UVLO comparator. When this pin falls below 0.4V, both HDRV and LDRV outputs
are latched off.
This pin is the output of the error amplifier and together with FB pin is used to
compensate the voltage control feedback loop.
10SW
Rev. 2.0
11/18/05
This pin is connected to the source of the high side MOSFET and provides return
path for the high side driver.
VIN - Input voltage
VOUT - Output voltage
IOUT - Output current
DVRIPPLE - Output voltage ripple
FS - Working frequency
DIRIPPLE - Inductor current ripple
Design Example
The following is typical application for NX2113A,
the schematic is figure 2.
VIN = 12V
VOUT=1.6V
IOUT=10A
DVRIPPLE <=20mVDVDROOP<=80mV @ 10A step
FS=600kHz
Output Inductor Selection
The selection of inductor value is based on inductor ripple current, power rating, switching frequency and
efficiency. Larger inductor value normally means smaller
ripple current. However if the inductance is chosen too
large, it brings slow response and lower efficiency. Usually the ripple current ranges from 20% to 40% of the
output current. This is a design freedom which can be
decided by design engineer according to various application requirements. The inductor value can be calculated by using the following equations:
V-VV
OUT
∆
INOUT OUT
××
×
12V-1.6V1.6V1
OUT
OUT
×
××
...(1)
L=
I=kI
RIPPLEOUTPUT
where k is between 0.2 to 0.4.
Select k=0.3, then
L=
L=0.8uH
Choose inductor from COILCRAFT DO5010P781HC with L=0.78uH is a good choice.
Current Ripple is recalculated as
V-VV
I=
∆××
RIPPLE
INOUT OUT
LVF
OUTINS
12V-1.6V1.6v1
0.78uH12v600kHz
××=
1
...(2)
Output Capacitor Selection
Output capacitor is basically decided by the
amount of the output voltage ripple allowed during steady
state(DC) load condition as well as specification for the
load transient. The optimum design may require a couple
of iterations to satisfy both condition.
Based on DC Load Condition
The amount of voltage ripple during the DC load
condition is determined by equation(3).
∆
I
∆=×∆+
VESRI
RIPPLERIPPLE
Where ESR is the output capacitors' equivalent
series resistance,C
Typically when large value capacitors are selected
such as Aluminum Electrolytic,POSCAP and OSCON
types are used, the amount of the output voltage ripple
is dominated by the first term in equation(3) and the
second term can be neglected.
For this example, POSCAP are chosen as output
capacitors, the ESR and inductor current typically determines the output voltage ripple.
∆
tiple capacitors in parallel are better than a big capacitor. For example, for 20mV output ripple, POSCAP
2R5TPE220MC with 12mΩ are chosen.
integer. Choose N =2.
desire
If low ESR is required, for most applications, mul-
ESRI
N
=
Number of Capacitor is calculated as
N
=
N =1.8
The number of capacitor has to be round up to a
If ceramic capacitors are chosen as output ca-
Ω×
20mV
is the value of output capacitors.
OUT
V
RIPPLE
I3A
∆
RIPPLE
20mV
×∆
V
∆
RIPPLE
RIPPLE
××
8FC
...(5)
...(3)
...(4)
Rev. 2.0
11/18/05
9
Page 10
NX2113/2113A
8600kHz100uF
DROOPTRAN
2
∆=×∆+×τ
OUTcrit
ESRCifLL
OUTOUTEEOUT
crit
LL
2
=+×τ
EEcrit
ESRCifLL
0.42H
=µ
12m220F2.24us
2
1.7×∆=+×τ
pacitors, both terms in equation (3) need to be evaluated
to determine the overall ripple. Usually when this type of
capacitors are selected, the amount of capacitance per
single unit is not sufficient to meet the transient specification, which results in parallel configuration of multiple
capacitors .
For example, one 100uF, X5R ceramic capacitor
with 2mΩ ESR is used. The amount of output ripple is
∆=Ω×+
V2m3A
RIPPLE
6mV6.2mV12.2mV
=+=
3A
××
Although this meets DC ripple spec, however it
needs to be studied for transient requirement.
Based On Transient Requirement
Typically, the output voltage droop during transient
is specified as:
V<V∆∆ @ step load DI
STEP
During the transient, the voltage droop during the
transient is composed of two sections. One Section is
dependent on the ESR of capacitor, the other section is
a function of the inductor, output capacitance as well as
input, output voltage. For example, for the overshoot,
when load from high load to light load with a DI
STEP
transient load, if assuming the bandwidth of system is
high enough, the overshoot can be estimated as the following equation.
V
VESRI
overshootstep
OUT
2LC
××
OUT
...(6)
where τ is the a function of capacitor, etc.
0ifLL
LI
×∆
τ=
V
OUT
≤
crit
step
−×≥
...(7)
where
ESRCVESRCV
××××
==
II
∆∆
stepstep
...(8)
L
crit
where ESRE and CE represents ESR and capacitance of each capacitor if multiple capacitors are used
in parallel.
The above equation shows that if the selected output inductor is smaller than the critical inductance, the
voltage droop or overshoot is only dependent on the ESR
of output capacitor. For low frequency capacitor such
as electrolytic capacitor, the product of ESR and ca-
pacitance is high and
≤
is true. In that case, the
transient spec is dependent on the ESR of capacitor.
In most cases, the output capacitors are multiple
capacitors in parallel. The number of capacitors can be
calculated by the following
ESRI
×∆
N
Estep
V2LCV
∆×××∆
tranEtran
V
OUT
...(9)
where
0ifLL
LI
×∆
τ=
V
OUT
≤
crit
step
−×≥
...(10)
For example, assume voltage droop during transient is 100mV for 10A load step.
If the POSCAP 2R5TPE220MC(220uF, 12mΩ ) is
used, the critical inductance is given as:
ESRCV
××
L
crit
12m220F1.6V
EEOUT
==
I
∆
step
Ω×µ×
10A
The selected inductor is 0.78uH which is bigger
than critical inductance. In that case, the output voltage
transient not only dependent on the ESR, but also capacitance.
number of capacitors is
LI
×∆
step
τ=−×
V
0.78H10A
µ×
=−Ω×µ=
1.6V
ESRI
N
12m10A
Ω×
=+
80mV
21.5H220F80mV
×µ×µ×
ESRC
OUT
Estep
V2LCV
∆×××∆
1.6V
EE
V
OUT
tranEtran
(2.24us)
×
2
≈
The number of capacitors has to satisfy both ripple
and transient requirement. Overall, we can choose N=3.
Rev. 2.0
11/18/05
10
Page 11
It should be considered that the proposed equa-
F ...(11)
F ...(12)
F ...(13)
F ...(14)
OUT minin1
V1gZZ/R
f
OUT in
Z
VZ
−
tion is based on ideal case, in reality, the droop or overshoot is typically more than the calculation. The equation gives a good start. For more margin, more capacitors have to be chosen after the test. Typically, for high
frequency capacitor such as high quality POSCAP especially ceramic capacitor, 20% to 100% (for ceramic)
more capacitors have to be chosen since the ESR of
capacitors is so low that the PCB parasitic can affect
the results tremendously. More capacitors have to be
selected to compensate these parasitic parameters.
Compensator Design
Due to the double pole generated by LC filter of the
power stage, the power system has 180o phase shift ,
and therefore, is unstable by itself. In order to achieve
accurate output voltage and fast transient response,
compensator is employed to provide highest possible
bandwidth and enough phase margin. Ideally, the Bode
plot of the closed loop system has crossover frequency
between 1/10 and 1/5 of the switching frequency, phase
margin greater than 50o and the gain crossing 0dB with 20dB/decade. Power stage output capacitors usually
decide the compensator type. If electrolytic capacitors
are chosen as output capacitors, type II compensator
can be used to compensate the system, because the
zero caused by output capacitor ESR is lower than crossover frequency. Otherwise type III compensator should
be chosen.
NX2113/2113A
=
Z1
=
Z2
=
P1
=
P2
where FZ1,FZ2,FP1 and FP2 are poles and zeros in
the compensator. Their locations are shown in figure 10.
The transfer function of type III compensator for
transconductance amplifier is given by:
V1gZ
emf
For the voltage amplifier, the transfer function of
compensator is
the compensator of transconductance amplifier must
satisfy this condition: R4>>2/gm. R1||R2||R3>>1/gm
is desirable.
=
V
e
=
To achieve the same effect as voltage amplifier,
Vout
Zin
1
2RC
×π××
42
1
2(RR)C
×π×+×
233
1
2RC
×π××
33
1
CC
×
2R
×π××
−×
+×+
4
CC
12
+
12
Zf
C1
A. Type III compensator design
For low ESR output capacitors, typically such as
Sanyo oscap and poscap, the frequency of ESR zero
caused by output capacitors is higher than the crossover frequency. In this case, it is necessary to compensate the system with type III compensator. The following figures and equations show how to realize the type III
compensator by transconductance amplifier.
Rev. 2.0
11/18/05
R3
C2
R4
R2
C3
Fb
gm
Ve
R1
Vref
Figure 9 - Type III compensator using
transconductance amplifier
11
Page 12
NX2113/2113A
20.78uH660uF
24m660uF
211k300kHz
260kHz2.2nF
=(-)
210k7kHz60kHz
=2nF
=660uF
20.757kHz11k
×π×××Ω
smaller than 1/10~ 1/5 of the switching frequency. Set
FO=45kHz.
power stage
LC
F
Gain(db)
40dB/decade
loop gain
ESR
F
20dB/decade
compensator
F
Z1Z2
F
F
O
F
P1
F
P2
Figure 10 - Bode plot of Type III compensator
Design example for type III compensator are in
order. Use the same power stage requirement as demo
board. The crossover frequency has to be selected as
FLC<FO<F
1.Calculate the location of LC double pole F
and ESR zero F
and FO<=1/10~1/5F
ESR,
.
ESR
F
=
LC
2LC
×π××
=
s.
LC
1
OUTOUT
1
×π××
7kHz
=
F
=
ESR
2ESRC
×π××
=
×π×Ω×
60kHz
=
1
OUT
1
C=(-)
111
3
2RFF
×π×
×
2z2p1
111
×
×π×Ω
V2FL
R=C
4out
VC
2V245kHz0.78uH
12V2.2nF
=11k
×π××
OSCO
××
in3
×π××
××
Ω
Choose C3=2.2nF, R4=11kΩ.
5. Calculate C2 with zero Fz1 at 75% of the LC
double pole by equation (11).
C
2.75nF
=
2
2FR
=
=
1
×π××
Z14
1
Choose C2=2.7nF.
6. Calculate C1 by equation (14) with pole Fp2 at
half the swithing frequency.
C
=
1
2RF
=
48pF
=
1
×π××
4P2
1
×π×Ω×
Choose C1=47pF.
7. Calculate R3 by equation (13).
1
2FC
×π××
P13
1
×π××
R
=
3
=
1.2k
=Ω
Choose R3=1.2kΩ.
2.Set R2 equal to10kΩ, then R1= 10kΩ.
3. Set zero FZ2 = FLC and Fp1 =F
4. Calculate R4 and C3 with the crossover frequency
Rev. 2.0
11/18/05
ESR
.
12
Page 13
NX2113/2113A
Gain=gR ... (15)
F= ... (16)
F ... (17)
24.7uH1360uF
218m1360uF
R4.7k
==Ω
12V18m2.5mA/V
B. Type II compensator design
If the electrolytic capacitors are chosen as power
stage output capacitors, usually the Type II compensator can be used to compensate the system.
Vout
R2
Fb
gm
R1
Vref
Figure 11 - Type II compensator with
transconductance amplifier
power stage
Ve
R3
C2
C1
noise. The following equations show the compensator
pole zero location and constant gain.
R
1
××
m3
R+R
12
1
z
2RC
×π××
≈
p
31
1
2RC
×π××
32
For this type of compensator, FO has to satisfy
FLC<F
<<FO<=1/10~1/5F
ESR
s.
The following uses typical design in figure 18 as
an example for type II compensator design, two 680uF
with 36mΩ electrolytic capacitors are used.
1.Calculate the location of LC double pole F
and ESR zero F
F
LC
.
ESR
=
2LC
×π××
=
1
OUTOUT
1
LC
×π××
2.0kHz
=
40dB/decade
Gain(db)
loop gain
20dB/decade
compensator
Gain
F
F
LC
Z
ESRFO
P
F
F
Figure 12 - Bode plot of Type II compensator
Type II compensator can be realized by simple
RC circuit without feedback as shown in figure 11. R3
and C1 introduce a zero to cancel the double pole
effect. C2 introduces a pole to suppress the switching
F
ESR
6.5kHz
2.Set R
1
=
2ESRC
×π××
=
×π×Ω×
=
equal to10kΩ. Using equation 18.
2
10k0.8V
Ω×
2.5V-0.8V
1
OUT
1
3. Set crossover frequency at 1/10~ 1/5 of the
swithing frequency, here FO=30kHz.
4.Calculate R3 value by the following equation.
V2FL
OSCO
R=
3
VRgR
2V230kHz4.7uH1
=
=10.3k
×π××
×××
inESRm1
×π××
××
10k+4.7k
ΩΩ
×
4.7k
Ω
Ω
1
R+R
12
Ω
Choose R3 =10kΩ.
Rev. 2.0
11/18/05
13
Page 14
NX2113/2113A
210k0.756.5kHz
p
F
10k300kHz
OUT
REF
2REF
OUT REF
R1.6V1.6V/(1/16W)40
=×=Ω
IID1-D
5. Calculate C1 by setting compensator zero F
Z
at 75% of the LC double pole.
C=
1
=
1
2RF
×π××
3z
1
×π×Ω××
=10.7nF
Choose C1=10nF.
6. Calculate C
by setting compensator pole
2
at
half the swithing frequency.
C=
2
=
1
RF
π××
3s
1
π×Ω×
=106pF
Choose C2=100pF.
Output Voltage Calculation
Output voltage is set by reference voltage and
external voltage divider. The reference voltage is fixed
at 0.8V. The divider consists of two ratioed resistors
so that the output voltage applied at the Fb pin is 0.8V
when the output voltage is at the desired value. The
following equation and picture show the relationship
between
value of R1 value can be set by voltage divider.
1.6V, the result of R1 is 10kΩ.
V,
R=
1
where R
Vand voltage divider..
RV
×
V-V
2 is part of the compensator, and the
...(18)
Choose R2=10kΩ, to set the output voltage at
Vout
R2
Fb
R1
Vref
Voltage divider
Figure 13 - Voltage divider load
In general, the minimum output load impedance
including the resistor divider should be less than 5kΩ to
prevent overcharge the output voltage by leakage current (e.g. Error Amplifier feedback pin bias current). A
minimum load for 5kΩ less (<1/16w for most of application) is recommended to put at the output. For example,
in this application,
Vout=1.6V
The power loss is 1/16W less
LOAD
Select minimum load is 1kΩ should be good
enough.
Input Capacitor Selection
Input capacitors are usually a mix of high frequency
ceramic capacitors and bulk capacitors. Ceramic capacitors bypass the high frequency noise, and bulk capacitors supply current to the MOSFETs. Usually 1uF
ceramic capacitor is chosen to decouple the high frequency noise. The bulk input capacitors are decided by
voltage rating and RMS current rating. The RMS current
in the input capacitors can be calculated as:
=××
RMSOUT
V
OUT
D
=
V
IN
...(19)
VIN = 12V, VOUT=1.6V, IOUT=10A, using equation
(19), the result of input RMS current is 3.4A.
For higher efficiency, low ESR capacitors are
recommended. One Sanyo OSCON SP series
16SP270M 16V 270uF with 4.4A is chosen as input
bulk capacitor.
Power MOSFETs Selection
The NX2113 requires two N-Channel power
MOSFETs. The selection of MOSFETs is based on
maximum drain source voltage, gate source voltage,
maximum current rating, MOSFET on resistance and
power dissipation. The main consideration is the power
loss contribution of MOSFETs to the overall converter
efficiency. In this design example, two IRFR3706 are
used. They have the following parameters: VDS=30V, I
=75A,R
=9mΩ,Q
DSON
GATE
=23nC.
D
Rev. 2.0
11/18/05
14
Page 15
NX2113/2113A
gateHGATEHGSLGATELGSS
P(QVQV)F
=×+××
P=I(1D)RK
×−××
SWINOUTSWS
PVITF
=××××
R6.8k
==Ω
There are three factors causing the MOSFET power
loss: conduction loss, switching loss and gate driver loss.
Gate driver loss is the loss generated by discharging the gate capacitor and is dissipated in driver circuits.
It is proportional to frequency and is defined as:
...(20)
where QHGATE is the high side MOSFETs gate
charge,QLGATE is the low side MOSFETs gate charge,VHGS
is the high side gate source voltage, and V
LGS
is
the low side gate source voltage.
According to equation (20), PGATE =0.14W. This
power dissipation should not exceed maximum power
dissipation of the driver device.
Conduction loss is simply defined as:
P=IDR
HCONOUTDS(ON)
LCONOUTDS(ON)
P=PP
TOTALHCONLCON
2
×××
2
K
+
...(21)
where the RDS(ON) will increases as MOSFET junction temperature increases, K is RDS(ON) temperature
dependency. As a result, RDS(ON) should be selected for
the worst case, in which K equals to 1.4 at 125oCaccording toIRFR3706 datasheet. Using equation (21),
the result of PTOTAL is 0.54W. Conduction loss should
not exceed package rating or overall system thermal
budget.
Switching loss is mainly caused by crossover conduction at the switching transition. The total switching
loss can be approximated.
1
2
...(22)
where IOUT is output current, TSW is the sum of TR and T
which can be found in mosfet datasheet, and FS is switching frequency. The result of PSW is 3W. Swithing loss
PSW is frequency dependent.
Soft Start, Enable and shut Down
The NX2113 has a digital start up. It is based on
digital counter with 1024 cycles. For NX2113 with 300kHz
operation, the start up time is about 3.5ms. For NX2113A
with 600kHz operation, the start up time is about half of
NX2113, 1.75mS.
Vbus
+
POR
ON
OFF
10k
R1
R2
EN
1.25/1.15
Figure 14 - Enable and Shut down NX2113 by
pulling down EN pin.
The start up of NX2113/2113A can be programmed
through resistor divider at Enable pin. For example, if
the input bus voltage is 12V and we want NX2113 starts
when Vbus is above 8V. We can select
R2=1.24k
(8V1.25V)R
1
1.25V
−×
2
The NX2113 can be turned off by pulling down the
ENable pin by extra signal MOSFET or NPN transistor
such as 2N3904 as shown in the above Figure. When
Enable pin is below 1.15V, the digital soft start is reset
to zero. In addition, all the high side is off and output
voltage is turned off.
A resistor should be added as preload to prevent
leakage current from FB pin charging the output capacitors.
Feedback Under Voltage Shut Down
NX2113 relies on the Feedback Under Voltage Lock
Out (FB UVLO ) to provide short circuit protection. Ba-
F
sically, NX2113 has a comparator compares the feedback voltage with the FB UVLO threshold 0.4V.
During the normal operation, if the output is short,
the feedback voltage will be lower than 0.4V and comparator will change the state. After certain internal delay,
both high side and low side driver will be turned off. The
output will be latched. The normal operation should be
achieved by removing the short and recycle the VCC.
During the start up, the output voltage is discharged to zero by the synchronous FET. FB voltage
starts increase from zero when digital start block
Digital
start
up
Rev. 2.0
11/18/05
15
Page 16
NX2113/2113A
operates. Before half of the start up time, the Feedback
Under Voltage Lock Out comparator is disabled. After
half of start up time, the Feedback UVLO comparator is
enabled. The FB UVLO threshold is set to be half of
voltage at the positive input of error amplifier. With this
set up, if the output is short before soft start, the
Feedback UVLO comparator can catch it and turn off
the driver. The short circuit operation waveform during
normal operation and during the soft start are shown as
follows.
CH3-FB voltage
0.5V/DIV
CH1-SW voltage
10V/DIV
The Feedback UVLO can provide certain short circuit protection. However, since feedback does not have
accurate information of current, this protection only provides certain level of over current protection. MOSFET
should design such that it can survive with high pulse
current for a short period of time.
The value of the capacitor on enable pin to ground
and the resistor value of voltage divider on enable pin
should be big enough to keep enable pin high during
short. Otherwise, once output shorts, the input bus voltage drops, the chip is disabled before Feedback UVLO
takes effect, and the system goes into hiccup status.
This phenomena is easy to be found during system
startup, if related resistor and capacitor value is not big
enough.
Figure 15 - Operation waveforms during short con-
dition.
Figure 16 - Feedback UVLO with start up at
short.
CH4-load current
10A/DIV
CH2-output voltage
1V/DIV
CH4-load current
10A/DIV
CH2-Output voltage
1V/DIV
CH4-load current
10A/DIV
Figure 17 -Hiccup with start up at short.
Layout Considerations
The layout is very important when designing high
frequency switching converters. Layout will affect noise
pickup and can cause a good design to perform with
less than expected results.
Start to place the power components, make all the
connection in the top layer with wide, copper filled areas. The inductor, output capacitor and the MOSFET
should be close to each other as possible. This helps to
reduce the EMI radiated by the power traces due to the
high switching currents through them. Place input capacitor directly to the drain of the high-side MOSFET, to
Rev. 2.0
11/18/05
16
Page 17
reduce the ESR replace the single input capacitor with
two parallel units. The feedback part of the system should
be kept away from the inductor and other noise sources,
and be placed close to the IC. In multilayer PCB use
one layer as power ground plane and have a control circuit ground (analog ground), to which all signals are referenced.
The goal is to localize the high current path to a
separate loop that does not interfere with the more sensitive analog control function. These two grounds must
be connected together on the PC board layout at a single
point.
NX2113/2113A
Rev. 2.0
11/18/05
17
Page 18
TYPICAL APPLICATION
Dual power supply (+5V BIAS,+12V BUS)
NX2113/2113A
Vin
+12V
Vin
+5V
1k
C4
47uF
R5
1k
R6
C1
100pF
R5
10
C5
1uF
C2
10nF
R4
10k
R2
4.7k 1%
7
9
8
C6
1uF
6
Vcc
EN
Comp
Fb
Figure 18 -Application of NX2113 for 5V bias and 12V input bus
Single power supply (+11V to +24V BUS)
5
PVcc
NX2113
PGnd/Gnd
3
10k 1%R1
L2 1uH
1
BST
Hdrv
SW
Ldrv
C5
1uF
D1
C7
2
0.1uF
10
4
M1
L1 4.7uH
M2
Cin
39uF,31mohm
Co
2 x (680uF,36mohm)
Vout
+2.5V,4A
Vin
+11~25V
L2 1uH
TL431
C1
R5
3k
2N3904
R6
12.7k
R7
10k
C2
10nF
R4
10k
R2
4.7k 1%
R8
76.8k
R9
10k
7
9
8
R5
10
C8
1uF
EN
Comp
Fb
Vcc
PGnd
6
3
C6
1uF
PVcc
1
5
BST
Hdrv
SW
NX2113
Ldrv
Gnd
11
R1
10k 1%
D1
C7
2
0.1uF
10
4
M1
M2
C4
47uF
100pF
Figure 19 -Application of NX2113 for high input bus application
C5
1uF
L1 4.7uH
Cin
2 x (47uF,60mohm)
Co
2 x (680uF,36mohm)
Vout
+1.6V,5A
Rev. 2.0
11/18/05
18
Page 19
TYPICAL APPLICATION
Single Supply 5V Input
NX2113/2113A
Vin
+5V
R4
120k
C2
330pF
C4
10uF
X7R
C1
4.7pF
R2
20k 1%
L2 1uH
R5
10
C8
1uF
7
EN
9
Comp
8
Fb
6
Vcc
PGnd
C6
1uF
5
PVcc
Gnd
3
R1
10k 1%
R3
787
D1
1
BST
2
Hdrv
10
SW
NX2113A
11
C3
820pF
Ldrv
4
C7
0.1uF
M1
L1 3.3uH
M2
C5
1uF
Cin
3 x 22uF
X7R
Co
10 x 22uF
X7R
Vout
+1.2V,4A
Figure 20 - Application of NX2113 A for 5V input and 1.6V output with ceramic output capacitors
Rev. 2.0
11/18/05
19
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