Datasheet nx2308ds Datasheets

Page 1
NEXSEM
SINGLE SUPPLY 12V SYNCHRONOUS PWM CONTROLLER
NX2308
ADVANCE DATA SHEET
Pb Free Product
DESCRIPTION
The NX2308 controller IC is a compact synchronous Buck controller IC designed for step down DC to DC con­verter applications. The NX2308 controller is optimized to convert single supply 12V bus voltage to as low as
0.8V output voltage. Internal UVLO keeps the regulator off until the supply voltage exceeds 9V where internal digital soft starts get initiated to ramp up output. The NX2308 employs loss-less current limiting followed by HICCUP feature. Other features includes: 12V gate drive capability , Converter Shutdown by pulling COMP pin to Gnd, Adaptive dead band control.
Vin
+12V
C4 100uF
R7
10
D1 1N4148
FEATURES
n 12V Gate Driver n Bus voltage operation from 9V to 15V n Hiccup current limit by sensing Rdson of
Synchronous MOSFET
n Internal 300kHz n Internal Digital Soft Start Function n Adaptive deadband Control n Shut Down via pulling COMP pin n Pb-free and RoHS compliant
APPLICATIONS
n Graphic Card on board converters n Vddq Supply in mother board applications n On board DC to DC such as
12V to 3.3V, 2.5V or 1.8V
n Set Top Box and LCD Display
TYPICAL APPLICATION
L2 1uH
C5
1uF
Cin
180uF
HI=SD
M3
C7
100pF
C7 1uF
5.6nF
C3 1uF
R4
10.2k
C2
6
5VREG
8
COMP
7
FB
5
BSTVcc
NX2308
Gnd
1
3
Hdrv
SW
OCP
Ldrv
C6
0.1uF
2
10
9
4
4k
M1
L1 2.2uH
R5
M2
1.1k
C1
3.9nF
8k
Co
2 x 470uF
R2
10k
Vout +1.8V 10A
Figure1 - Typical application of NX2308
ORDERING INFORMATION
Device Temperature Package Frequency Pb-Free NX2308CUTR 0 to 70oC MSOP - 10L 300kHz Yes NX2308CMTR 0 to 70oC MLPD - 10L 300kHz Yes
Rev. 2.0 12/19/05
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NEXSEM
θ≈200/
CW
θ≈52/
CW
REF
CC
Supply Current
NX2308
ABSOLUTE MAXIMUM RATINGS
Vcc to PGND & BST to SW voltage .................... -0.3V to 16V
BST to PGND Voltage ...................................... -0.3V to 35V
SW to PGND .................................................... -2V to 35V
All other pins .................................................... -0.3V to 6.5V
Storage Temperature Range ............................... -65oC to 150oC
Operating Junction Temperature Range ............... -40oC to 125oC
ESD Susceptibility ........................................... 2kV
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
o
o
JA
BST
HDrv
Gnd
LDrv
Vcc
1 2 3 4 5
10
9 8
7 6
SW OCP Comp FB 5VReg
BST
HDrv
NC
LDrv VCC
1
2 3
4 5
Gnd (PAD)
10
9 8 7
6
SW OCP
COMP
FB 5VReg
ELECTRICAL SPECIFICATIONS
Unless otherwise specified, these specifications apply over Vcc =12V, V values refer to TA = 25oC.
PARAMETER SYM Test Condition Min TYP MAX Units
Reference Voltage
Ref Voltage V Ref Voltage line regulation 10V<=VCC<=14V 0.2 %
Supply Voltage(Vcc)
VCC Voltage Range V V
CC
(Static) VCC Supply Current
(Dynamic)
Supply Voltage(V
V
Voltage Range V
BST
V
Supply Current V
BST
Under Voltage Lockout
VCC-Threshold VCC_UVLO VCC Rising VCC-Hysteresis VCC_Hyst VCC Falling 0.3 V
BST)
ICC (Static) mAOutputs not switching 5
I
CC
(Dynamic)
to V
BST
BST
(Dynamic)
CL=3300PF 17 mA
SW
CL=3300PF 12 mA
BST-VSW
=12V, and TA = 0 to 70oC. Typical
7 14
7 14
0.8
6.6
V
V
V
V
Rev. 2.0 12/19/05
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NEXSEM
S
RAMP
Comp SD Threshold
0.2
V
sink
OCP current
40
uA
Ldrv going Low to Hdrv going
NX2308
PARAMETER SYM Test Condition Min TYP MAX Units
Oscillator
Frequency F Ramp-Amplitude Voltage V Max Duty Cycle Min Duty Cycle
Error Amplifiers
Transconductance 2000 umho
Input Bias Current Ib 100 nA
Soft Start
Soft Start time Tss 6.8 mS
High Side Driver (CL=3300pF)
R
Output Impedance , Sinking
Current
Output Impedance , Sinking
Current
Rise Time THdrv(Rise) 10% to 90% 30 ns Fall Time THdrv(Fall) 90% to 10% 20 ns Deadband Time
Low Side Driver (CL=3300pF)
Output Impedance, Sourcing Current
Output Impedance, Sourcing Current
Rise Time TLdrv(Rise) 10% to 90% 30 ns
N
Fall Time TLdrv(Fall) 90% to 10% 20 ns Deadband Time Tdead(H to L)SW going Low to Ldrv going
(Hdrv) I= 200mA 3.6 ohm
source
R
(Hdrv) I=200mA 1 ohm
Tdead(L to
H)
R
(Ldrv) I=200mA 2.2 ohm
source
R
(Ldrv) I=200mA 1 ohm
sink
High, 10% to 10%
High, 10% to 10%
300 KHz
1.1 V 94 %
0
50
%
ns50
ns
OCP Adjust
Rev. 2.0 12/19/05
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NEXSEM
PIN DESCRIPTIONS
PIN # PIN SYMBOL PIN DESCRIPTION
Power supply voltage. A high freq 1uF ceramic capacitor is placed as close as
5
1
VCC
BST
possible to and connected to this pin and ground pin. The maximum rating of this pin is 16V.
This pin supplies voltage to high side FET driver. A high freq 0.1uF ceramic capacitor is placed as close as possible to and connected to these pins and respected SW pins.
NX2308
10
3
7
8
2 4
9
GND
FB
COMP
SW
HDRV
LDRV
OCP
Power ground. This pin is the error amplifiers inverting input. This pin is connected via resistor
divider to the output of the switching regulator to set the output DC voltage.
This pin is the output of the error amplifier and together with FB pin is used to compensate the voltage control feedback loop. This pin is also used as a shut down pin. When this pin is pulled below 0.2V, both drivers are turned off and internal soft start is reset.
This pin is connected to source of high side FET and provide return path for the high side driver. It is also used to hold the low side driver low until this pin is brought low by the action of high side turning off. LDRV can only go high if SW is below 1V threshold .
High side gate driver output. Low side gate driver output. This pin is connected to the drain of the external low side MOSFET and is the input
of the over current protection(OCP) comparator. An internal current source 40uA is flown to the external resistor which sets the OCP voltage across the Rdson of the low side MOSFET. Current limit point is this voltage divided by the Rds-on. Once this threshold is reached the Hdrv and Ldrv pins are switched low and an internal hiccup circuit is set that recycles the soft start circuit after 2048 switching cycles.
Rev. 2.0 12/19/05
6
5VREG
Output of internal 5V regulator. An external 0.1uF capacitor is required for stabil­ity.
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NEXSEM
BLOCK DIAGRAM
NX2308
VCC
5VREG
FB
COMP
Bias Regulator
Bias Generator
START
Digital start Up
0.8V
COMP
0.2V
START
1.25V
0.8V
7.2/6.8V
OSC
ramp
0.6V CLAMP
UVLO
set1
1.3V CLAMP
POR
START
OC
Control Logic
PWM
S
Q
R
Hiccup Logic
OC
OCP comparator
VCC
I
BST
HDRV
SW
LDRV
OCP
OCP
Rev. 2.0 12/19/05
GND
Figure 2 - Simplified block diagram of the NX2308
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NEXSEM
RIPPLEINS
1
IVF
0.310A12V300kHz
=2.3A
SOUT
==Ω
ESR=8.7m
ERIPPLE
9m2.3A
NX2308
APPLICATION INFORMATION
Symbol Used In Application Information:
VIN - Input voltage VOUT - Output voltage IOUT - Output current DVRIPPLE - Output voltage ripple FS - Switching frequency DIRIPPLE - Inductor current ripple
Design Example
Power stage design requirements: VIN=12V VOUT=1.8V IOUT =10A DVRIPPLE <=20mV DVTRAN<=100mV @ 10A step FS=300kHz
Output Inductor Selection
The selection of inductor value is based on induc­tor ripple current, power rating, working 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
L=
I=kI
RIPPLEOUTPUT
where k is between 0.2 to 0.4.
Select k=0.3, then
L=
OUT
L=1.7uH
OUT
Choose LOUT=2.2uH, then coilcraft inductor DO5010P-222HC is a good choice.
Current Ripple is calculated as
INOUT OUT
OUT
12V-1.8V1.8V1
××
×
××
×
...(1)
V-VV 1
I=
RIPPLE
INOUT OUT
LVF
12V-1.8V1.8V1
2.2uH12V300kHz
××
OUTINS
...(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 2R5TPE470M9 with 9m are chosen.
integer. Choose N =2.
desire
If low ESR is required, for most applications, mul-
ESRI
N
=
Number of Capacitor is calculated as
Ω×
=
N
N =1.03
The number of capacitor has to be round up to a
20mV
is the value of output capacitors.
OUT
V 20mV
RIPPLE
I2.3A
RIPPLE
×∆
V
RIPPLE
RIPPLE
××
8FC
...(5)
...(3)
...(4)
Rev. 2.0 12/19/05
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NEXSEM
8300kHz100uF
tran
2
∆=×∆+×τ
OUTcrit
ESRCifLL
OUTOUTEEOUT
crit
LL
2
=+×τ
EEcrit
ESRCifLL
0.76H
9m470F7.97us
2
(7.97us)
NX2308
If ceramic capacitors are chosen as output ca­pacitors, 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 2m ESR is used. The amount of output ripple is
∆=Ω×+
V2m2.3A
RIPPLE
4.6mV9.6mV14.2mV
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
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
transient load, if assuming the bandwidth of
STEP
system is high enough, the overshoot can be esti­mated as the following equation.
VESRI
where τ is the a function of capacitor,etc.
where
=+=
V
<
droop
overshootstep
0ifLL
 
LI
×∆τ=
step
V
OUT
@step load DI
crit
−×≥
2LC
2.3A
××
STEP
V
OUT
××
OUT
...(6)
...(7)
put 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 transient spec is mostly like to dependent on the ESR
of capacitor.
Most case, the output capacitor is multiple capaci­tor in parallel. The number of capacitor can be calcu­lated by the following
ESRI
×∆
N
where
 
sient is 100mV for 10A load step.
ESR) is used, the crticial inductance is given as
 
For example, assume voltage droop during tran-
If the POSCAP 2R5TPE470M9 (470uF, 9mohm
Estep
V2LCV
∆×××∆
tranEtran
0ifLL
LI
×∆τ=
step
V
OUT
ESRCV
L
==
crit
9m470F1.8V
Ω×µ×
is true. In that case, the
V
OUT
crit
−×≥
××
EEOUT
I
step
...(9)
...(10)
10A
The selected inductor is 2.2uH which is bigger than critical inductance. In that case, the output voltage tran­sient not only dependent on the ESR, but also capaci­tance.
number of capacitor is
LI
×∆
step
τ=−×
V
OUT
2.2H10A
µ×
=−Ω×µ=
ESRC
EE
1.8V
ESRCVESRCV
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 out-
Rev. 2.0 12/19/05
××××
==
II
∆∆
stepstep
...(8)
ESRI
N
=+×τ
9m10A1.8V
Ω×
=+×
100mV22.2H470F100mV
1.44
=
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×∆
Estep
V2LCV
∆×××∆
tranEtran
×µ×µ×
V
2OUT
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NEXSEM
F ...(11)
F ...(12)
F ...(13)
F ...(14)
OUT minin1
V1gZZ/R
f
OUT in
Z
VZ
NX2308
The number of capacitors has to satisfied both ripple and transient requirement. Overall, we choose N=2.
It should be considered that the proposed equa­tion 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.
=
Z1
=
Z2
=
P1
=
P2
where FZ1,FZ2,FP1 and FP2 are poles and zeros in
the compensator.
The transfer function of type III compensator for
transconductance amplifier is given by:
V 1gZ
e mf
For the voltage amplifier, the transfer function of compensator is
the compensator of transconductance amplifier must satisfy this condition: R4>>2/gm. And it would be desir­able if R1||R2||R3>>1/gm can be met at the same time,
=
V
e
=
To achieve the same effect as voltage amplifier,
Zin
R3
1
2RC
×π××
42
1
2(RR)C
×π×+×
2RC
×π××
2R
×π××
+×+
Vout
233
1
33
1
CC
12
4
CC
12
−×
× +
Zf
C1
C2
R4
R2
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 12/19/05
C3
Figure 3 - Type III compensator using
transconductance amplifier
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R1
Fb
Vref
gm
Ve
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NEXSEM
22.2uH940uF
24.5m940uF
=940uF
20.753.5kHz10.2k
×π×××Ω
210.2k150kHz
237.6kHz3.9nF
==Ω
R=8k
=(-)
210k3.5kHz37.6kHz
Case 1: FLC<FO<F
power stage
Gain(db)
ESR
LC
F
40dB/decade
NX2308
× Ω×
RV 10k0.8V
2REF
1
frequency at 1/10~ 1/5 of the switching frequency. Set FO=25kHz.
V-V1.8V-0.8V
OUT REF
Choose R1=8kΩ.
3. Set zero FZ2 = FLC and Fp1 =F
4. Calculate R4 and C3 with the crossover
ESR
.
loop gain
ESR
F
20dB/decade
compensator
F
Z1
F
Z2
Figure 4 - Bode plot of Type III compensator
(FLC<FO<F
Typical design example of type III compensator in which t he crossover frequency is selected as FLC<FO<F following steps.
1. Calculate the location of LC double pole F
and ESR zero F
and FO<=1/10~1/5Fs is shown as the
ESR
.
ESR
F
=
LC
2LC
×π××
=
O
F
ESR
1
OUTOUT
1
F
P1
F
)
P2
LC
×π××
3.5kHz
=
C=(-)
111
3
2RFF
×π×
×
2z2p1
111
×
×π×Ω
=4.1nF
V2FL
R=C
4out
VC
1.5V225kHz2.2uH
×π××
OSCO
××
in3
×π××
××
12V3.9nF
=10.4k
Choose C3=3.9nF, R4=10.2k.
5. Calculate C2 with zero Fz1 at 75% of the LC
double pole by equation (11).
C
2
=
5.95nF
Choose C2=5.6nF.
6. Calculate C1 by equation (14) with pole Fp2 at
half the switching frequency.
C
1
104pF
Choose C1=100pF.
7. Calculate R3 by equation (13).
=
1
2FR
×π××
Z14
=
=
=
1
2RF
×π××
4P2
×π×Ω×
=
1
1
F
ESR
=
2ESRC
=
1
×π××
OUT
1
×π×Ω×
37.6kHz
=
2. Set R2 equal to10k Ω.
Rev. 2.0 12/19/05
R
=
3
=
1.1k
=Ω
Choose R3 =1.1kΩ.
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1
2FC
×π××
P13
1
×π××
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NEXSEM
22.2uH1500uF
213m1500uF
==Ω
R=12k
=(-)
215k2.77kHz8.16kHz
28.16kHz2.7nF
1.5V230kHz2.2uH15k7.32k
12V13m15k7.32k
×π××Ω×Ω
ΩΩ+Ω
20.752.77kHz19.6k
×π×××Ω
219.6k150kHz
NX2308
Case 2: FLC<F
power stage
Gain(db)
loop gain
compensator
F
Z1
ESR<FO
LC
F
ESR
F
F
Z2
40dB/decade
O
F
P1
F
20dB/decade
F
P2
2. Set R2 equal to 15k Ω.
× Ω×
RV 15k0.8V
2REF
1
V-V1.8V-0.8V
OUT REF
Choose R1=12kΩ.
3. Set zero FZ2 = FLC and Fp1 =F
4. Calculate C3 .
C=(-)
111
3
2RFF
×π×
×
2z2p1
111
×
×π×Ω
=2.5nF
Choose C3=2.7nF.
5. Calculate R3 .
1
2FC
×π××
P13
1
R
=
3
=
×π××
7.22k
=Ω
Choose R3 =7.32kΩ.
6. Calculate R4 with FO=30kHz.
ESR
.
Figure 5 - Bode plot of Type III compensator
(FLC<F
If electrolytic capacitors are used as output capacitors, typical design example of type III compensator in which t he crossover frequency is selected as FLC<F as the following steps. Here one SANYO MV-WG1500 with 13 mΩ is chosen as output capacitor.
1. Calculate the location of LC double pole F
and ESR zero F
F
=
LC
=
ESR<FO
.
ESR
1
2LC
×π××
OUTOUT
)
ESR<FO
and FO<=1/10~1/5Fs is shown
1
LC
×π××
2.77kHz
=
F
=
ESR
2ESRC
=
1
×π××
OUT
1
×π×Ω×
8.16kHz
=
V2FLRR
OSCO23
R=
4
VESRRR = =19.6k
Choose R4=19.6k.
5. Calculate C2 with zero Fz1 at 75% of the LC
double pole by equation (11).
C
2
2.9nF
Choose C2=2.7nF.
6. Calculate C1 by equation (14) with pole Fp2 at
half the switching frequency.
C
1
54pF
Choose C1=56pF.
×π×××
××
in23
+
××
=
=
1
2FR
×π××
Z14
1
=
=
=
1
2RF
×π××
4P2
1
×π×Ω×
=
Rev. 2.0 12/19/05
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NEXSEM
Gain= ... (15)
F= ... (16)
F ... (17)
21.5uH4500uF
26.33m4500uF
××Ω
=10k
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.
For this type of compensator, FO has to satisfy FLC<F
<<FO<=1/10~1/5F
ESR
s.
R2
R1
Vout
Fb
R3
NX2308
C2
C1
Ve
Case 1:
Type II compensator can be realized by simple RC circuit as shown in figure 7. R3 and C1 introduce a zero to cancel the double pole effect. C2 introduces a pole to suppress the switching noise.
To achieve the same effect as voltage amplifier, the compensator of transconductance amplifier must
satisfy this condition: R3>>1/gm and R1||R2>>1/gm. The following equations show the compensator pole zero lo­cation and constant gain.
R
3
R
2
1
z
2RC
×π××
31
p
1
2RC
×π××
32
power stage
Vref
Figure 7 - Type II compensator with transconductance amplifier(case 1)
The following parameters are used as an ex­ample for type II compensator design, three 1500uF with 19mohm Sanyo electrolytic CAP 6MV1500WGL are used as output capacitors. Coilcraft DO5010P­152HC 1.5uH is used as output inductor. See figure
19. The power stage information is that: VIN=12V, VOUT=1.2V, IOUT =12A, FS=300kHz.
1.Calculate the location of LC double pole F
and ESR zero F
=
F
LC
2LC
=
.
ESR
1
×π××
OUTOUT
1
LC
×π××
=
1.94kHz
40dB/decade
Gain(db)
loop gain
20dB/decade
compensator
Gain
F
F
Z LCFESR
F
Figure 6 - Bode plot of Type II compensator
Rev. 2.0 12/19/05
P
O
F
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F
ESR
=
×π××
2ESRC
=
1
OUT
1
×π×Ω×
=
5.6kHz
2.Set crossover frequency FO=30kHz>>F
3. Set R2 equal to10k . Based on output voltage,
using equation 21, the final selection of R1 is 20k Ω.
4.Calculate R3 value by the following equation.
V2FL
R=R
OSCO
32
VESR
in
1.1V230kHz1.5uH 12V6.33m
=37.2k
Choose R3 =37.4k Ω.
×π××
××
×π××
ESR
.
11
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NEXSEM
Gain=gR ... (18)
F= ... (19)
F ... (20)
237.4k0.751.94kHz
p
F
37.4k150kHz
NX2308
5. Calculate C1 by setting compensator zero F
at 75% of the LC double pole.
C=
1
= =2.9nF
Choose C1=2.7nF.
6. Calculate C2 by setting compensator pole
at half the swithing frequency.
C=
2
= =57pF
Choose C2=56pF.
Case 2:
Type II compensator can also be realized by simple RC circuit without feedback as shown in figure 9. R3 and C1 introduce a zero to cancel the double pole effect. C2 introduces a pole to suppress the switching noise. The following equations show the compensator pole zero lo­cation and constant gain.
1
×π××
2RF
3z
1
×π×Ω××
1
π××
RF
3s
1
π×Ω×
R
1
××
m3
R+R
12
Z
1
z
2RC
×π××
p
31
1
2RC
×π××
32
power stage
40dB/decade
Gain(db)
loop gain
20dB/decade
compensator
Gain
F
F
Z LCFESR
F
Figure 8 - Bode plot of Type II compensator
P
O
F
Vout
R2
Fb
gm
R1
Vref
Ve
R3
C2
C1
Rev. 2.0 12/19/05
Figure 9 - Type II compensator with transconductance amplifier
For this type of compensator, FO has to satisfy
FLC<F
tor design. Input voltage is 12V, output voltage is 3.3V, output inductor is 1.5uH, output capacitors are two 680uF with 41m electrolytic capacitors.
and ESR zero F
<<FO<=1/10~1/5F
ESR
The following is parameters for type II compensa-
1.Calculate the location of LC double pole F
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ESR
s.
LC
.
12
Page 13
NEXSEM
21.5uH1360uF
220.5m1360uF
1220.52mA/V
23.57k0.753.5kHz
p
F
3.57k300kHz
OUT
REF
V
2REF
OUT REF
IID1-D
NX2308
1
OUTOUT
1
F
=
LC
2LC
×π××
=
×π××
3.5kHz
=
1
×π××
OUT
1
F
ESR
=
2ESRC
=
×π×Ω×
5.7kHz
=
2.Set R2 equal to10.2k . Using equation 21, the
final selection of R1 is 3.24k Ω.
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 R+R
OSCO 12
R=
3
VRgR
1.5V230kHz1.5uH1
=
=3.55k
Choose R3 =3.57k Ω.
5. Calculate C1 by setting compensator zero F
at 75% of the LC double pole.
C=
= =16.9nF
Choose C1=15nF.
6. Calculate C2 by setting compensator pole
at half the swithing frequency.
×π××
×××
inESRm1
×π××
××
10.2k+3.24k
×
ΩΩ
3.24k
1
1
1
2RF
×π××
3z
1
×π×Ω××
Output Voltage Calculation
Output voltage is set by reference voltage and ex-
ternal 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
V ,
where R2 is part of the compensator, and the
value of R1 value can be set by voltage divider.
Choose R2=15k, to set the output voltage at
1.8V, the result of R1 is 12kΩ.
Z
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:
and voltage divider..
Vout
R2
Fb
R1
Vref
Figure 10 - Voltage divider
RV
R=
1
×
V-V
...(21)
C=
2
= =297pF
Choose C1=330pF.
Rev. 2.0 12/19/05
1
RF
π××
3s
π×Ω×
=××
RMSOUT
V
OUT
D
1
VIN = 12V, VOUT=1.8V, IOUT=10A, using equation (19), the result of input RMS current is 3.6A.
recommended.
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=
V
IN
For higher efficiency, low ESR capacitors are
...(22)
13
Page 14
NEXSEM
P=I(1D)RK
×−××
SWINOUTSWS
PVITF
=××××
gateHGATEHGSLGATELGSS
P(QVQV)F
=×+××
SWLDSON
IR+V
IIR/R
===Ω
R3.375k
NX2308
One Sanyo OS-CON 16SVP180M 16V 180uF 20m with 3.64A RMS rating are chosen as input bulk capacitors.
Power MOSFETs Selection
The NX2305 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 IRFR3709Z are used. They have the following parameters: VDS=30V,R
=6.5m,Q
GATE
=17nC.
There are two factors causing the MOSFET power loss:conduction loss, switching loss.
Conduction loss is simply defined as:
P=IDR
HCONOUTDS(ON)
LCONOUTDS(ON)
P=PP
TOTALHCONLCON
2
×××
2
K
+
...(23)
where the R DS(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 approximately equals to 1.4 at 125oC according to IRFR3709Z datasheet . Conduc- tion 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
...(24)
where IOUT is output current, TSW is the sum of T and TF which can be found in mosfet datasheet, and FS is switching frequency. Swithing loss PSW is frequency dependent.
Also MOSFET gate driver loss should be consid­ered when choosing the proper power MOSFET. MOSFET 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:
DSON
...(25)
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
is the low
LGS
side gate source voltage.
This power dissipation should not exceed maxi­mum power dissipation of the driver device.
Over Current Limit Protection
Over current protection for NX2308 is achieved by sensing current through the low side MOSFET. An inter­nal current source of 40uA flows through an external re­sistor connected from OCP pin to SW node sets the over current protection threshold. When synchronous FET is on, the voltage at node SW is given as
V=-IR×
The voltage at pin OCP is given as
×
OCPOCPSW
When the voltage is below zero, the over current occurs as shown in figure.
vbus
OCP
I
40uA
OCP comparator
OCP
SW
OCP
R
Figure 11 - Over current protection
The over current limit can be set by the following equation
SETOCPOCPDSON
If the MOSFET R
=9m, and the current limit
DSON
is set at 15A, then
× ×Ω
R
IR 15A9m
SETDSON
OCP
Choose R
I40uA
OCP
OCP
=4k
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.
There are two sets of components considered in
Rev. 2.0 12/19/05
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14
Page 15
NEXSEM
NX2308
the layout which are power components and small sig­nal components. Power components usually consist of input capacitors, high-side MOSFET, low-side MOSFET, inductor and output capacitors. A noisy environment is generated by the power components due to the switch­ing power. Small signal components are connected to sensitive pins or nodes. A multilayer layout which in­cludes power plane, ground plane and signal plane is recommended .
Layout guidelines:
1. First put all the power components in the top layer connected by wide, copper filled areas. The input capacitor, inductor, output capacitor and the MOSFETs should be close to each other as possible. This helps to reduce the EMI radiated by the power loop due to the high switching currents through them.
2. Low ESR capacitor which can handle input RMS ripple current and a high frequency decoupling ceramic cap which usually is 1uF need to be practically touch­ing the drain pin of the upper MOSFET, a plane connec­tion is a must.
3. The output capacitors should be placed as close as to the load as possible and plane connection is re­quired.
4. Drain of the low-side MOSFET and source of the high-side MOSFET need to be connected thru a plane ans as close as possible. A snubber nedds to be placed as close to this junction as possible.
5. Source of the lower MOSFET needs to be con­nected to the GND plane with multiple vias. One is not enough. This is very important. The same applies to the output capacitors and input capacitors.
6. Hdrv and Ldrv pins should be as close to MOSFET gate as possible. The gate traces should be wide and short. A place for gate drv resistors is needed to fine tune noise if needed.
7. Vcc capacitor, BST capacitor or any other by­passing capacitor needs to be placed first around the IC and as close as possible. The capacitor on comp to GND or comp back to FB needs to be place as close to the pin as well as resistor divider.
8. The output sense line which is sensing output back to the resistor divider should not go through high frequency signals.
9. All GNDs need to go directly thru via to GND
plane.
10. The feedback part of the system should be kept away from the inductor and other noise sources, and be placed close to the IC.
11. In multilayer PCB, separate power ground and analog ground. These two grounds must be connected together on the PC board layout at a single point. The goal is to localize the high current path to a separate loop that does not interfere with the more sensitive ana­log control function.
Rev. 2.0 12/19/05
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15
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