Control of Boost type Converter in Discontinuous Conduction Mode

Control of Boost type Converter in Discontinuous Conduction Mode by Controlling the Product of
Inductor Voltage-Second
Chongming (Michael) Qiao, Jason Zhang
International Rectifier
233 Kansas Street, El Segundo, CA 90245 USA
[email protected]; [email protected]
As presented at PESC 2005 - Recife, Brazil
Abstract: Battery-operated systems such as cell-phone, digital
camera become more and more popular. In these applications,
a boost-type converter is usually required to convert low
battery voltage to higher voltage. In this paper, a variable
frequency control of boost converter is discussed. The prototype circuit is built to prove the concept. The extension of this
approach in Power Factor-Correction application is discussed.
II
PROPOSED CONTROLLER FOR BOOST
CONVERTER WITH INDUCTOR CURRENT
SENSING
The proposed controller for boost converter with inductor
current sensing is shown in Figure 1.
I
D1
L
Vin
Vout
+
S1
Rload
Cout
Rs
GND
Drv
Q
10mV
+
200mV
Isen
R S
Reset Dom
SR1
S
R
Q
Reset dom
SR2
VCC
Q1
+
INTRODUCTION
Battery-operated systems such as digital camera, TFT-LCD
bias supplies, require a boost converter to step up the low
battery voltage to higher voltage. For these applications, it
is very important to extend the battery life. Therefore,
efficiency is critical even at light load condition. Fixed
frequency PWM control is very popular. Two items related
to PWM boost converter is a concern for customers. First, if
the boost converter is operated in the continuous–conduction
mode (CCM), there is a right half plane zero, which is
difficult to be stable. The discontinuous conduction mode is
desired for low power application. Second, at light load,
boost converter is difficult to regulate because PWM
controller typical has certain minimum on time and the on
time of switch at fixed frequency will keep pumping energy
to output and it will cause over voltage at very light load or
no load condition.
In this paper, another approach is investigated. This
approach controls the boost converter always in
discontinuous conduction mode by forcing the product of
inductor voltage-second to be zero in each switching cycle.
By doing so, the stability of system is always guaranteed and
no compensation network is required. In addition, the
proposed control has natural power limit and will prevent the
boost converter from being over stressed by over load.
Since it operates in variable frequency, at light load, the
frequency is very low and it helps regulate the output
voltage as well as offer better efficiency since low switching
loss is resulted. The concept can be implemented by sensing
inductor current or switching current with an integrator.
One extension of the approach to control of Power Factor
Correction is also proposed. The experimental result is
provided to prove the concept.
FB
C_dly
Programmable
delay
Vref
Figure 1. Proposed control approach diagram for a boost converter.
Vin
Inductor
voltage
0
Vin-Vout
inductor
current
voltage
across
sensing
resistor
Drv
0A
200mV
10mV
C_dly
FB
comparator
output
t1
t0
t2
t3
Operation at regulation mode
Figure 2. Operation waveforms at regulation mode.
This control has two operation mode, regulation mode and
power limit mode. At regulation mode, the waveform is
shown in Figure 2. The inductor operates at discontinuous
conduction mode and the output voltage is regulated at
desired output voltage
1.
Regulation Mode
The operation concept is as follows.
First, during time t0~t1, Latch SR2 outputs logic High and
the switch is on. The inductor current linearly increases from
zero. When the voltage at sensing resistor Rs reaches the
current threshold VIL _ TH for example 200mV, Latch SR1
and SR2 are reset to zero. The switch is turned off at t1. The
inductor voltage is given as
VL ( 0 ~ t1 ) = VIN
The peak inductor current is given as
V
= IN × t1 --------------(1)
L
The peak inductor current is limited by the current threshold
VIL _ TH and current sensing resistor.
iL _ peak =
VIL _ TH
RS
where VIL _ TH = 200mV ---(2)
Combination of above two equations results in
t1 =
VL ( t1 ~ t2 ) = VIN − VOUT .
The following equation exists based on inductor voltagesecond balance.
VIN × t1 + (VIN − VOUT ) × ( t2 − t1 ) = 0
t2 − t1 =
Q1
iL _ peak
to High. This will enable the SET of latch SR2 to be
controlled by feedback comparator. If we neglect 10mV, the
inductor current reduced to zero at t2. The voltage across
the inductor is
VIL _ TH × L
RS × VIN
--------------------(3)
From t1 to t2, the inductor current decreases. Before the
voltage across the sensing resistor reaches 10mV, the output
of latch SR1 keeps low and switch holds off. At time t2, the
voltage across current sensing resistor reaches 10mV and the
inductor current decreases to almost zero, the latch Sr1 is set
VIN
× t1 ------(4)
VOUT − VIN
From t2 to t3, the output voltage is discharged through
output load until the output voltage is below reference
voltage. At t3, the FB comparator goes high and SET the
latch SR2. Switch is ON again and another cycles starts.
The programmable delay is added as an option to ensure the
inductor current goes to zero.
Since the inductor current reaches zero in each cycle, the
input power will be the energy stored in the inductor divided
by switching period.
The input power is given as
PIN =
1
2
× L × iL2 _ peak
TS
-----------(5)
where Ts is the switching period. Substitution of equation
(2) into above equation results in
PIN =
L × VIL2 _ TH
2 × RS2 × TS
-------------(6))
Since the inductor current is discharged to zero in each
cycle, the energy stored in the inductor is transferred to the
load in each cycle. If assuming the efficiency is 100%, the
input power will be equal to output power.
PIN = POUT = VOUT × I OUT -----(7)
Substitution of equation (6) into above equation results in
FS =
2 × RS2 × VOUT × I OUT
-------------(8)
L × VIL2 _ TH
where Fs is the switching frequency and
FS =
1
.
TS
Since at regulation mode, the output voltage equals nominal
output voltage.
VOUT = VOUT _ nom . The equation (8) can be written as
FS =
2 × RS2 × VOUT _ nom × I OUT
L × VIL2 _ TH
---------(9)
The above equation shows that the switching frequency
linearly increases when load current goes up.
2.
Power Regulation Mode
Where I OUT _ reg is maximum load output current with
Vin
inductor
voltage
regulated output voltage VOUT _ nom .
0
Vin-Vout
During the power limit mode, the switch period is given as
TS = t2 = t1 + ( t2 − t1 )
inductor
current
voltage
across
sensing
resistor
Drv
200mV
10mV
FS =
C_dly
tied to VCC
0
t1
High
t2
0
Operation at power limit mode
Figure 3. Operation waveform at power limit mode with C_ldy=VCC
When load current keeps going up, eventually the inductor
will operate in the boundary of Continuous Conduction
Mode (CCM) and Discontinuous Conduction Mode (DCM).
The concept of this control is that the switch is turned on
only after the inductor current reaches to zero. This concept
will limit the maximum power that the input can deliver.
When load current is high enough, the output power will
reach the input power limit. The output voltage will be no
longer regulated and it will keep decrease as load current
increase. The operation waveform is shown in Figure 3. At
power limit mode, since the output voltage is lower than
regulation, the FB comparator output is always high. The
switch is simply controlled by the latch SR1 and current
sensing comparator. The switch is on when inductor current
reaches low threshold such as 10mV and turn off when
inductor current reaches high threshold. The average
inductor current is given as
1
1 VIL _ TH
iL _ avg = × iL _ pk = ×
------(10)
RS
2
2
Input power equals output power, therefore
PIN = VIN × I L _ avg = POUT = VOUT × I OUT
Substitution of equation (10) into above equation results in
VOUT =
VIL _ TH × VIN
2 × RS × I OUT
⎛
R ×V
V
1
= S IN × ⎜1 − IN
TS VIL _ TH × L ⎝ VOUT
⎞
⎟ ---(13)
⎠
⎛ 2 × RS × I OUT
R ×V
1
= S IN × ⎜1 −
TS VIL _ TH × L ⎜⎝
VIL _ TH
⎞
⎟⎟ --(14)
⎠
The above equation shows that the frequency will decrease
when load current increases. Overall, the relationship
between output voltage, frequency and load current is shown
in Figure 4. The peak frequency occurs at the transition
between regulation mode and power limit mode. At
transition time, VOUT = VOUT _ nom
Substitute of above equation to equation (13) results in the
maximum operation frequency
FS _ max =
⎛
R ×V
VIN ⎞
1
= S IN × ⎜1 −
⎟ ----(15)
TS VIL _ TH × L ⎜⎝ VOUT _ nom ⎟⎠
Average
input
current
Switching
Frequency
Output
voltage
regulation mode
Power limit mode
Io(MAX) Load current
---------(11)
The above equation shows that the output voltage will be
reduced when output current goes up. The maximum load
current with regulated output voltage will be
I OUT _ reg =
FS =
Substitution of equation (11) into above equation results in
Q1
FB
comparator
output
Substitution equation (3) and (4) into above equation, we
have
VIL _ TH × VIN
2 × RS × VOUT _ nom
-----(12)
Figure 4. Theoretical characteristics for the boost converter with proposed
control approach.
With this control approach, at each cycle, the voltagesecond product of inductor is always reset to zero and
inductor current always goes to zero before another cycle
starts. Ideally, the threshold voltage to ensure inductor
current decreases to zero should be 0mV. However, in
reality, since comparator has offset and 10mV is used to
compensate the comparator offset. Additional delay can be
generated by putting extra cap at “C_dly” pin. The
programmable delay is to ensure inductor current fully going
to zero before other cycles starts
. From equation (3), the switch ON time is fixed if the input
voltage is fixed, the operation principle will be similar to
constant on-time control and the output voltage is regulated
by changing the off time and switching frequency. The
characteristics of this control is shown in Figure 4. Before
load current reaches critical current Io(MAX), the output
voltage is regulated to desired output. The switching
frequency increases as load current increases. At light load,
the switching frequency can be very low and efficiency is
high comparing to fixed PWM control. This feature is
usefully for battery-operated application because of energy
saving at idle mode. When load current keeps increasing
and inductor current starts to operate at the boundary of
Discontinuous and Continuous mode due to the nature of
control. The system goes into power limit mode as shown in
Figure 3. In this mode, the average inductor current is fixed
and output voltage starts to goes down as load current
increases. And the switching frequency also goes down due
to longer turn off time. This control approach has natural
power limit, which is useful at over load condition as well as
soft start. Overall, the following features is summarized as
• Variable frequency control. At light load, frequency
goes down and system efficiency is relatively high. This
is beneficial for battery operated systems
• System is self stable, no output loop compensation
network required.
•
Natural current limit. No soft start is required since the
output starts up with limited power.
• Switch turns on at zero current results in low switching
loss.
• Simple implementation and easy to be integrated into
IC.
The drawback of the proposed control is that the output
and the input do not share a common ground. This can be
relieved by putting the inductor sensing resistor in series
with inductor as shown in Figure 5. This requires highspeed differential comparator and it is limited to low input
voltage application as well. But it will be a good choice for
battery operated systems such as white LED driver
application.
D1 Vout
L
Rs
Vin
+
Rload
Cout
S1
Isen Drv
VCC
GND
FB
Figure 5. Boost controller with proposed control and
differential inductor current sensing.
III
EXPERIMENTAL VERIFICATION
R9
D1
L1 coilcraft 5010p-223HC
Vin
J3
J2
C2
0.05
22uH
Vin
2
1
R10
9.1k
1N5140
1
2
C4
100uF
Q2
2N3904
R7
CON2
R6
1k
20V,15uF,80mohmESR
CON2
Q4
IRF1010E/TO
10
Q3
2N3906
R11
2.4k
13
10
Q2
U11C
FB
U11D
74HC02
74HC02
12
11
U9A
LM319
3
6
9
8
-5V
U5A
set1
12
11
74HC00
U11A
2
R4
190
1uF -5V
J4
JUMPER
1
3
C7
LM319
-5V
74HC02
Vref
R15 100p
5V
R1
1k
TL431/TO
Q1
C1
1uF
11
U4
C9
1
5 -
C14
10uF
1uF
R12
1k
1
R3
1k
Vref
5VC10
2
4 +
CON2
5V
2
5V
1uf
6
3
2
1
4
U10A
R5
20
11
C3
1uF
J1
C6
5V
5V
3
-5V
5
+
5VC5
-
12
R16
1k
9 +
5V
U5B
100
R13
1k
u11B
7
10 -
2N3904
U7
LM431/TO
4
reset1
6
8
R14
10k
5
Q1
D2
1N5139
6
LM319
74HC02
R2
2.5k
Figure 6. Schematic of a prototype circuit using differential inductor current sensing.
A small power prototype was built to verify the concept.
The schematic is shown in Figure 6. The experiment
waveforms for start up and normal operation are shown in
Figure 7, Figure 8 and Figure 9. The comparison between
experimental results and theoretical prediction for output
voltage and frequency versus output current is shown in
Figure 10 and Figure 11. System specification is as follows:
Vin=3.4V. Vout=12.5V. Cout=15uF with 80mohm ESR,
Current sensing resistor is Rs=0.05ohm and input inductance
is L=22uH. The proposed control offers better efficiency at
light load, natural current limit and simple implementation.
Figure 7. Operation waveforms during the start up.
1uF
Frequency versus output current
30
Frequency (kH
25
20
15
10
5
0
Figure 8. Operation waveforms at regulation mode.
0
500
1000
Iout(mA)
Fs(KHz) experimental
Fs(KHz) theoretical
Figure 11. Comparison between experimental results and theoretical
prediction for frequency versus output current.
IV
.
Figure 9. Operation waveform at power limit mode.
Output voltage versus output current
14
12
Vout(V)
10
8
6
4
2
0
0
500
1000
1500
IOout(mA)
Vout(v) experimental
Vout (theoretical)
Figure 10. Comparison of output voltage versus output current (theoretical
and experimental)
EXTENSION I – PWM CONTROL WITH
SWITCHING CURRENT SENSING
The proposed concept can be applied to use switching
current as well. The basic concept of this approach is to
ensure inductor voltage-second going to zero or inductor
current going to zero before next cycle starts. This is
achieved by using integrator to emulate the inductor current
as shown in Figure 12. The operation waveforms are shown
in Figure 13. When switch is ON, a capacitor “Cint” is
charged by an internal current source that is proportional to
VCC(=Vin). When switching current reaches threshold at
200mV/Rs, the switch is turned off. Then the capacitor
“Cint” is discharged by current source proportional to (VoutVin). Until the capacitor voltage is discharged to a preset
voltage such as 200mV, the latches are enabled for SET,
which is controlled by the feedback comparator. The
capacitor voltage will emulate the inductor current. If the
current source voltage coefficients are identical, when the
capacitor voltage is discharged to preset voltage, the
inductor-second product will go to zero and the theoretical
inductor current will go to zero. Figure 14 shows a simulated
operation waveform for a 5V to 12V application.
D1
L
Vin
0
Vin-Vout
Vout
S2
S1
+
Vin
Rload
Cout
Rs
Drv
0A
200mV/Rs
Switching
current
VOUT
+
VCC
inductor
current
VCC
1V
Cint
200mV
Cint
Drv
200mV
+
GND
200mV
Reset
Dom Q1
S
Q
R
Q
R S
Q1
Reset
dom
C_dly
+
Isen
FB
C_dly
Programmable
delay
FB
comparator
output
Vref
Figure 13. Operation waveforms for proposed control with switching
current sensing.
Figure 12. Proposed controller for boost converter with switching current
sensing.
Comparing with the approach using inductor current
sensing, this scheme offers same feature such as natural
current limit and variable frequency control as well as
additional features.
• Switching current is sensed. It is convenient for small
power application with monolithic IC implementation,
where switch is integrated inside IC.
• Sensing switching current will result in lower losses
comparing with inductor current sensing.
• Common ground between input and output.
It can be easily extended to buck-boost type converter as
shown in Figure 15, with three more features. (1) Output can
be either higher or lower than input. (2) The output can be
short to ground with current limit. (3) The output can be shut
down.
Figure 14. Simulation waveforms for 5V to 12V application with proposed
control in Figure 12.
S2
L
Vout
S2
M1
Vin
S1
+
Cout
Rload
Rs
VCC
Drv2
gnd
Isen
Drv1
Proposed controller
Vout
FB
Cint
C_dly
Figure 15. Buck boost converter with proposed controller and switching
current sensing.
V
EXTENSION II - PFC CONTROL AT
BOUNDARY OF DISCONTINUOUS AND
CONTINUOUS MODE
D1
L
Vin
Inductor
current
Vout
+
Vin
Vac
S2
Rload
Cout
COMP
-
Cint
Rs
Drv
GND
Drv
R
S
Q
SET
VCC
Reset
Dom
FB
10mV
+
gm
300mV
C_int
SS
+
Isen
Figure 17. Theoretical operation waveforms for proposed PFC controller..
Vref
Current Limit
Comparator
COMP
Figure 16. Proposed PFC controller operates in boundary of CCM and
DCM.
The same concept can be applied to control PFC (power
factor correction). The diagram is shown in Figure 16 and
operation waveforms are shown in Figure 17 and simulation
result is shown in Figure 18. Instead of using multiplier and
sensing input voltage shown in previous article, the on time
of switch is controlled by comparing with output of error
amplifier and a ramp generated by a constant current source.
Since the On time is almost constant during a line cycle if
the voltage loop is slow enough, the peak inductor current
will be linearly proportional to the input voltage and
inductance. The switch is turned on again when the inductor
current reaches almost zero (10mV/Rs). By this operation,
the inductor current operates in the boundary of
Discontinuous Conduction Mode (DCM) and Continuous
Conduction Mode (CCM). The average input current will be
proportion to input voltage and unit-power-factor is
achieved.
The load regulation is achieved through
modifying the switch ON time by voltage compensation
loop. An open loop simulation waveform is shown in Figure
18. Comparing with previous approach such as L6561 from
ST, this approach does not require high precision multiplier
and no input voltage sensing is required. This is simple and
less noise sensitive.
Figure 18. Simulated waveform for a line cycle.
VI
CONCLUSION
A new approach to control the boost type converter in
discontinuous conduction mode is proposed. This approach
offers variable frequency control and natural current limit.
Two extensions are derived. One approach uses switching
current and an integrator to emulate the inductor current.
The other extended approach provides simple PFC control.
References
[1]. IRU3065
datasheet.
http://www.irf.com/technicalinfo/refdesigns/irdc3065.pdf.
[2]. ST L6561 datasheet,
http://www.st.com/stonline/books/pdf/docs/5109.pdf