Transcript aaa
Design of Class-D Audio
Amplifiers
Chun-Hsien Su
中央大學電機系 蘇純賢
[email protected]
May 17, 2006
OUTLINE
1. Introduction of Class-D Audio Amplifier
2. Large-Power Class-D Applications
3. Integrated Class-D Audio Power Stages
4. Sigma-Delta Class-D Audio Amplifiers
5. Conclusions
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Introduction of Class-D Audio Amplifier
– Traditional Class-AB Amplifier
Class AB amplifier uses linear regulating transistors to
modulate output voltage.
η = 30% at temp rise test condition.
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Introduction of Class-D Audio Amplifier
– Class-D Audio Amplifier
Class D amplifier uses MOSFETs that are either ON or OFF.
PWM technique is used to express analog audio signals with
ON or OFF states in output devices.
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Basic PWM Operation
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Audio Output Spectral Density
Fundamental
Carrier and modulated signals
LC-filtered
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Topology Comparison: Class AB vs. Class D
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Efficiency: Class AB vs. Class D
[From TI’s report]
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Measured Efficiency
[From TI’s data]
– TI-TPA2000D4
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Temperature vs. Output Power
– Class-D Advantage: Less Heat
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Battery Life
A head to head test of
TI’s class-AB and class-D
~1W mono solutions:
Class-AB - TPA731
Class-D - TPA2001D
Both set-up on the PnP
platform powered by
3x1.2V NiMH batteries
driving a typical 8-Ω
speaker used in wireless
applications.
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Battery Life
A head to head test of
TI’s class-AB and class-D
~1W mono solutions:
Class-AB - TPA731
Class-D - TPA2001D
Both set-up on the PnP
platform powered by
3x1.2V NiMH batteries
driving a typical 8-Ω
speaker used in wireless
applications.
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Analogy to Buck DC-DC Converter
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Loss in Power Device
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Full Bridge versus Half Bridge
– Full Bridge
– Full Bridge
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Full Bridge versus Half Bridge (Cont.)
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Major Cause of Imperfection
Architecture
Analog/digital
w/SDM
Switch nonidealities
Finite Ron
Body diode Recovery
(EMI)
Poor PSRR
Noise coupling
Feedback
Nonlinear LC
PWM
Audio source
Modulation error
Quantization error
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Gate
Driver
Dead time
Delay time
Single-bridge/Full bridge
Filterless modulation scheme
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THD and Dead Time
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Shoot Through and Dead Time
- Shoot through charge increases rapidly as dead time gets shorter.
- Need to consider manufacturing tolerances and temperature
characteristics.
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Power Supply Pumping
- Significant at low frequency output
- Significant at low load impedance
- Significant at small bus capacitors
- Largest at duty = 25%, and 75%
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EMI consideration: Qrr in Body Diode
1. Low side drains inductor current
2. During dead time body diode of low side
conducts and keep inductor current flow
3. At the moment high side is turned ON after
dead time, the body diode is still conducting
to wipe away minority carrier charge stored
in the duration of forward conduction.
This current generates large high frequency
current waveform and causes EMI noises.
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Gate Driver: Why is it Needed?
Gate of MOSFET is a capacitor to be charged and
discharged. Typical effective capacitance is 2nF.
High side needs to have a gate voltage referenced to it’s Source.
Gate voltage must be 10-15V higher than the drain voltage.
Need to control HS and LS independently to have dead time.
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Functional Block Diagram Inside Gate Driver
High side needs to have a gate voltage
referenced to it’s Source.
With the addition of few components, they
provide very fast switching speeds and low
power dissipation.
Need to control HS and LS independently to have dead time.
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Bootstrap High Side Power Supply
When Vs is pulled down to ground through the low side FET,
the bootstrap capacitor (CBOOT) charges through the
bootstrap diode (Dbs) from the Vcc supply, thus providing a
supply to Vbs.
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Power Dissipation in Gate Driver
Whenever a capacitor is charged or discharged through a
resistor, half of energy that goes into the capacitance is
dissipated in the resistor. Thus, the losses in the gate drive
resistance, internal and external to the MGD, for one complete
cycle is the following:
PG V f SW QG
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Power Dissipation in Gate Driver (Cont’d)
The use of gate resistors
reduces the amount of gate
drive power that is dissipated
inside the MGD by the ratio
of the respective resistances.
These losses are not
temperature dependent.
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MOSFET Power Switch
A MOSFET is a voltage-controlled power switch.
A voltage must be applied between Gate and
Source terminals to produce a flow of current in
the Drain.
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Key Parameters of Power MOSFETs
(1). Voltage Rating, BVDSS : Drain-source breakdown voltage.
Temperature dependent.
(2). Gate Charge, Qg : Directly related to MOSFET speed
Temperature dependent.
(3). D-to-S On-Resistance, RDS(ON) : Directly related to MOSFET
conduction losses. Temperature dependent.
(4). Body Diode Reverse Recovery Characteristics, Qrr, trr , Irr , and S
factor. Influence THD, EMI, and Efficiency. Temperature dependent.
(5). Package : Power dissipation capability, current capability,
internal inductance, internal resistance, electrical isolation, and
mounting process.
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Voltage Rating, BVDSS
This is the drain-source breakdown voltage (with VGS = 0).
BVDSS should be greater than or equal to the rated voltage
of the device, at the specified leakage current, normally
measured at Id=250uA.
This parameter is temperature-dependent and
frequently ∆BVDSS/∆Tj (V/°C) is specified on datasheets.
BVDSS MOSFET voltages are available from tens to
thousand volts.
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Gate Charge, Qg
parameter is directly
related to the MOSFET speed
and is temperatureindependent.
Lower Qg results in faster
switching speeds and
consequently lower switching
losses.
The total gate charge has two
main components: the gate
source charge, Qgs and, the
gate-drain charge, Qgd (often
called the Miller charge).
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D-to-S On-Resistance, RDS(ON)
This is the drain-source
resistance, typically
specified on data sheet at
25°C with VGS = 10V.
RDS(ON) parameter is
temperature-dependent, and
is directly related to the
MOSFET conduction losses.
lower RDS(ON) results in
lower conduction losses.
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Body Diode Reverse Recovery Characteristics, Qrr, trr , Irr , and S Factor
Power MOSFETs inherently have
an integral reverse body-drain
diode. This body diode exhibits
reverse recovery characteristics.
Reverse Recovery Charge Qrr,
Reverse Recovery Time trr,
Reverse Recovery Current Irr and
Softness factor (S = tb/ta), are
typically specified on data sheets
at 25°C and di/dt = 100A/us.
Power recovery characteristics
are temperature-dependent and
lower trr, Irr and Qrr improves
THD, EMI and Efficiency η.
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Package
MOSFETs devices are available in several packages as
SO-8,TO-220, D-Pak, I-Pak, TO-262, DirectFET™, etc.
The selection of a MOSFET package for a specific
application depends on the package characteristics such
as dimensions, power dissipation capability, current
capability, internal inductance, internal resistance,
electrical isolation and mounting process.
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Choosing the MOSFET Voltage Rating
MOSFET voltage rating for a Class D amplifier is determined by:
– Desired POUT and load impedance (i.e. 250W on 4Ω)
– Topology (Full Bridge or Half Bridge)
– Modulation Factor M (80-90%)
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Trends in Class-D Audio Amplifiers
– Make it smaller!
higher efficiency
smaller package
Half Bridge
– Make it sound better!
THD improvement
fully digitally processed modulator
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Trends in Class-D (1)
– Patent Blooming since Y2K
US Patent Class 330/207A – Class-D Amplifier
50+
Patent #
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Trends in Class-D (2)
– Systems by ICs
Bipolar
CMOS
DMOS
(doublediffused
MOS)
DMOS features:
• It is a (lateral) double-diffused MOS transistor.
• The device is asymmetrical.
• A lightly doped Nwell(extended drain) region supports high drain voltages.
• The thin gate oxide allows a high device but restricts
• The Pbody is shorted to source of device in metal 1.
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Trends in Class-D (3)
– Full versus Half, Performance versus Cost
Full Bridge
Half Bridge
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Trends in Class-D (4)
– Performance Improved by Analog FB Loop
US Patent : 6300825, issued 2001/10/9
“PWM with feedback loop Integrator”
Similar: Yokoyama 4504793
1985/3/12
This structure improves output waveform & PSRR.
This patent can be avoided by using different architecture.
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Trends in Class-D (5)
– Filterless Modulation for Portable Applications
Gate
Driver
Information in pulse width
Information in phase
US Patent : 6262632, issued 2001/7/17
“Concept and method to enable filterless, efficient operation of Class-D amplifiers”
Limits the development of small-power (~1W) class-D amplifier.
Can be solved by using different modulation schemes.
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Trends in Class-D (6)
– Performance Improvement by Sigma-Delta?
PWM
Delta
Sigma
-Delta
The power efficiency and the signal-to-noise
ratio (SNR) for a amplifier based on the
above scheme are compared with the values
typical of linear and PWM amplifiers of the
same rated power. The power efficiency of
the solution is an intermediate value
between the linear and PWM amplifiers,
whereas SNR mainly depends on the
modulator type adopted. A SNR around 60–
70 dB was estimated by adopting a fourthorder modulator. However, this value can be
significantly improved by increasing the
switching frequency or the modulator order.
[Dallago, Tran. CAS-I, Aug, 1997]
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Trend in Class D Amplifiers
In any case, to extend the power range of high-frequency
modulation, future studies should be oriented in the following
direction:
(1). Reduction of power circuit parasitic capacitance by technological
improvement of both semiconductor and magnetic devices;
(2). Adoption of soft-switching schemes able to perform a larger
exploitation of converter parasitic parameters under a load range
that is as wide as possible;
(3). development of extended modulation techniques (for example of
multilevel type or nonconstant switching period type or, generally,
of hybrid type) allowing a lower switching frequency under the
same baseband performance.
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PWM versus PDM
THD
Class-D
CT SDM
Comparator Run-free
Clocked
Output
PWM
1-b PDM
Min. pulse
Width
1/fs
fs<1MHz
1/fs
fs>1MHz
Drive
H-bridge
OK
May burn out
PWM
1-bit
PDM
For second-order M
fs=40kHzx128=5.12MHz
Open-loop, Full-bridge, low-OSR M with bit grouping
Audio source
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High-order
Single-bit
M
Bit flipping
(bit grouping)
(digital)
(digital)
Gate
Driver
(d & a)
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Class-D Amplifier
Dual noise-shaper architecture - Simple, almost all digitized
Audio
source
Digital
M
PCM
Interpolator
+
-
Noise
Shaper
PCM
Interpolator
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Grouping
Gate
Driver
Waveform
Represent
m-bit
AD
1/m-bit
DAC
CT
filter
Noise
Shaper
Class D
Amplifier
Class AB Speaker
/Class D
Amplifier
Speaker
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Conclusion
– Highly efficient Class D amplifiers now provide similar
performance to conventional Class AB amplifiers - If key
components are carefully selected and the layout takes into
account the subtle, yet significant impact due to parasitic
components.
– Constant innovation in semiconductor technologies helps the
growing Class D amplifiers usage due to improvements in
higher efficiency, increased power density and better audio
performance. Trends in class-D: half-bridge filterless
scheme, analog-feedback loop to improve performance.
– All-digital Sigma-delta class-D Future work.
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References
[1]. M. Berkhout, “An integrated 200-W Class-D audio amplifer,” IEEE J.
Solid-State Circuits, vol. 38, pp. 1198–1206, July 2003.
[2]. H. Ballan, M. Declercq, and J. U. Duncombe, “12 V - Class-D
amplifier in 5 V CMOS technology,” in Proc. IEEE CICC, 1995, pp.
559–562.
[3]. E. Dallago, “Advances in high-frequency power conversion by deltasigma
modulation,” IEEE Trans. Circuits Syst. I, vol. 44, pp. 712–721,
Aug. 1997.
[4]. Marco Berkhout, “An integrated 200 W class-D audio amplifier,” IEEE J.
Solid-State Circuits, vol. 38, no. 7, pp. 1198–1206, Jul. 2003.
[5]. Jun Honda and Jorge Cerezo, IRA Technical Report.
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