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Prof R T KennedyProf R T Kennedy POWER ELECTRONICS 2POWER ELECTRONICS 2 11
Prof R T Kennedy POWER ELECTRONICS 2 2
Class D audio amplifiers
switching - PWM amplifiers
-Vcc
Prof R T Kennedy POWER ELECTRONICS 2 3
C
R
L
C
R
L
C
R
L
Prof R T Kennedy POWER ELECTRONICS 2 4
+
-
gatedriver
load
L
C
SYNCHRONOUS BUCK SMPS
+
-E /A gate
driverload
L
C
+
-
gatedriver
load
L
C
CLASS ‘D’ AMPLIFIER
Prof R T Kennedy POWER ELECTRONICS 2 5
+
-
gatedriver
load
L
C
SYNCHRONOUS BUCK SMPS
the reference signal is a DC voltage from the error amplifier output
determined by sensing the output voltage switch duty cycle
load current is unidirectional from source to load
Prof R T Kennedy POWER ELECTRONICS 2 6
+
-
gatedriver
load
L
C
SYNCHRONOUS BUCK SMPS
the MOSFETs are optimised differently • higher duty cycle mosfet optimised for lower on-state resistance
• lower duty cycle mosfet optimised for lower gate charge
Prof R T Kennedy POWER ELECTRONICS 2 7
+
-E /A gate
driverload
L
C
+
-
gatedriver
load
L
C
CLASS ‘D’ AMPLIFIER
the reference signal is a continuously varying audio signal
resulting in a continuously varying switch duty cycle
load current in the half-bridge class 'D' amplifier is bidirectional
inductor energy from one half of the bridge is returning to the supply
Prof R T Kennedy POWER ELECTRONICS 2 8
+
-E /A gate
driverload
L
C
+
-
gatedriver
load
L
C
CLASS ‘D’ AMPLIFIER
• both mosfets are optimised for low on-state resistance
Prof R T Kennedy POWER ELECTRONICS 2 9
PWM
25 kHz
400 kHz
Prof R T Kennedy POWER ELECTRONICS 2 10
+
-
gatedriver
load
L
C
SYNCHRONOUS BUCK SMPS
the filter capacitor is selected to
• store energy and smooth the output DC voltage low esr to minimise losses
the inductor is selected to minimise ripple current
• the inductor core material is based on energy storage & losses
and not to saturate at the DC current level
Prof R T Kennedy POWER ELECTRONICS 2 11
+
-E /A gate
driverload
L
C
+
-
gatedriver
load
L
C
CLASS ‘D’ AMPLIFIER
the LOW PASS filter corner frequency is selected to
attenuate the switching noise in the output waveform
pass the audio signal to the loudspeaker
capacitor selected to have minimum capacitance change versus voltage to reduce
distortion
Prof R T Kennedy POWER ELECTRONICS 2 12
+
-E /A gate
driverload
L
C
+
-
gatedriver
load
L
C
CLASS ‘D’ AMPLIFIER
INDUCTOR selected
not to saturate at the DC current level
to have minimum inductance change versus load current (< 10%) core material selected based on harmonic distortion and low hysteresis loss
Prof R T Kennedy POWER ELECTRONICS 2 13
gatedriv
e
L
C
gatedriv
e
L
C
Prof R T Kennedy POWER ELECTRONICS 2 14
Prof R T Kennedy POWER ELECTRONICS 2 15
L
C
gatedriv
e
L gatedriv
e
L
C
gatedriv
e
L gatedriv
e
Prof R T Kennedy POWER ELECTRONICS 2 16
• Half-Bridge simpler & lower cost
• Full-Bridge has better audio performance differential output structure can inherently cancel even
order harmonic distortion DC offsets
• feedback from the output in H-B compensates for variation in the ± bus voltages (voltage pumping)
• open loop class ‘D’ operation is common in FB
Prof R T Kennedy POWER ELECTRONICS 2 17
a few nano-seconds
gate switching timing error
produces non –linearity >1% of THD
on off
offon
highside deadtime
lowside deadtime
Prof R T Kennedy POWER ELECTRONICS 2 18
• Higher efficiency, increased power density and better audio performance are driving the increased use of Class D amplifiers; an approach first proposed in 1958.
• A Class D audio amplifier is basically a switching amplifier or PWM amplifier with the switches being either fully on or fully off resulting in reduced transistor power losses and higher efficiency (90-95%).
Prof R T Kennedy POWER ELECTRONICS 2 19
POWER requirements vary considerably dependent on the application
application specific power supplies needed to optimise the system performance
UNDER-DESIGNED power supplies amplifier does not meet
performance specifications
OVER-DESIGNED power supplies increase product cost
Prof R T Kennedy POWER ELECTRONICS 2 20
POWER SUPPLY OUTPUT VOLTAGE AND CURRENT FACTORS
• amplifier output power• rated amplifier power @ min supply output
voltage• load (speaker) impedance • amplifier output configuration single-ended or BTL (bridge-tied load) output• amplifier maximum achievable duty cycle • parasitic output path resistance • under-voltage lockout to avoid poor low input voltage performance• output voltage 'pumping'
Prof R T Kennedy POWER ELECTRONICS 2 21
Vpower supply
Ipower supply
Ppk
POWER
2
1
2
,
2
,
2
,
pkloadav
load
pkloadav
rmsloadav
PP
R
VP
R
VP
MAXIMUM ‘UNDISTORTED‘
POWER
Prof R T Kennedy POWER ELECTRONICS 2 22
Vload
Iload
Ppk
POWER
22
max,,
2
2
,
2
2
,
2
,
2,
2
)(
2
2
total
loadccswloadav
total
loadpkloadav
paraload
loadpkloadav
loadparaload
rmsloadav
loadrmsloadav
R
RVDP
R
RVP
RR
RVP
RRR
VP
RIP
Rparasitic
RloadVamp
Prof R T Kennedy POWER ELECTRONICS 2 23
avHBT
loadCCswavFB P
R
RVDP ,2
2max,
, 42
)(
48
)( ,2
2max,
,avFB
T
loadCCswavHB
P
R
RVDP
Prof R T Kennedy POWER ELECTRONICS 2 24
RT : sum of all of the DC resistances in series with the load:
RT = Rload + Rdson + Rind + Rpcb + Rps,out
Rload : loudspeaker resistance:
Rdson : mosfet on -state resistance: HB Rdson FB 2 Rdson
Rind : filter inductor DC resistance
Rpcb : board traces, connectors, and wires
Rps,out : power supply output impedance
(use the component's resistance at maximum operating temperature)
• Dsw,max: amplifier maximum output duty cycle
Dsw is also referred to as the modulation index (M)MMAX is the maximum modulation factor
Prof R T Kennedy POWER ELECTRONICS 2 25
amplifier peak output power occurs at loudspeaker's peak voltage or peak current
avHBT
loadout
T
loadoutloadoutpkHB P
R
RV
R
RVRIP ,2
2
2
22
, 24)2(
avFBT
loadoutloadoutFBpk P
R
RVRIP ,2
22 2
Prof R T Kennedy POWER ELECTRONICS 2 26
power supply voltage is determined at the lower limit
of the power supply's output voltage tolerance
based on the amplifier's rated output power
with unclipped output voltage
Prof R T Kennedy POWER ELECTRONICS 2 27
tolerance
VV
R
P
D
R
RD
RPV
CCFBnomCCFB
load
FB
sw
T
loadsw
TFBCCFB
1
2
)(
)(2
min,,
max2
max
2
min,
tolerance
VV
R
P
D
R
RD
RPV
CCHBnomCCHB
load
HB
sw
T
loadsw
THBCCHB
1
22
)(
)(8
min,,
max2
max
2
min,
Prof R T Kennedy POWER ELECTRONICS 2 28
)(max
)(max
amp
ampoutPSout
PP
T
CCswit R
VDI min,max,
min,lim
Prof R T Kennedy POWER ELECTRONICS 2 29
PFB,max amplifier maximum output power
20 W
ηmax amplifier maximum efficiency 90%
Dswmax amplifier maximum duty cycle
0.8
Rload amplifier loudspeaker impedance
8 Ω
RT total output resistance 8.2 Ω
power supply output voltage tolerance
±10 %
Prof R T Kennedy POWER ELECTRONICS 2 30
Vtolerance
VV
VV
R
P
D
R
RD
RPV
CCCCnom
CC
load
FB
sw
T
loadsw
TFBCC
466.251.01
919.22
1
919.228
202
8.0
2.8
2
)()(
)(2
min
min
max2
max
2
min
Prof R T Kennedy POWER ELECTRONICS 2 31
AR
VDI
T
CCswit 236.2
2.8
919.228.0minmaxminlim
WP
Pamp
ampoutPSout 22.22
9.0
20
)(max
)(max
Prof R T Kennedy POWER ELECTRONICS 2 32
Prof R T Kennedy POWER ELECTRONICS 2 33
Prof R T Kennedy POWER ELECTRONICS 2 34
Cell Phone Application for TI's TPA2012D2 Class D Amplifier