The TDA1560Q contains a mono class-H BTL output
power amplifier. At low output power, up to 10 W, the
device operates as a normal BTL amplifier. When a larger
output voltage swing is required, the internal supply
voltage is lifted to approximately twice the external supply
voltage. This extra supply voltage is obtained from the
charge in the external electrolytic capacitors. Due to this
momentarily higher supply voltage, the maximum output
power is 40 W typical at a THD of 10%.
In normal use, when the output is driven with music-type
signals, the high output power is only required for a small
percentage of the time. Assuming a music signal has a
normal (Gaussian) amplitude distribution, the reduction in
dissipation is approximately 50% when compared to a
class-B output amplifier with the same output power.
The heatsink should be designed for use with music
signals.
If the device is continuous sine wave driven, instead of
driven with music signals and at a high output power
(class-H operation), the case temperature can rise above
120 °C with such a practical heatsink. In this event, the
thermal protection disables the high power supply voltage
and limits the output power to 10 W and the maximum
dissipation to 5 W.
The gain of each amplifier is internally fixed at 30 dB. With
the mode select input the device can be switched to the
following modes:
• Low standby current (<50 µA)
• Mute condition, DC adjusted
• On, operation in class-B, limited output power
• On, operation in class-H, high output power.
The open voltage on the class-B/class-H pin is related to
the global temperature of the crystal. By measuring this
voltage, external actions can be taken to reduce an
excessive temperature (e.g. by cutting off low frequencies
or externally switching to class-B). For the relationship
between the crystal temperature and the voltage on this
pin, see Fig.3.
By forcing a high voltage level on the class-B/class-H pin,
thereby simulating a high temperature, the device can be
externally switched to class-B operation. Similarly, by
forcing a low voltage level on the class-B/class-H pin,
thereby simulating a low temperature, the device can be
forced into class-H operation, even if the case temperature
exceeds 120 °C.
The device is fully protected against short-circuiting of the
outputs to ground or V
and across the load, high crystal
P
temperature and electrostatic discharge at all input and
output pins. In the event of a continuing short-circuit to
ground or VP, excessive dissipation is prevented because
the output stages will be switched off. The output stages
will be switched on again within 20 ms after the
short-circuit has been removed.
A diagnostic facility is available at pin 14. In normal
conditions the voltage at this pin will be the supply voltage
(VP). In the event of the following conditions:
• Junction temperature exceeds 150 °C
• Short-circuit of one of the outputs to ground or to V
P
• Load dump; VP>20V.
The voltage level at pin 14 will be at a constant level of
approximately1⁄2VP during fault condition. At a short-circuit
over the load, pin 14 will be at1⁄2VP for approximately
20 ms and VP for approximately 50 µs.
The device can be used as a normal BTL class-AB
amplifier if the electrolytic capacitors C1 and C2 are
omitted; see Fig.6. If the case temperature exceeds
120 °C, the device will switch back from class-H to class-B
operation. The high power supply voltage is then disabled
and the output power is limited to 10 W. By measuring the
voltage on the class-B/class-H pin, the actual crystal
temperature can be detected.
1996 May 145
Page 6
Philips SemiconductorsProduct specification
40 W car radio high power amplifierTDA1560Q
LIMITING VALUES
In accordance with the Absolute Maximum Rating System (IEC 134).
SYMBOLPARAMETERCONDITIONSMIN.MAX.UNIT
V
P
I
OSM
I
ORM
V
P(sc)
E
cap
I
17
P
tot
T
stg
T
amb
supply voltageoperating−18V
non-operating−30V
load dump protection; tr≥ 2.5 ms −45V
non-repetitive peak output current−6A
repetitive peak output current−4A
AC and DC short-circuit safe voltage−18V
energy handling capability at outputs VP=0−200mJ
current at pin 17V17<VP−1−5mA
total power dissipation−60W
storage temperature−55+150°C
operating ambient temperature−40−°C
THERMAL CHARACTERISTICS
SYMBOLPARAMETERVALUEUNIT
R
th j-a
R
th j-case
Heatsink design
There are two parameters that determine the size of the
heatsink. The first is the rating for the case temperature
and the second is the ambient temperature at which the
amplifier must still deliver its full power in the class-H
mode.
thermal resistance from junction to ambient in free air40K/W
thermal resistance from junction to case (measured in Fig.6)3K/W
XAMPLE 2
E
With disabled class-H mode, an 8 Ω load and driven with
a sine wave signal the maximum power dissipation is
approximately 5 W. At a virtual junction temperature of
150 °C and T
R
th case-h
= 1 K/W the thermal resistance of the heatsink
amb(max)
at 60 °C, R
th vj-case
= 3 K/W and
should be:
E
XAMPLE 1
With an 8 Ω load and driven with a music signal, the
maximum power dissipation is approximately 6.5 W. If the
amplifier is to deliver its full power at ambient temperatures
up to 50 °C the case temperature should not be higher
150 60–
---------------------5
In this example the size of the heatsink is determined by
the virtual junction temperature.
3 114 K/W=––
than120 °C for class-H operation.
R
th case-h
120 50–
----------------------
= 1 K/W, thus the external heatsink should be:
6.5
1.0–10 K/W=
In this example and with an 8 Ω load, the size of the
heatsink is determined by the rating for the maximum full
power ambient temperature. If the case temperature of the
device exceeds 120 °C then the device switches back to
class-B, see “Example 2”.
1996 May 146
Page 7
Philips SemiconductorsProduct specification
40 W car radio high power amplifierTDA1560Q
DC CHARACTERISTICS
V
= 14.4 V; RL=8Ω; T
P
SYMBOLPARAMETERCONDITIONSMIN.TYP.MAX.UNIT
Supply
V
P
I
q(tot)
V
O
∆V
V
14
O
supply voltagenote 18.014.418.0V
total quiescent current−100160mA
DC output voltagenote 2−6.5−V
DC output offset voltage−−150mV
diagnostic output voltagenote 36−8V
Mode select switch (see Fig.4)
V
16
I
SW max
I
sb
∆V
V
O
O
switch input voltage levelstandby condition0−1.2V
maximum switch current−−20µA
DC supply currentstandby condition−550µA
DC output offset voltagemute condition−−150mV
output signal voltage in mute conditionV
=25°C and using 4 K/W heatsink; measured in Fig.6; unless otherwise specified.
Class-B/class-H operation (see Fig.3 and note 5)
V
17
switch input voltage levelclass-B operation2.5−VP− 1V
class-H operation0−1.0V
I
SW
T
case
switch currentnote 6−−2mA
case temperature for switching to class-B−120−°C
Notes
1. The circuit is DC adjusted at V
= 8 to 18 V and AC operating at VP= 8.5 to 18 V.
P
2. The DC output voltage, or the common mode voltage on the loudspeaker terminals with respect to ground, is 6.3 V
at output power up to 8.5 W. At higher output power, the common mode voltage will be higher.
3. The voltage at pin 14 is approximately1⁄2VP in the event of a short-circuit, load dump or temperature protection. Any
circuit connected to pin 14 should have an input resistance of >2 MΩ and an input capacitance of <5 nF.
4. The DC output offset voltage step is the difference in output offset voltage in the mute condition and the on condition.
The absolute value of this voltage step is given as +∆V
o mute
−∆V
< 150 mV.
oon
5. Figure 3 shows the relationship between the global crystal temperature and the open voltage at the
class-B/class-H pin.
6. The maximum voltage on pin 17 is VP− 1 (VP≤ 18 V).
low frequency roll-off−3 dB; note 3−40−Hz
high frequency roll-off−1dB20−−kHz
voltage gain293031dB
SVRRsupply voltage ripple rejectionnote 4
CMRRcommon mode rejection rationote 564−−dB
V
i(max)
V
no
Z
input impedancenote 8180300−kΩ
I
maximum input voltage−1.2−V
noise output voltageon; RS=0Ω; note 6−100300µV
=25°C and using 4 K/W heatsink; measured in Fig.6;
amb
THD = 0.5%2730−W
THD = 10%;
3639−W
continuously driven
THD = 10%;
−40−W
with burst signals; note 1
class-B operation
THD = 10%710−W
=1W−0.05−%
o
=10W−0.1−%
P
o
= −1dB
o
−40 to 15000−Hz
with respect to 30 W; note 2
on4855−dB
mute4865−dB
standby80−−dB
on; R
=10kΩ; note 6−150−µV
S
mute; notes 6 and 7−100−µV
Notes
1. With a continuous sine wave input signal the output power is approximately 1 W less than driven with a bursted
signal; also depending on the equivalent series resistance of the electrolytic capacitors C1 and C2 (see Fig.6) and
the resistance of the connections between pins 5, 8, 10 and 13 and C1, C2.
2. The power bandwidth is limited by the value of the electrolytic capacitors C1 and C2.
3. Frequency response is externally fixed by the input coupling capacitor.
4. Ripple rejection measured at the output, across R
, with a source impedance of 0 Ω and a frequency between 100 Hz
L
and 10 kHz, and an amplitude of 2 V (p-p). The maximum supply voltage ripple is 2.5 V RMS.
5. The common mode rejection ratio is measured at the output, across RL, with a voltage source (500 mV RMS)
between both short-circuited inputs and signal ground (see Fig.5). Frequencies are between 100 Hz and 10 kHz.
6. Noise output voltage measured in a bandwidth of 20 Hz to 20 kHz.
7. Noise output voltage independent of source impedance.
8. Input impedance without external resistor (Rex).
1996 May 149
Page 10
Philips SemiconductorsProduct specification
40 W car radio high power amplifierTDA1560Q
+V
handbook, full pagewidth
input ( )
V
P
9
1
output 1 ( )
7
P
input ( )
2
TDA1560Q
3
6,12
Fig.5 Common mode rejection ratio measurements.
Table 1 Values of capacitors C1, C2 and Ck and frequency roll off
1. Plastic or metal protrusions of 0.25 mm maximum per side are not included.
OUTLINE
VERSION
SOT243-1
A2bpcD
17.0
4.6
4.2
0.75
0.60
15.5
0.48
0.38
IEC JEDEC EIAJ
1
e
(1)
deD
24.0
20.0
23.6
19.6
w M
b
p
(1)
E
h
12.2
102.54
11.8
REFERENCES
0510 mm
scale
1
1.27
e
5.08
L
3
L
E
2
h
6
Q
LL3m
3.4
12.4
3.1
11.0
m
2.4
1.6
c
e
2
Qj
2.1
4.3
1.8
EUROPEAN
PROJECTION
v M
v
0.8
x
0.4w0.03
ISSUE DATE
95-03-11
97-12-16
(1)
Z
2.00
1.45
1996 May 1414
Page 15
Philips SemiconductorsProduct specification
40 W car radio high power amplifierTDA1560Q
SOLDERING
Introduction
There is no soldering method that is ideal for all IC
packages. Wave soldering is often preferred when
through-hole and surface mounted components are mixed
on one printed-circuit board. However, wave soldering is
not always suitable for surface mounted ICs, or for
printed-circuits with high population densities. In these
situations reflow soldering is often used.
This text gives a very brief insight to a complex technology.
A more in-depth account of soldering ICs can be found in
our
“IC Package Databook”
Soldering by dipping or by wave
The maximum permissible temperature of the solder is
260 °C; solder at this temperature must not be in contact
with the joint for more than 5 seconds. The total contact
time of successive solder waves must not exceed
5 seconds.
DEFINITIONS
Data sheet status
Objective specificationThis data sheet contains target or goal specifications for product development.
Preliminary specificationThis data sheet contains preliminary data; supplementary data may be published later.
Product specificationThis data sheet contains final product specifications.
(order code 9398 652 90011).
The device may be mounted up to the seating plane, but
the temperature of the plastic body must not exceed the
specified maximum storage temperature (T
printed-circuit board has been pre-heated, forced cooling
may be necessary immediately after soldering to keep the
temperature within the permissible limit.
Repairing soldered joints
Apply a low voltage soldering iron (less than 24 V) to the
lead(s) of the package, below the seating plane or not
more than 2 mm above it. If the temperature of the
soldering iron bit is less than 300 °C it may remain in
contact for up to 10 seconds. If the bit temperature is
between 300 and 400 °C, contact may be up to 5 seconds.
stg max
). If the
Limiting values
Limiting values given are in accordance with the Absolute Maximum Rating System (IEC 134). Stress above one or
more of the limiting values may cause permanent damage to the device. These are stress ratings only and operation
of the device at these or at any other conditions above those given in the Characteristics sections of the specification
is not implied. Exposure to limiting values for extended periods may affect device reliability.
Application information
Where application information is given, it is advisory and does not form part of the specification.
LIFE SUPPORT APPLICATIONS
These products are not designed for use in life support appliances, devices, or systems where malfunction of these
products can reasonably be expected to result in personal injury. Philips customers using or selling these products for
use in such applications do so at their own risk and agree to fully indemnify Philips for any damages resulting from such
improper use or sale.
1996 May 1415
Page 16
Philips Semiconductors – a worldwide company
Argentina: see South America
Australia: 34 Waterloo Road, NORTH RYDE, NSW 2113,
All rights are reserved. Reproduction in whole or in part is prohibited without the
prior written consent of the copyright owner.
The information presented in this document does not form part of any quotation
or contract, is believed to be accurate and reliable and may be changed without
notice. No liability will be accepted by the publisher for any consequence of its
use. Publication thereof does not convey nor imply any license under patent- or
other industrial or intellectual property rights.
Printed in The Netherlands
517021/1200/04/pp16Date of release: 1996 May 14
Document order number:9397 750 00844
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