|
Description  |
|
|
BACKGROUND OF THE INVENTION
1. Field of the Invention
This invention relates to an overload detecting circuit for an amplifier
and, particularly to an overload detecting circuit which is preferably
used for a PWM amplifier to produce an amplified output by means of pulse
width modulation in response to an input signal.
2. Description of the Prior Art
A transistor output amplifier being of class-D type is converted into a
pulse-width-modulated signal (PWM signal), a switching element being
controlled in ON-OFF state in response to the PWM signal, and the
switching output being demodulated through a filter to derive an amplified
output signal.
When, for example, a speaker unit having a lower input impedance than a
rating of the amplifier is connected as a load, or the output terminals of
the amplifier are shorted, the amplifier runs into an overload condition.
The current flowing through the switching element exceeds rated value of
the amplifier, so that the switching device is in danger of being broken
down.
Therefore, the amplifier needs an overload detecting circuit for protecting
the switching element. A such conventional overload detecting circuit
operates in the manner that the current flowing through the switching
element is detected, and when the detecting current exceeds a rated value,
the input signal is attenuated or the PWM signal to the switching element
is cut off. The detecting circuit detects the current flowing through the
switching element. The detecting current is larger than the rated maximum
permissible current of the switching element. Thus, when such a trouble
that the output terminals are shorted occurs, a current larger than the
rated maximum permissible current flows through the switching element. The
current causes a large quantity of loss such as generation of heat, until
an overload protecting means operates.
Further, the filter to which the output of the switching element is
supplied to demodulate the PWM signal, consists of an inductor and a
capacitor. The switching current induces a counter electromotive force,
which causes a reverse current. The reverse current flows through a
discharge diode. Thus, in the amplifier using such an overload detecting
circuit, the reverse current flowing through the diode becomes larger in
accordance with the maximum output current of the amplifier under the
overload condition thereof, which results in generation of a large
quantity of power loss in the diode.
SUMMARY OF THE INVENTION
Accordingly, it is an object of this invention to provide an overload
detecting circuit for a PWM amplifier in which the aforenoted
disadvantages in the prior art are removed.
It is another object of this invention to provide an overload detecting
circuit for a PWM amplifier in which the current flowing through the
switching circuit is depressed upon detecting the overload condition to
decrease the generation of heat in the switching element.
It is still another object of this invention to provide an overload
detecting circuit for a PWM amplifier in which clipping of the waveform of
the output signal due to the phase difference between the PWM output
voltage and output current does not occur.
In accordance with one aspect of the present invention, an overload
detecting circuit for a PWM amplifier is provided, which includes a DC
voltage source having a pair of terminals; first and second switching
elements connected in series between the terminals of the DC voltage
source; a signal input circuit for ON/OFF controlling the first and second
switching elements, alternatively, in response to an input pulse signal; a
low pass filter connected between the connection point of the first and
second switching elements and an output terminal adapted to be connected
with a load; a first detecting circuit for detecting an output current
flowing through the first switching element; a second detecting circuit
for detecting an output voltage produced at the output terminal; a first
rectifying circuit connected to the second detecting circuit and having a
discharge time constant circuit determined by the cut-off frequency of the
low pass filter; and a first comparing circuit for comparing the outputs
of the first detecting circuit and of the first rectifying circuit and for
producing an overload indicative signal in response to the comparison
result therebetween.
The other objects, features and advantages of the present invention will be
apparent from the following description taken in conjunction with the
attached drawings.
BRIEF DESCRIPTION OF THE DRAWINGS
FIG. 1 is a circuit diagram showing a preferred embodiment of this
invention; and
FIG. 2 is a graph for explanation of operation of this invention.
DESCRIPTION OF THE PREFERRED EMBODIMENTS
An overload detecting circuit according to one embodiment of this invention
includes a pulse width modulated signal amplifier 1, shown in FIG. 1,
consisting of a pulse width modulator 2, a pulse drive circuit 3, a PNP
transistor 4 and an NPN transistor 5 for switching for operation, and a
low-pass filter 6, an overload detecting circuit 7 and a field effect
transistor (FET) 8 for attenuation of an input signal.
A DC voltage +Vcc is supplied to the emitter of the transistor 4 from a
power supply terminal 9 through a resistor 10, and a DC voltage -Vcc is
supplied to the emitter of the transistor 5 from another power supply
terminal 11 through a resistor 12. The filter 6 consists of inductors and
capacitors. A reverse voltage of the inductors, induced by the switching
operation of the transistors 4 and 5 is absorbed by diodes 13 and 14. The
input signal is supplied through an input terminal 15, and an output
signal is led out through an output terminal 16 to which a loud speaker 17
is connected as a load of the amplifier.
The overload detecting circuit 7 is constituted as follows.
The emitter of a PNP transistor 18 is connected to the power supply
terminal 9 and the collector thereof is connected to the gate of the FET
8. The base of the transistor 18 is connected to one end of the resistor
10 through a resistor 19 and is connected to one end of a resistor 20
whose other end is connected to the other end of the resistor 10. Further,
the base of the transistor 18 is connected to the other power supply
terminal 11 through a series connection circuit of resistors 21 and 22.
The emitter of an NPN transistor 23 is connected to the terminal 11 and the
collector thereof is connected to the base of the transistor 18 through a
resistor 24. The base of the transistor 23 is connected to one end of a
resistor 12 through a resistor 25 and is connected to one end of a
resistor 26 whose other end is connected to another end of the resistor
12. The base of the transistor 23 is connected to the power supply
terminal 9 through a series connection circuit of resistors 27 and 28.
When the resistances of the resistors 10 and 12 are represented by R.sub.1,
resistors 20 and 26 by R.sub.2, resistors 19 and 25 by R.sub.3 and
resistors 21, 22 and 27, 28 by R.sub.4, these resistances are set in
relation expressed by R.sub.1 <<R.sub.2 and R.sub.3 <<R.sub.4. These
resistances may have the following values: R.sub.1 =0.1.about.1.OMEGA.,
4.sub.2 =1 k.OMEGA., R.sub.3 =510.OMEGA., and R.sub.4 =68 k.OMEGA..
A part of the output signal from the filter 6 is detected through diodes 29
and 30. The signal in positive polarity is supplied to the connecting
point a of the series connection of the resistors 21 and 22. The signal in
negative polarity is supplied to the connecting point b of the series
connection of the resistors 27 and 28. Capacitors 31 and 32 connected
respectively between the point a and ground, and point b and ground,
operate to eliminate high frequency component in the detected signal for
preventing detecting circuit 7 from operating in the high frequency region
of the output signal for the reason described below.
The operation of the overload detecting circuit will be described.
In normal operation of the amplifier 1, the input signal supplied from a
pre-amplifier through the input terminal 15 is converted to a PWM signal
at the pulse width modulator 2. The PWM signal is supplied to the
transistors 4 and 5 through the pulse drive circuit 3. These transistors 4
and 5 turn on and off alternately. As a result, an amplified PWM signal of
500 kHz, for example, having peak levels near the supply voltages .+-.Vcc
is obtained at the connecting point of the collectors of the transistors 4
and 5. The PWM signal is supplied to the low-pass filter 6 to be
demodulated into an audio signal. An amplified output signal having peak
levels near the supply voltages .+-.Vcc is obtained from the filter 6. The
output signal is supplied to the loud speaker 17.
A part of the output signal is supplied to the connecting points a and b
respectively through the diodes 29 and 30. On the other hand, to the point
a, the power supply voltage +Vcc is supplied, through the circuit
consisting of the resistors 10, 19 and 20 and through the resistor 21, and
the power supply voltage -Vcc is supplied through the resistor 22. The
resistors 21 and 22 have the same resistance R.sub.4 as each other, and
the resistances R.sub.1, R.sub.2 and R.sub.3 of the resistors 10, 19 and
20 are respectively much less than resistance R.sub.4 (R.sub.1, R.sub.2
and R.sub.3 <<R.sub.4). In the absence of the output signal, the voltage
of the point a is nearly zero. When the output voltage of positive
polarity is supplied to the point a through the diode 29, the voltage of
the point a changes within the range of nearly 0 to +Vcc in proportion to
the positive output voltage.
To the point b, similarly, the power supply +Vcc is supplied through the
resistor 28 and the other supply voltage -Vcc is supplied through the
circuit consisting of the resistors 12, 25 and 26 and through the resistor
27. The resistors 27 and 28 have the same resistance R.sub.4 as each
other, and the resistances R.sub.1, R.sub.2 and R.sub.3 of the resistors
12, 25 and 26 are respectively much less than the resistance R.sub.4
(R.sub.1, R.sub.2 and R.sub.3 <<R.sub.4). Accordingly, when the output
voltage of negative polarity is supplied to the point b through the diode
30, the voltage of the point b changes within the range of nearly 0 to
-Vcc in proportion to the negative output voltage.
Currents I.sub.1 and I.sub.2 respectively flow through the resistors 21 and
27 in accordance with the variation of voltage at the points a and b. The
currents I.sub.1 and I.sub.2 are nearly zero when the voltage of the
output signal is .+-.Vcc, and they reach almost maximum value Vcc/R.sub.4,
when the voltage of the output signal is zero, because of the fact:
R.sub.1, R.sub.2 and R.sub.3 <<R.sub.4. Thus, the currents I.sub.1 and
I.sub.2 vary from the maximum Vcc/R.sub.4 to zero in accordance with the
output voltage. On the other hand, the transistors 4 and 5 connected
between the power supply terminals 9 and 11 alternately become conductive
to produce a switching current I.sub.0 which flows alternately through the
resistors 10 and 12. The current I.sub.0 varies almost from zero to a
maximum output current Vcc/R.sub.1 in proportion to the output signal, in
contrast with the variation of the currents I.sub.1 and I.sub.2 varying
almost from the maximum to zero.
When a loudspeaker 17 having a lower input impedance than a rating of the
amplifier is connected or the loudspeaker 17 is shorted, the current
I.sub.0 increases and the amplifier 1 runs into an overload condition.
Under that condition, the voltage at the output terminal 16 falls nearly
to zero. Therefore, the voltages at the points a and b fall nearly to
zero, too, which makes the currents I.sub.1 and I.sub.2 flow at their
maximum values.
The voltage across the resistor 19, i.e., the base voltage V.sub.B, is the
sum of a voltage (IoR.sub.1 .times.[R.sub.3 /R.sub.2 +R.sub.3 ]) yielded
by the current I.sub.0 and a voltage (I.sub.1 .times.[R.sub.2 R.sub.3
/R.sub.2 +R.sub.3 ]); because the circuit consisting of the resistors 10,
19 and 20 is regarded as a parallel connection of the resistors R.sub.2
and R.sub.3. Thus, the voltage V.sub.B is expressed as follows:
V.sub.B =(I.sub.1 .times.[R.sub.2 R.sub.3 /R.sub.2 +R.sub.3 ])+(I.sub.0
R.sub.1 .times.[R.sub.3 /R.sub.2 +R.sub.3 ]) (1)
In the overload condition of the amplifier, the currents I.sub.1 and
I.sub.0 in the expression (1) increase to cause a condition: V.sub.B
.gtoreq.V.sub.BE, in which V.sub.BE represents a voltage across the base
and emitter of the transistor 18, that is, for instance, about 0.6 V. As a
result, the transistor 18 turns on.
In the same way, the current I.sub.0 of the transistor 5 and the current
I.sub.2 yield a voltage V.sub.B across the resistor 25 in accordance with
a similar expression to (1). The voltage V.sub.B in the overload condition
makes the transistor 23 conductive, which causes a current to flow through
the resistor 24. As a result, the current I.sub.1 increases to turn on the
transistor 18. The turning sequence of the transistor 18, due to the
current I.sub.1 and due to the turning-on of the transistor 23, is
determined by the timing of switching action of the transistors 4 and 5.
Thus, in the overload condition, the transistor 18 turns on to generate a
signal, which is supplied to the gate of the FET 8. The FET 8 turns on to
attenuate the level of the input signal, which causes the transistors 4
and 5 to stop the switching operation. The amplifier 1 turns into a
condition similar to the condition that the input signal is not supplied
thereto.
Accordingly, the transistors 4 and 5 are kept away from the overload
condition.
According to this invention, as shown in FIG. 2, the output current is
limited to .+-.I.sub.0 (s) in the overload condition such as short circuit
of the output terminal of the amplifier. A protective line is formed on
the basis of the current .+-.I.sub.0 (s) and rated maximum currents
.+-.I.sub.0 (max) at maximum output voltage .+-.E.sub.0 in normal
operation of the amplifier. The amplifier operates inside the protective
line, and is protected from overload outside the protective line. Thus,
the rated maximum current I.sub.0 (max) flows in the amplifier with the
conventional overload detecting circuit in the overload condition. On the
other hand, the current can be decreased to I.sub.0 (s) in accordance with
this invention. The heat generation of the switching element can be
decreased.
In the operation of normal load, the amplifier can normally operate when
the phase of the PWM signal at the collectors of the transistors 4 and 5
matches with the phase of the output signal, i.e., the phase of the
voltages at the points a and b. Since the filter 6, however, consists of
inductors and capacitors, a certain phase difference is produced between
the PWM output current and the output voltage. As the phase difference is
small in lower frequency region of the output signal, the amplifier
operates normally in the lower frequency region. The phase difference
increases in higher frequency region. As a result, when the voltage of the
point a falls nearly to zero to bring the current I.sub.1 to a maximum,
then the transistor 4 turns on, a little current I.sub.1 flows through the
transistor 4. The PWM signal at the collector is clipped, so that the
level of the output signal is clipped.
In this embodiment, capacitors 31 and 32 having a small capacitance are
respectively connected to the diodes 29 and 30, in order to prevent the
output signal from clipping in the higher frequency region. The capacitors
31 and 32 are charged in the higher frequency region, so that the voltages
at the points a and b increase to the charging voltages of the capacitors
31 and 32. Accordingly, the increase of the currents I.sub.1 and I.sub.2
is suppressed, and the current I.sub.0 flows sufficiently. Thus, as the
sensitivity of the overload detecting circuit 7 is lowered in the higher
frequency region, a clip of the output level caused by the filter 6 which
produces phase difference between the PWM signal and the output signal, is
prevented.
The capacitance of the capacitors 31 and 32 and the resistances of the
resistors 22 and 28 are so determined that the voltages at the points a
and b rise to a predetermined value when the frequency of the output
signal reaches a predetermined frequency which is lower than the cut-off
frequency of the filter 6. The time constant Td may be selected as
follows:
Td=R.sub.4 .multidot.C.sub.31 >(1/f.alpha.)
in which f.sub.60 stands for the cut-off frequency of the filter 6, R.sub.4
for the resistance of the resistor 22 and C.sub.31 for the capacitance of
the capacitor 31.
While there has been described preferred embodiments of the invention,
obviously further modifications and variations are possible in the light
of the above teachings. It is understood, therefore, that within the scope
of the appended claims, the invention may be practiced otherwise than as
specifically described.
* * * * *
|
|
|
|
|
Description  |
|