Showing posts with label low. Show all posts
Showing posts with label low. Show all posts
Tuesday, October 8, 2013
Low Battery Indicator I
Here is the circuit diagram of low battery indicator from silicon chip electronics. This simple circuit lights LED1 when the battery voltage drops below the setting set by trimpot VR1. In effect, VR1 and associated resistors bias Q1 on which holds Q2 and the LED off. When the voltage drops below the set value, Q1 turns off, allowing Q2 to turn on and light the LED. The circuit is suitable for nominal battery voltages up to 12V.
Continue Reading[...]
Monday, May 13, 2013
A Low Cost Hearing Aid
This low-cost, general-purpose electronic hearing aid works off 3V DC (2x1.5V battery). The circuit can be easily assembled on a veroboard. For easy assembling and maintenance, use an 8-pin DIP IC socket for TDA2822M.
In this circuit, transistor Q1 and associated components form the audio signal preamplifier for the acoustic signals picked up by the condenser microphone and converted into corresponding electrical signals. Resistor R5 and capacitor C3 decouple the power supply of the preamplifier stage. Resistor R1 biases the internal circuit of the low-voltage condenser microphone for proper working. The audio output from the preamplifier stage is fed to the input of the medium-power amplifier circuit via capacitor C2 and volume control P1.
The medium-power amplifier section is wired around popular audio amplifier IC TDA2822M (not TDA2822). This IC, specially designed for portable low-power applications, is readily available in 8-pin mini DIP package. Here the IC is wired in bridge configuration to drive the 32-ohm general-purpose monophonic earphone. Red LED (D1) indicates the power status. Resistor R8 limits the operating current of D1. The audio output of this circuit is 10 to 15mW and the quiescent current drain is below 1 mA.
Parts:
P1 = 10K
R1 = 2.2K
R2 = 330K
R3 = 680R
R4 = 33R
R5 = 100R
R6 = 4.7R
R7 = 4.7R
R8 = 220R
C1 = 0.01uF-10V
C2 = 100nF-63V
C3 = 47uF-10V
C4 = 10uF-10V
C5 = 0.01uF-10V
C6 = 100uF-10V
C7 = 100nF-63V
C8 = 100nF-63V
D1 = Red LED
Q1 = BC547
IC1 = TDA2822M
EP1 = Mono Earphone 32R
SW1 = On-Off Switch
Continue Reading[...]
In this circuit, transistor Q1 and associated components form the audio signal preamplifier for the acoustic signals picked up by the condenser microphone and converted into corresponding electrical signals. Resistor R5 and capacitor C3 decouple the power supply of the preamplifier stage. Resistor R1 biases the internal circuit of the low-voltage condenser microphone for proper working. The audio output from the preamplifier stage is fed to the input of the medium-power amplifier circuit via capacitor C2 and volume control P1.
The medium-power amplifier section is wired around popular audio amplifier IC TDA2822M (not TDA2822). This IC, specially designed for portable low-power applications, is readily available in 8-pin mini DIP package. Here the IC is wired in bridge configuration to drive the 32-ohm general-purpose monophonic earphone. Red LED (D1) indicates the power status. Resistor R8 limits the operating current of D1. The audio output of this circuit is 10 to 15mW and the quiescent current drain is below 1 mA.
Parts:
P1 = 10K
R1 = 2.2K
R2 = 330K
R3 = 680R
R4 = 33R
R5 = 100R
R6 = 4.7R
R7 = 4.7R
R8 = 220R
C1 = 0.01uF-10V
C2 = 100nF-63V
C3 = 47uF-10V
C4 = 10uF-10V
C5 = 0.01uF-10V
C6 = 100uF-10V
C7 = 100nF-63V
C8 = 100nF-63V
D1 = Red LED
Q1 = BC547
IC1 = TDA2822M
EP1 = Mono Earphone 32R
SW1 = On-Off Switch
Sunday, April 7, 2013
Low Power Voltage Doubler Circuit Diagram
All
miniature electronic devices operate off batteries. Some of them need
higher than the standard battery voltages to operate efficiently. If
the battery of that specific voltage is unavailable, we are forced to
connect additional cells in series to step up the DC voltage. Thus, the
true meaning of miniaturisation is lost. A simple way to overcome this
problem is to employ a voltage doubler, if the device under
consideration can operate at a small current.
Here we present a
low-power voltage doubler circuit that can be readily used with devices
that demand higher voltage than that of a standard battery but low
operating current to work with. The circuit is quite simple as it uses
only a few components. Yet, the output efficiency is 75 to 85 percent
along its operating voltage range. The available battery voltage is
almost doubled at the output of the circuit.
Here IC1 is wired as
an astable multivibrator to generate rectangular pulses at around 10
kHz. This frequency and duty cycle of the pulses can be varied using
preset VR1. The pulses are applied to switching transistors T1 and T2
for driving the output section, which is configured as a
voltage-doubling circuit. The doubled voltage is available across
capacitor C5. During each cycle of the pulse occurance, the high level
drives T1 into its saturation, keeping transistor T2 cut off.
Circuit diagram:

So
transistor T1 charges capacitor C4 via the path formed by diodes D2
and D1 to a voltage level slightly lesser than the supply. But during
the low period of the pulse, transistor T1 is cut off while transistor
T2 is driven into saturation. Now, transistor T2 raises the charge on
the negative pole of capacitor C4 by another step equal to the supply
voltage. Therefore an equal amount of charging is built up on capacitor
C5 via diode D3.
This doubling action increases the total
voltage across capacitor C5 to almost double the input voltage. If the
output of the pulse generator is maintained with a high enough
amplitude and frequency, the output voltage and current remain constant
and cater to the needs of the load. Even with the half-wave function,
this circuit is almost free of ripple voltage. If the connected load
doesn’t require a high current, the efficiency can be expected in the
upper 90 percentranges.
Since the input voltage is doubled, the
current drain from the input power supply is also doubled at the input
but halved at the output. One point of caution is that if the
multivibrator’s frequency is fairly high, the output may suffer with the
interference imposed over the DC voltage. In this case, the frequency
must be set favorably by trials and actual load connection procedure.
This tiny circuit can be assembled on the general-purpose PCB. If all of
the components are surface-mount type, the whole module can be
genuinely miniaturized.
EFY Lab note.
During testing with input of 8V and 1.25mA load current the output voltage was found to be around 13V.
Source: EFY Mag
miniature electronic devices operate off batteries. Some of them need
higher than the standard battery voltages to operate efficiently. If
the battery of that specific voltage is unavailable, we are forced to
connect additional cells in series to step up the DC voltage. Thus, the
true meaning of miniaturisation is lost. A simple way to overcome this
problem is to employ a voltage doubler, if the device under
consideration can operate at a small current.
Here we present a
low-power voltage doubler circuit that can be readily used with devices
that demand higher voltage than that of a standard battery but low
operating current to work with. The circuit is quite simple as it uses
only a few components. Yet, the output efficiency is 75 to 85 percent
along its operating voltage range. The available battery voltage is
almost doubled at the output of the circuit.
Here IC1 is wired as
an astable multivibrator to generate rectangular pulses at around 10
kHz. This frequency and duty cycle of the pulses can be varied using
preset VR1. The pulses are applied to switching transistors T1 and T2
for driving the output section, which is configured as a
voltage-doubling circuit. The doubled voltage is available across
capacitor C5. During each cycle of the pulse occurance, the high level
drives T1 into its saturation, keeping transistor T2 cut off.
Circuit diagram:

Low-Power Voltage Doubler Circuit Diagram
So
transistor T1 charges capacitor C4 via the path formed by diodes D2
and D1 to a voltage level slightly lesser than the supply. But during
the low period of the pulse, transistor T1 is cut off while transistor
T2 is driven into saturation. Now, transistor T2 raises the charge on
the negative pole of capacitor C4 by another step equal to the supply
voltage. Therefore an equal amount of charging is built up on capacitor
C5 via diode D3.
This doubling action increases the total
voltage across capacitor C5 to almost double the input voltage. If the
output of the pulse generator is maintained with a high enough
amplitude and frequency, the output voltage and current remain constant
and cater to the needs of the load. Even with the half-wave function,
this circuit is almost free of ripple voltage. If the connected load
doesn’t require a high current, the efficiency can be expected in the
upper 90 percentranges.
Since the input voltage is doubled, the
current drain from the input power supply is also doubled at the input
but halved at the output. One point of caution is that if the
multivibrator’s frequency is fairly high, the output may suffer with the
interference imposed over the DC voltage. In this case, the frequency
must be set favorably by trials and actual load connection procedure.
This tiny circuit can be assembled on the general-purpose PCB. If all of
the components are surface-mount type, the whole module can be
genuinely miniaturized.
EFY Lab note.
During testing with input of 8V and 1.25mA load current the output voltage was found to be around 13V.
Source: EFY Mag
Sunday, March 31, 2013
How to Make a Simple Active Low Pass Filter Circuit Using IC 741
In electronics, filter circuits are basically employed for restricting the passage of a certain frequency range while allowing some other band of frequency into the further stages of the circuit.
Primarily there are three types of frequency filters that are used for the above mentioned operations.
These are: Low pass filter, high pass filter and the band pass filter.
As the name suggests, a low pass filter circuit will allow all frequencies below a certain set frequency range.
A high pass filter circuit will allow only the frequencies which are higher than the preferred set range of frequency while a band pass filter will allow only an intermediate band of frequencies to flow to the next stage, inhibiting all frequencies which may be outside this set range of oscillations.
Filters are generally made with two types of configurations, the active type and the passive type.
Passive type filter are less efficient and involve complicated inductor and capacitor networks, making the unit bulky and undesirable. However these will not require any power requirement for itself to operate, a benefit too small to be considered really useful.
Contrary to this active type of filters are very efficient, can be optimized to the point and are less complicated in terms of component count and calculations.
In this article we are discussing a very simple circuit of a low pass filter, which was requested by one of our avid readers Mr.Bourgeoisie.
Looking at the circuit diagram we can see a very easy configuration consisting of a single opamp as the main active component.
The resistors and the capacitors are discretely dimensioned for a 50 Hz cut OFF, meaning no frequency above 50 Hz will be allowed to pass through the circuit into the output.

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