Showing posts with label diagram. Show all posts
Showing posts with label diagram. Show all posts

Friday, October 24, 2014

Ni Cd and Ni MH Adjustable constant current Circuit Diagram

This is a battery charger circuit with adjustable current for Ni-MH or Ni-Cd. It can be used for a constant current power, which can be set to any value from a few milliamps to about 500 mA. The maximum current is 500 mA, because that is the limit of transistor BC140. The input voltage must be above 5.25V output voltage, this is due to losses as 1.25V current limit and approximately 4V regulator.

 Battery Charger Ni-Cd and Ni-MH Adjustable constant current Circuit Diagram
 
 


The LM317 regulator is used, it should have a sink.

Components
R1 100Ω resistor
VR1 trimpot or potentiometer 500Ω
Capacitor C1 0.1μF
C2 Capacitor 0.01μF
Diode D1 1N4001
Q1 Transistor BC140
IC1 Voltage Regulator LM317
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8 Amp Regulated Power Supply circuit Diagram

This power supply is powered by a transformer operating from 120 Vac on the primary and providing proximately 20 Vac on the primary, and providing approximately 20 Vac on the secondary. Four 10-A diodes with a 100 PIV rating are used in a full-wave bridge rectifier.

 8-Amp Regulated Power Supply Circuit Diagram


8-Amp Regulated Power Supply circuit Diagram

A 10,000 ^F/36 Vdc capacitor completes the filtering, providing 28 Vdc. The dc voltage is fed to the collectors of the Darlington connected 2N3055s. Base drive for the pass transistors is from pin 10 of the µ723 through a 200 ohm current limiting resistor, Rl. The reference terminal (pin 6) is tied directly to the non-inverting input of the error amplifier (pin 5), providing 7.15 V for comparison. Link

The inverting input to the error amplifier (pin 4) is fed from the center arm of a 10 k ohm potentiometer connected across the output of the supply. This control is set for the desired output voltage of 13.8 V. Compensation of the error amplifier is accomplished with a 500 pF capacitor connected from pin 13 to pin 4. If the power supply should exceed 8 A or develop a short circuit, the µ723 regulator will bias the transistors to cutoff and the output voltage will drop to near zero until the short circuit condition is corrected.
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Discrete Virtual Ground Circuit Diagram

Here is the simple virtual ground circuit based on discrete components. This simple design comes from miniaturization guru Sijosae. Is to make a buffer from generic discrete components. The transistors can be most any complementary pair of small-signal transistors. Suitable alternatives are the PN2222A and PN2907A. The diodes are generic small-signal types. An acceptable alternative is the 1N914. This circuit has better performance than a simple resistive divider virtual ground, and the parts cost is lower than for any other circuit mentioned here. It is, however, the least accurate of the buffered virtual ground circuits.

 ircuit diagram:
 
 
 Parts:

R1,R2 = 4.7K
R3,R4 = 4.7R
C1,C2 = 470uF-25V
C3,C4 = 47uF-25V
D1,D2 = 1N4148
Q1 = 2SC1384
Q2 = 2SA684
B1 = Battery
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Simple Voltage to Frequency Converter Circuits Diagram

This Simple Voltage to Frequency Converter Circuits Diagram has a 1 Hz-to-30 MHz output, 150-dB dynamic range, for a 0 to 5 V input. It maintains 0.08% linearity over its entire 71/3 decade range with a full-scale drift of about 20 ppm/°C. To get the additional bandwidth, the fast )FET buffer drives the Schottky TTL Schmitt trigger. 

Simple Voltage to Frequency Converter Circuits Diagram

Simple Voltage to Frequency Converter Circuits Diagram

The Schottky diode prevents the Schmitt trigger from ever seeing negative voltage at its input. The Schmitt`s input voltage hysteresis provides the limits which the oscillator runs between. The 30-MHz, full-scale output is much faster than the LTC1043 can accept, so the digital divider stages are used to reduce the feedback frequency signal by a factor of 20. The remaining Schmitt sections furnish complementary outputs.
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Monday, October 20, 2014

Build a Period To Voltage Converter Circuit Diagram

this is the simple Period To Voltage Converter Circuit Diagram. The input signal drives ICD. Because ICD`s positive input (V+) is slightly offset to + 0.1 V, its steady state output will be around +13 V. This voltage is sent to ICC through D2, setting ICC`s output to +13 V. Therefore, point D is cut off by Dl, and CI is charged by the current source. 

Assuming the initial voltage on CI is zero, the maximum voltage (^Cinax) is given by: When the input goes from low to high, a narrow positive pulse is generated at point A. This pulse becomes -13 V at point B, which cuts off D2. ICC`s V+ voltage becomes zero. 

Period To Voltage Converter Circuit Diagram

Period To Voltage Converter Circuit Diagram

The charge on CI will be absorbed by ICC on in a short time. The time constant of C2 and R5 determines the discharge period— about 10 /is. ICB is a buffer whose gain is equal to (R& + R9)~Rg = lM5. ICD`s average voltage will be (1362f 1.545) + 2 = 1052/. RIO and C3 smooth the sawtooth waveform to a dc output.
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Photo Electric Street Light Circuit Diagram

This is basically a Schmitt Trigger circuit which receives input from a cadmium sulfide photo cell and controls a relay that can be used to switch off and on a street lamp at dawn and dusk. I have built the circuit with a 120 ohm/12 volt relay and monitored performance using a lamp dimmer, but did not connect the relay to an outside light.

The photo cell should be shielded from the lamp to prevent feedback and is usually mounted above the light on top of a reflector and pointed upward at the sky so the lamp light does not strike the photo cell and switch off the lamp.

Photo Electric Street Light Circuit Diagram

Lights Circuit Diagram
 
The photo cell is wired in series with a potentiometer so the voltage at the junction (and base of transistor) can be adjusted to about half the supply, at the desired ambient light level. The two PNP transistors are connected with a common emitter resistor for positive feedback so as one transistor turns on, the other will turn off, and visa versa. Under dark conditions, the photo cell resistance will be higher than the potentiometer producing a voltage at Q1 that is higher than the base voltage at Q2 which causes Q2 to conduct and activate the relay.

The switching points are about 8 volts and 4 volts using the resistor values shown but could be brought closer together by using a lower value for the 7.5K resistor. 3.3K would move the levels to about 3.5 and 5.5 for a range of 2 volts instead of 4 so the relay turns on and off closer to the same ambient light level. The potentiometer would need to be readjusted so that the voltage is around 4.5 at the desired ambient condition. Link
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Simple Solar Engine Circuit Diagram

 Simple Solar Engine Circuit Diagram
 
Simple Solar Engine Circuit Diagram Small DC motor runs off of calculator solar cell in dim light. How do we achive 10nA operation? By using diodes in place of pull up resistors, and by isolating the DC load from the trigger circuit via junction drops and the 10nF capacitor. If there is too much power comming from the solar cell then the motor might run too often or even continuously. You can avoid this by putting a 100K ohm resistor in series with the solar cell. 

 Simple Solar Engine Circuit Diagram

 Simple Solar Engine Circuit Diagram

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Friday, October 17, 2014

Build a Simple Audio Amplifier 2800W Circuit Diagram

How to Build a Simple Audio Amplifier 2800W Circuit Diagram. This is a Mono high power amplifier is actually a powerful 1400 W, but if this high power amplifier circuit is doubled and you want to create stereo, high power amplifier the necessary components and pcb requires two-fold. So if the stereo high power amplifier 2 X 1400W. Schematic Circuit diagram is still less by looking at the circuit that was so below, the finished circuit has been added with a gains using JRC4558 IC by the two and the picture ic where it can be seen below. 

For circuit buffers, drivers, and booster use multiple transistors and other components (can be seen listed component). And high power amplifier project that is so below is just part of the buffer and driver while the booster has not been made​​. For additional transistors in the booster or high power amplifier end scheme can be found Booster output power amplifier.

 Audio Amplifier 2800W Circuit Diagram


Part List :

Resistor
R1_____560Ω
R2_____100Ω
R3_____2K2Ω
R4_____560Ω
R5_____1Ω
R6_____27KΩ
R7_____10KΩ
R8_____100Ω
R9_____100Ω
R10____100Ω
R11____12KΩ
R12____100Ω
R13____100Ω
R14____100Ω
R15____27KΩ
R16____2K2Ω
R17____560Ω
R18____100Ω
R19____10KΩ
R20____330Ω
R21____47Ω 2W
R22____56Ω
R23____2K2Ω
R24____22Ω
R25____56Ω
R26____180Ω
R27____500-1KΩ Trim
R28____560Ω
R29____56Ω
R30____56Ω
R31____22Ω 1W
R32____5Ω6 2W
R33____10Ω
R34____180Ω
R35____100Ω
R36____22Ω 2W
R37____180Ω
R38____56Ω
R39____47Ω 2W
R40____5Ω6 2W
R41____10Ω
R42____10Ω
R43____10Ω
R45____10Ω
R46____0.22Ω 5W
R47____0.22Ω 5W
R48____0.22Ω 5W
R49____0.22Ω 5W
R50____10Ω 5W

Capacitor
C1_____1цF
C2_____1.5nF
C3_____0.1цF 250-275V
C4_____0.1цF 250-275VC5_____100nF
C6_____100цF 50V
C7_____39pF
C8_____330pF
C9_____330pF
C10____330pF
C11____47nF 250-275V
C12____220nF 250-275V

Transistor
T1_____MJE340
T2_____2N5551 / C2240
T3_____2N5551 / C2240
T4_____2N5551 / C2240
T5_____2N5551 / C2240
T6_____2N5401 / BF423
T7_____2N5401 / BF423
T8_____2N5401 / BF423
T9_____2N5401 / BF423
T10____MJE350
T11____B1186
T12____TIP127
T13____D1763
T14____D1763
T15____B1186
T16____C5198
T17____A1941
T18____2SC2922 / MJ15024G
T19____2SC2922 / MJ15024G
T20____2SA1216 / MJ15025G
T21____2SA1216 / MJ15025G


Sourced by SIGMA-4 Madiun ©
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Saturday, October 11, 2014

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:

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.

Author :M.K. Chandra ,Mouleeswaran And A.N. Vadivudai Naayaki
 
 
Source
: www . efymag . com
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Saturday, February 8, 2014

Solid State Relay Circuit Diagram

Solid State Relay Circuit
Solid state relay is a series that functions like a relay hibryd mechanics. Solid state relays is built with insulating an MOC for separate the input and the switch. With Solid state relays we can avoid the occurrence of sparks as it did in the relay can also avoid the occurrence of conventional connection is not perfect because porous contactor as in conventional relays.


The series of solid state relays This is quite simple and we can make in a PCB hole. For more details can be seen in the picture following a series of solid state relays.

Solid State Relay Circuit
Solid State Relay Circuit Diagram

Solid state relay has many advantages including no mechanical friction on the contactor, the connection process only occur when there are crosses zero, there is no spark at the contactor, not noisy, small konsusi flow control, better endurance.
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Friday, February 7, 2014

Wiring Diagram Protection For Telephone Line

A
long time ago when telephones were so simple almost nothing could go
amiss from an electrical point of view, Telecom operators installed
surge protection on all telephone lines exposed to storm risks.
Paradoxically, now that we are hooking up delicate and expensive
equipment such as telephones filled with electronics, fax machines,
(A)DSL modems, etc., this protection has disappeared.

However, if
you have the good fortune to live in the countryside in a building
served by overhead telephone lines, there’s an obvious risk of very high
voltages being induced on the lines during thunderstorms. While we
have lost count today of all of the modems, fax machines and other
telephones that have been destroyed by a ‘bolt of lightning’,
surprisingly you only have to invest a few pounds to get a remarkably
efficient protection device like the one we are proposing here.

During
a storm, often with lightning striking near a telephone line, the line
carries transient voltages up to several thousands of volts. Contrary
to the HV section of television sets or electrical fences, on which
practically no current is running, in the case of lighting striking
current surges of thousand of amps are not uncommon. To protect oneself
from such destructive pulses, traditional components are not powerful
or fast enough.

As you can see on our drawing, a (gas-filled)
spark gap should be used. Such a component contains three electrodes,
insulated from each other, in an airtight cylinder filled with rare gas.
As long as the voltage present between the electrodes is below a
certain threshold, the spark gap remains perfectly passive and presents
an impedance of several hundreds of MW. On the other hand, when the
voltage rises above this threshold, the gas is very rapidly ionized and
the spark-gap suddenly becomes a full conductor to the point of being
able to absorb colossal currents without being destroyed.


telephone line protector circuit schematic

The
one we are using here, whose size is of the same magnitude as an
ordinary one watt resistor, can absorb a standardized 5,000 amps pulse
lasting 8/20 ms! Since we are utilizing a three-electrode spark gap, the
voltage between the two wires of the line or between any wire and
ground, cannot exceed the sparking voltage, which is about 250 volts
here. Such protection could theoretically suffice but we preferred to
add a second security device made with a VDR (GeMOV or SiOV depending on
the manufacturer), which also limits the voltage between line wires to
a maximum of 250 volts.

Even if this value seems high to you,
we should remember that all of the authorized telephone equipment,
carrying the CE mark must be able to withstand it without damage. This
is not always the case however with some low-end devices made in China,
but that’s an entirely different problem. Since pulses generated by
lightning are very brief, the ground connection of our assembly must be
as low-inductance as possible.

It must therefore be short, and
composed of heavy-duty wire (1.5 mm2 c.s.a. is the minimum). If not, the
coil, composed of the ground connection, blocks the high frequency
signal that constitutes the pulse and reduces the assembly’s
effectiveness to nothing. Finally, please note that this device
obviously has no effect on the low frequency signals of telephones and
fax machines and it does not disturb (A)DSL signals either.
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Wednesday, February 5, 2014

On/Off Infrared Remote Control

Most
homes today have at least a few infrared remote controls, whether they
be for the television, the video recorder, the stereo, etc. Despite
that fact, who among us has not cursed the light that remained lit
after we just sat down in a comfortable chair to watch a good film? This
project proposes to solve that problem thanks to its original
approach. In fact, it is for a common on/off switch for infrared remote
controls, but what differentiates it from the commercial products is
the fact that it is capable of working with any remote control.

Therefore,
the first one you find allows you to turn off the light and enjoy your
movie in the best possible conditions. The infrared receiver part of
our project is entrusted to an integrated receiver (Sony SBX 1620-52)
which has the advantage of costing less than the components required to
make the same function. After being inverted by T1, the pulses
delivered by this receiver trigger IC2a, which is nothing other than a D
flip-flop configured in monostable mode by feeding back its output Q
on its reset input via R4 and C3. The pulse that is produced on the
output Q of IC.2A makes IC.2B change state, which has the effect of
turning on or turning off the LED contained in IC3.


On-off Infrared Remote Control circuit schematic

This
circuit is an opto triac with zero-crossing detection which allows our
setup to accomplish switching without noise. It actually triggers the
triac T2 in the anode where the load to be controlled is found. The
selected model allows us to switch up to 3 amperes but nothing should
stop you from using a more powerful triac if this model turns out to be
insufficient for your use. In order to reduce its size and total cost,
the circuit is powered directly from the mains using capacitor C5 which
must be a class X or X2 model rated at 230 volts AC.

This type
of capacitor, called ‘self-healing’, is the only type we should use
today for power supplies that are connected to ground. ‘Traditional’
capacitors, rated at 400 volts, do not really have sufficient safety
guarantees in this area. Considering the fact that the setup is
connected directly to the mains, it must be mounted in a completely
insulated housing. A power outlet model works very well and can easily
be used to inter-space between the grounded wall outlet and that of the
remote control device.

Based on this principle, this setup
reacts to any infrared signal and, as we said before, this makes it
compatible with any remote control. On the other hand, it has a small
disadvantage which is that sometimes it might react to the ‘normal’
utilization of one of these, which could be undesirable. To avoid that,
we advise you to mask the infrared receiver window as much as possible
so that it is necessary to point the remote control in its direction
in order to activate it.
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