Showing posts with label a. Show all posts
Showing posts with label a. Show all posts

Monday, December 23, 2013

Build a Remotely Adjustable Solid State High voltage Supply Circuit Diagram

How to build a remotely adjustable solid state high-voltage supply Circuit Diagram. The output voltage changes approximately linearly up to 20 KV as the input voltage is varied from 0 to 5 V. The oscillator is tuned by a 5-0 potentiometer to peak the output voltage at the frequency of maximum transformer response between 45 and 55 kHz. 

The feedback voltage is applied through a 100-KO resistor, an op amp, and a comparator to a high-voltage amplifier. A diode and varistors on the primary side of the transformer protect the output transistor. The transformer is a flyback-type used in color-television sets. A feedback loop balances between the high-voltage output and the low-voltage input.


Remotely Adjustable Solid State High-voltage Supply Circuit Diagram





Remotely Adjustable Solid State High-voltage Supply Circuit Diagram
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Wednesday, May 29, 2013

How to Build a Simplest Modified Sine Wave Power Inverter Circuit


If you are looking for a simple modified sine wave power inverter circuit design to build, then perhaps you have hit the bull’s eye here. The present article very explicitly deals with a circuit idea of the same that’s astonishingly simple and low cost with an output that’s to a very extent is comparable with its sine wave counterparts.

Here we discuss a circuit design of a modified sine wave power inverter unit that’s probably the simplest and the cheapest to build. Whole circuit description and circuit schematic is included here in, read on.....


Circuit Design Discussion
In one of my recent articles I discussed a circuit design of a modified sine wave power inverter and we came to know how it’s different and more efficient than a few other designs available in some other websites. In this article we go through yet another design of a modified sine wave inverter which may not be as efficient as the previous one but is definitely better than a square wave design and is also perhaps the simplest one to build.
Folks who are new to electronics may get a bit confused regarding the difference between a square wave and a modified square wave inverter. It may be understood through the following brief explanation:
As we all know an inverter will always generate an alternating current (AC) similar to our domestic AC line voltage so that it can replace it during power failures. An AC in simple words is basically a rise and fall of voltage of a particular magnitude.
This rise and fall of voltage happens at a particular rate i.e. at a particular number of times per second, known as its frequency. So for example a 50 Hz AC means 50 cycles or 50 ups and downs of a particular voltage in one second.
In a sine wave AC as found in our normal domestic mains outlet the above rise and fall of voltage is in the form of a sinusoidal curve, i.e. its pattern gradually varies with time and thus is not sudden or abrupt. Such smooth transitions in the AC waveform becomes very suitable and a recommended type of supply for the many common electronic gadgets like TVs , music systems , Refrigerators, motors etc.
However, in a square wave pattern the voltage ups and downs are instant and sudden. Such immediate rise and fall of potential creates sharp spikes at the edges of each wave and thus becomes very undesirable and unsuitable for sophisticated electronic equipments. Therefore it is always dangerous to operate them through a Square weave inverter supply.
In a modified square wave design, the waveform shape basically remains the same but the size of each section of the wave-form is appropriately dimensioned so that its average value matches closely to an AC waveform’s average value.
For the present design we yet again take the help of the evergreen versatile IC 4017.
We know that when a clock input is applied to its pin #14, the IC produces a shifting cycle logic high pulses through its 10 output pins.
Looking at the circuit diagram we find that the pin outs of the IC are terminated to supply the base of the output transistors such that they conduct after every alternate output pulse from the IC.
This happens simply because the bases of the transistors are connected alternately to the IC pin outs and the intermediate pin-out connections are just eliminated or kept open.
The transformer windings which are connected to the transistor’s collector respond to the alternate transistor switching and produce a stepped up AC at its output having a waveform exactly as shown in the diagram.
The output of this Modified sine wave power inverter is although not quite comparable to the output of a pure sine wave inverter but definitely will be far better than that of an ordinary square wave inverter. Moreover the idea is very easy and cheap to build.

 



QUIZ = Can anybody tell the reason behind powering IC2 via T0 and the associated circuit instead of providing a direct supply to its pin 16?


Parts List

R1=20K
R2,R3=1K
R4,R5=220 Ohms, 1 watt
C1=0.095Uf
C2,C3,C4=10UF/25V
T0 = BC557B
T1,T2=TIP122
T3,T4=BDY29
IC1= SN74LVC1G132 or a single gate from IC4093
IC2=4017
IC3=7805
TRANSFORMER=12-0-12V/10AMP/230V

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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
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Wednesday, April 10, 2013

A D Conversion Circuit for Single Ended MSB First Mode


This is a design circuit for analog to digital converter that can be used in data acquisition. This circuit is based on ADC0833 and controlled by INS8048. Before explaining the system configuration, it is worthwhile for one to understand the operation of the INS8048 processors I/O ports. Ports 1 and 2 are quasi-bidirectional; that is, they can be used as inputs or outputs while being statically latched. If a ``1 is written into any port bit, that bit can function as an input or as a high level output. If a ``0 is written into any port bit, that bit can function only as a low level output.



Outputs are latched until changed and inputs are unlatched and must be read immediately. When used with the ANL Pp, A (AND accumulator to port) or the ORL Pp, A (OR accumulator to port) instructions, these ports provide an efficient means of handling single line inputs and outputs. Port expansion, if anticipated, is handled via the lower four bits of Port 2. Only four pins of the processors Port 1 or Port 2 are needed for physical interfacing. The ANL or ORL instructions set up the port pins to produce the proper outputs (CS, CLK, and the multiplex address) or to allow for data input from the A/D converter.



[Circuit schematic source: National Semiconductor Notes].

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Tuesday, April 9, 2013

Build a Radio Wave Alarm

This simple circuit is sure to have the police beating a path to your door- however, it has the added advantage of alerting you to their presence even before their footsteps fall on the doormat.

Simple Radio Wave Alarm Circuit Diagram :
Build a Radio Wave Alarm

Notes :
  • The circuit transmits on Medium Wave (this is the small problem with the police). IC1a, together with a sensor (try a 20cm x 20cm sheet of tin foil) oscillates at just over 1MHz. This is modulated by an audio frequency (a continuous beep) produced by IC1b. When a hand or a foot approaches the sensor, the frequency of the transmitter (IC1a) drops appreciably.
  • Suppose now that the circuit transmits at 1MHz. Suppose also that your radio is tuned to a frequency just below this. The 1MHz transmission will therefore not be heard by the radio. But bring a hand or a foot near to the sensor, and the transmitters frequency will drop, and a beep will be heard from the radio.
  • Attach the antenna to a multiplug adapter that is plugged into the mains, and you will find that the Medium Wave transmission radiates from every wire in your house. Now place a suitably tuned Medium Wave radio near some wires or a plug point in your house, and an early-warning system is set up.
  • Instead of using the sheet of tin foil as the sensor, you could use a doorknob, or burglar bars. Or you could use a pushbutton and series resistor (wired in series with the 33K resistor - the pushbutton would short it out) to decrease the frequency of IC1a, so activating the system by means of a pushbutton switch. In this case, the radio would be tuned to a frequency just below that of the transmitter.
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Sunday, April 7, 2013

A Simple Fog Lamp Sensor

For several years now, a rear fog lamp has been mandatory for trailers and caravans in order to improve visibility under foggy conditions. When this fog lamp is switched on, the fog lamp of the pulling vehicle must be switched of to avoid irritating reflections. For this purpose, a mechanical switch is now built into the 13-way female connector in order to switch of the fog lamp of the pulling vehicle and switch on the fog lamp of the trailer or caravan. For anyone who uses a 7-way connector, this switching can also be implemented electronically with the aid of the circuit illustrated here.

Fog Lamp Sensor Circuit Diagram

Fog Lamp Sensor Circuit Daigram

Here a type P521 optocoupler detects whether the fog lamp of the caravan or trailer is connected. If the fog lamp is switched on in the car, a current flows through the caravan fog lamp via diodes D1 and D2. This causes the LED in the optocoupler to light up, with the result that the photo-transistor conducts and energies the relay via transistor T1. The relay switches of the fog lamp of the car. For anyone who’s not all thumbs, this small circuit can easily be built on a small piece of perforated circuit board and then fitted somewhere close to the rear lamp fitting of the pulling vehicle.

Source: http://www.ecircuitslab.com/2011/06/simple-fog-lamp-sensor.html
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Friday, April 5, 2013

How to Build a Solar Panel Voltage Regulator Charger Circuit Charger Circuit at Home

How to Build a Solar Panel Voltage Regulator, Charger Circuit, Charger Circuit at Home


We all know pretty well about solar panels and their functions. The basic functions of these amazing devices is to convert solar energy or sun light into electricity.
Basically a solar panel is made up discrete sections of individual photo voltaic cells. Each of these cells are able to generate a tiny magnitude of electrical power, normally around 1.5 to 3 volts.  

Many of these cells over the panel are wired in series so that the total effective voltage generated by the entire unit mounts up to an usable 12 volts or 24 volts outputs.
The current generated by the unit is directly proportional to the level of the sun light incident over the surface of the panel.
The power generated from a solar panel is normally used for charging a lead acid battery. The lead acid battery when fully charged is used with an inverter for acquiring the required AC mains voltage for powering the house electrical.
Ideally the sun rays should be incident over the surface of the panel for it to function optimally. However since the sun is never still, the panel needs to track or follow the suns path constantly so that it generates electricity at an efficient rate.
 If you are interested to build an automatic dual tracker solar panel system you may refer one of my earlier articles. Without a solar tracker, the solar panel will be able to do the conversions only at around 30 % efficiency.
Coming back to our actual discussions about solar panels, this device may be considered the heart of the system as far converting solar energy into electricity is concerned, however the electricity generated requires a lot of dimensioning to be done before it can be used effectively in the preceding grid tie system.
The voltage acquired from a solar panel is never stable and varies drastically according to the position of the sun and intensity of the sun rays and of course on the degree of incidence over the solar panel.
This voltage if fed to the battery for charging can cause harm and unnecessary heating of the battery and the associated electronics; therefore can be dangerous to the whole system.
In order to regulate the voltage from the solar panel normally a voltage regulator circuit is used in between the solar panel output and the battery input. This circuit makes sure that the voltage from the solar panel never exceeds the safe value required by the battery for charging.
Normally to get optimum results from the solar panel, the minimum voltage output from the panel should be higher than the required battery charging voltage, meaning even during adverse conditions when the sun rays are not sharp or optimum, the solar panel still should be able to generate a voltage more than say 12 volts which may be the battery voltage under charge.
Solar Voltage regulators available in the market can be too costly and not so reliable; however making one such regulator at home using ordinary electronic components can be not only fun but also very economical.
Referring to the figure we see a circuit design that utilizes very ordinary components and yet fulfills the needs just as required by our specs.
 A single IC LM 338 becomes the heart of the entire configuration and becomes responsibly for implementing the desired voltage regulations single handedly.
The shown solar panel regulator, charger circuit is framed as per the standard mode of the IC 338 configuration.
The input is given to the shown input points of the IC and the output for the battery received at the output of the IC. The pot or the preset is used to accurately set the voltage level that may be considered as the safe value for the battery.
The circuit also offers a current control feature, which makes sure that the battery always receives a fixed predetermined charging current rate and is never over driven.
The module can be wired as directed in the diagram. The relevant positions indicated can be simply wired even by a layman. Rest of the function is taken care of by the regulator circuit.
The switch S1 should be toggled to inverter mode once the battery gets fully charged (as indicated over the meter).
The charging current may be selected by appropriately selecting the value of the resistors R3. It can be done by solving the formula:
0.6/R3 = 1/10 battery AH
The preset VR1 is adjusted for getting the required charging voltage from the regulator.
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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.
For technical explanation of the circuit you may refer to the data provided here.
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