Showing posts with label to. Show all posts
Showing posts with label to. Show all posts
Friday, April 26, 2013
Easy to Use FM Radio Receiver
The project is a user-friendly and cheap FM radio receiver which produces the desired audio signals using integrated circuit to achieve the pre-processing units. During operation, the user is allowed to change stations and interact with the receiver by integrating a keypad and an LCD for communication. There are several functions that this radio receiver can perform including adjusting the threshold when picking up stronger or weaker stations, setting up 3 favorite stations for quick tuning, scanning up/down for next strong signal station, and tuning up/down a frequency.
A keypad is designed for controlling the receiver and the buttons are mapped to their corresponding functionality while the other buttons are not connected. The 4 main sub-components of the receiver include the LCD, the keypad, the favorite station storage, and the communication with receiver. Each of them is being controlled by their software components. The antenna transfers the incoming radio signal to the AR1010 FM radio receiver. To communicate with the AR1010, the I2C protocol is used since the sample code is available online. Also, the AR1010 is powered by 3V. The button presses on the keypad are scanned by the program.
Saturday, March 30, 2013
Variable 5 to 20V DC Supply Rise
If you are looking for a low drop voltage regulator that can provide a power supply of 1A with an output voltage of between 5V and 20V DC, National Semiconductor LM2941 Low Dropout Adjustable Regulator is that you can pick to make use of. Its a typical dropout voltage of 0.5V which means that the input supply need only must be 0.5V DC over the desired output voltage. Its other features include internal short circuit current limit and reverse battery protection.
As shown in the schematic below, the regulator has five pins which consists of the ON/OFF control, Input Voltage, Output Voltage, Ground & Adjustable pins. ON/OFF is used for the purpose of switching on & off of the regulator. The capacitors C1 & E1 are to be placed as close as feasible to the regulator.
The output of the circuit can be varied by varying the worth of potentiometer VR1 from 5V DC to 20V DC. The input voltage is limited from five.5V DC to 30V DC. Resistor R1 must be greater than 1K. The worth of the VR1 that needs to be set is calculated from the formula given below:
If R1=1K, Vout = 5V, VR1 should be set to 2.9K ohm.
If R1=1K, Vout = 20V, VR1 should be set to 14.7K ohm
Wednesday, March 27, 2013
How to Make Your Own Active Loudspeakers Speaker Amplifier
With the advent of ultra modern cell phones, now it has become possible to store huge music data and listen to them with just a flick of your finger. But listening to music becomes significantly pleasing only if it’s hugely amplified and reproduced over active loudspeakers or with systems incorporating a speaker amplifier circuit.
By amplifying a small music signal from either a cell phone or similar source and hearing it over active loudspeakers can become more interesting and the outcome simply amazing. Complete design idea and schematic of a simple speaker amplifier is produced here.
A normal loudspeaker may be a 3-way type with the connected amplifier equipped with the usual bass treble controls etc. No matter how good they may be in their performance, they can never beat the sound quality that is normally achieved through active loudspeakers. Whether it’s by quality or power they are the best sound reproducing gadgets.
Building an active loudspeaker system may look complex but can be very amusing, and once built can indeed become a treat hearing its magnificent response. Although the cost involved compared to its passive counterpart is much higher, an active system has definitely a clear edge over the passive systems.
The various advantages of a built in speaker amplifier over the passive design may be listed as follows:
No external amplifiers required and so no cumbersome wiring involved.
No use of passive filter circuits using resistors and inductors means an increase in the overall efficiency of the output response due to the absence of power losses through heat dissipations generally involved with passive filter resistors.
Unlike passive filters, the active filters help to boost the set responses. With passive filters it’s just the opposite, they tend to make the input music response deteriorate to a great extent.
Here we will discuss one such active loudspeaker circuit, capable of transforming even an ordinary music inputs into outstanding reproductions. Let’s read its circuit details.
Circuit Description
The following points will discuss one such speaker amplifier circuit, capable of transforming even an ordinary music inputs into outstanding reproductions.
The idea is very simple, equalize the inputs by passing them through appropriate lo-pass and hi-pass filters at the input stages, then amplify this dimensioned content to suitable high volumes using ordinary amplifier.
We do exactly as mentioned above; referring to the figure we find that a single IC TL072 which is basically a dual op-amp in a single package is discretely configured into two separate filters.
IC 2A is wired as a standard high pass filter. As the name suggests, the circuit will pass only specified degree of high input frequencies. The cut off frequency may lie around 3 kHz and can be varied by adjusting VR1 and VR2 or any one of them.
IC 2B is wired in just the opposite configuration i.e. as a low pass filter and allows only the specified degree of frequencies iver the lower ranges, the cut off frequency being 2.5 kHz. It will stop all frequencies above this. The response is adjustable using VR3.
The above suitably equalized audio now is simply fed to an audio amplifier for the required amplifications over the connected loudspeakers. The channel responsible for producing higher frequencies uses a twitter for better optimization where as the other section which handles the lower frequencies is integrated to a woofer for the relevantly bass output optimization.
Best yet cheap CAR AMPLIFIER you can buy.
Best yet cheap CAR AMPLIFIER you can buy.
Monday, March 25, 2013
3V DC to 5V DC REGULATED POWER SUPPLY ELECTRONIC DIAGRAM

3V DC to 5V DC REGULATED POWER SUPPLY ELECTRONIC DIAGRAM
A 5V DC regulated output from 2 cells 3V DC batteries. The output current of the circuit is limited to 50mA. However, it still able to supply many microcontroller circuits. 3009 and 560R Resistor provide the 5V DC output, make up a voltage divider network.
Thursday, March 21, 2013
Introduction to Amplifier Rise
Amplification is the method of increasing the amplitude of a AC signal current or voltage such as audio signal for sound or video signal for a television picture. The amplifier allows a small input signal to control a bigger amount of power in the output circuit. The output signal is a replica of the original input signal but has higher amplitude.
Amplification is necessary as in most applications, the signal is weak to be used directly. For example, an audio output of 1mV from a microphone is unable to drive a loud speaker which requires a few volts to operate. Hence, the signal require to be amplified to a few volts before it can be fed in to the loud speaker.
NP N Transistor Circuit Configurations
An example of different type of transistor configurations in the circuit is as shown in Figure one below.
(1) The common emitter(CE) circuit makes use of emitter as its common electrode. The input signal is applied to the base and the amplified output is taken from the collector. This is the usually use because its the best combination of current gain & voltage gain.
(2) The common base (CB) circuit makes use of base as its common electrode. The input signal is applied to the emitter & the amplified output is taken from the collector. The comparatively high emitter current compared to the base current ends in low input impedance value. For this reason, the CB circuit is never used.
(3) The common collector (CC) circuit makes use of collector as its common electrode. The input signal is applied to the base & the amplified output is taken from the emitter. This circuit is also called an emitter follower. This name means that the output signal voltage at the emitter follows the input signal at the base with the same phase but less amplitude. The voltage gain is less than one & is usually used for impedance matching. Its high input at the base as a load for the earlier circuit & low output impedance at the emitter as a signal source for the next circuit.
Classes
They can be classified in to classes A, B, C & AB. They are defined based on the percent of the cycle of input signal that can produce output current.
In Class A, the output current flows for the full cycle of 360 degree of input signal. The distortion is the lowest with around 5% to 10% &an efficiency of 20% to 40%. In general, most tiny signal operate class A
In Class C, the output current flows for less than half of the input cycle. Typical operation is 120 degree of input current in the coursework of the positive half cycle of the input current. This class has an efficiency of 80% but has the highest distortion. This class is usually used for RF amplification with a tuned circuit in the output.
In Class B, the output current flows for half of the input cycle which is around 180 degree. Class B operation lies between class A & class C. Classes B are usually connected in pairs & in such a circuit called push-pull amplifier. The push pull is often used for audio power output to a loud speaker.
In Class AB, it offers a compromise between the low distortion of class A & the higher power of class B. It is usually used for push pull audio power amplifiers.
Sunday, March 17, 2013
how to repair Nokia n73 Mic problem
Here is tips for Nokia N73 Mic problem :
1. Check headset connector first for dust and water damage, replace if needed.
2. Check mic, replace mic if needed.
3. If still problem replace Avilma.
4. If still problem check mic circuit for broken circuit.

More...
1. Check headset connector first for dust and water damage, replace if needed.
2. Check mic, replace mic if needed.
3. If still problem replace Avilma.
4. If still problem check mic circuit for broken circuit.

Thursday, March 14, 2013
How to repair nokia 6500 keypad problem
Here is tips for nokia 6500 keypad failure :
More...
1. Clean keypad doomshit first, replace doomshit if needed.
2. If not solved, check flexible cable, replace flexible cable if needed.
3. If still not solved, please trace and check keypad circuit.
How to Make an LED AC Voltage Indicator Project Do it Yourself
A simple construction and accurate result are the main features of this tiny circuit. Learn how to make ac voltage indicator from led in a most simple and easy to understand method.

The AC mains line that we get in our household electric socket outlets, may at times be full of dangerous fluctuations. These may either be in the form of a sudden high voltage or a low voltage. Both the situations can be very “fatal” to our sophisticated electronic equipments like TVs, DVD players, refrigerators, computers etc to name a few.
A simple electronic part such as an LED can play an important role in displaying the condition of this AC mains voltage and warn us of a possible electrical hazard.
Yeah, we will exactly learn how to make ac voltage indicator from led through a construction of a little electronic circuit.

Parts Required
You will need the following mentioned parts for the project:
TRANSISTORS T1, 2, 3, 4, 5 = BC547
ZENER DIODE Z1----Z5 = 3 VOLTS / 400mW
RESISTORS R 1—R10 = 1 K ¼ WATT, CFR.
CAPACITOR C1 = 1000uF/25v,
DIODE D1 = 1N4007
LED 1, 2, 3, 4, 5 = RED 5mm DIFFUSED
PRESET P1, 2, 3, 4, 5 = 47K LINEAR
GENERAL PURPOSE BOARD = 6” BY 2”
TRANSFORMER = O – 6 VOLTS/ 500mA
How to Construct the LED AC Voltage Indicator
It is completed through the following few easy steps:
In the procured general purpose board, with the help of the circuit schematic start inserting the transistors first in a straight line and solder their leads.
Similarly insert and solder the resistors, zener diodes, LEDs, capacitors, presets etc. in an organized manner and solder them with reference to the circuit diagram.
How to Test the Circuit?
The following testing details will furthermore help you to understand exactly how to make ac voltage indicator from led:
For testing the completed circuit board you will require a transformer with multiple voltage outputs.
Connect the transformer to the AC mains; also connect the common secondary output of the transformer to the negative point of the circuit.
Make an alligator clip/ wire assembly. Solder the wire end of the clip to 1N4007 diode input.
Now bite the clip to the 3 volt output of the transformer, adjust P1 so that the first LED just starts glowing.
As above go on connecting the clip to 6, 7.5, 9 and 12 volts of the transformer and adjust the presets P2, P3, P4 andP5 so that the relevant LEDs just start to glow at the respective voltages.
This completes the testing and the setting of the circuit.
Finally join the 6 volt transformer to the circuit and switch ON the power. You will find that LED 1, 2 and 3 are glowing brightly, LED no.4 is glowing with less brightness while the last LED is completely OFF, indicating a safe level of AC mains voltage.
Now in case the voltage exceeds a high level (above 260 volts) the last LED will start glowing brightly indicating a dangerous situation.
If the voltage drops to a dangerous level (below 160 V) LED 3 and may be LED 2 may cease to glow, again indicating a bad low voltage.
Wednesday, March 13, 2013
How to Understand Technical Specs of Solar Panels
Solar panels are devices which are used for generating electricity from sun light. Solar panels consist of many individual photo voltaic cells arranged in series. Each cell is able to generate a small amount of voltage in response to the incident sun rays over its surface. Arrays of these individual cells are connected in series to form a single solar panel, which results in the generation of a significant magnitude of voltage in the presence of sunlight.
This amazing ability of these devices to convert free and abundant solar energy into electrical power has made it immensely useful in the relevant application.

This amazing ability of these devices to convert free and abundant solar energy into electrical power has made it immensely useful in the relevant application.
No doubt, solar panels are gaining popularity at a very rapid pace and can be considered as the devices of the future for replacing conventional methods of generating electricity.
When it comes to personal usage, solar panels can become a difficult parameter to digest. While selecting solar panels, folks tend to depend entirely on the manufacturer and the technical personnel, and therefore are unable to take personal decisions with the devices technical specs and quality.
In this article we’ll discuss some of the basic technical points related to solar panels which will help us to understand solar panels from the core and use them efficiently. The discussed points are though very basic, provides general yet useful inputs regarding these outstanding devices.
As discussed in the above paragraph, solar panels convert direct sunlight incident over their surface into electricity. Since the generated electricity is directly proportional to the striking sunrays, the direction and the intensity of the rays become the main factors affecting the outcomes.
Therefore, the voltage magnitude available across solar panel output terminals may vary according to the intensity and the amount of sun light available over its surface, and varies linearly.
Typically every solar panel is associated with a particular set of technical and electrical specifications, which defines its functioning and application.
The following technical specs can be normally witnessed:
Optimal voltage,
Optimal current,
Maximum voltage,
Short circuit current,
Maximum wattage,
Fuse rating.
As a customer, the parameters which would be particularly important are: optimal voltage, optimal current, short circuit current and the fuse rating.
Though the installations will be handled by the associated engineer, the user should also be aware regarding the operating terms related to these devices. This would greatly help them to analyze, customize and even troubleshoot some of the common faults accompanied with these devices.
Image Credit - http://cndingwen.en.made-in-china.com/offer/QMsmDPNUHgYy/Sell-285W-Polycrystalline-Solar-Panels.html
Coming back to the specs, optimal voltage refers to the magnitude of voltage that may be acquired from a solar panel under normal conditions; optimal current is also the magnitude of current that’s available from it under the above conditions, that is when the sun light is perpendicular to the surface of the panel with clear skies.
Optimal voltage should always be greater than the minimum required voltage for the application. In fact it should greater than twice the required value. This makes sure that even under gloomy conditions the output from the panel might be just enough for the needs or above the minimum requirements.
During optimal conditions, the excess voltage from the panel is appropriately tailored by the associated voltage regulator such that only the required magnitude reaches the application; normally this voltage will be used for charging an inverter battery.
Maximum voltage can be ignored as it refers to the ability of the panel to produce electricity under maximum artificial forced light conditions, not something related to normal usage.
Short circuit current is the magnitude of current which causes the output of the solar panel reach a zero level when its output leads are joined or shorted, a point at which the panel output indicates a zero voltage and fails to operate.
The condition may cause severe deterioration or even a permanent damage to the device. This specification indicates the loading current of the panel which cannot be exceeded above the rated value; typically this value must be kept at around 50% of the specified value.
The maximum fuse rating is the amperage of the fuse wire connected in series with the panels output. This rating should be a shade lower to the above short circuit current rating so that the fuse instantly blows-of before the current can exceed and reach the dangerous short circuit conditions.
The maximum wattage spec may also be ignored because once the optimal current and voltage are selected appropriately, the wattage which the product of the above two parameters, automatically adjust with the requirements.
The maximum wattage spec may also be ignored because once the optimal current and voltage are selected appropriately, the wattage which the product of the above two parameters, automatically adjust with the requirements.
However today’s modern solar voltage regulators and charger associated with solar panels take care of the most critical situations, eliminating short circuit, overload or over voltage situations, safeguarding both the solar panel and the inverter/battery stage which are integrated to the panel for the desired operations.
Although the solar panel may be generating just about enough current for your batteries, it may be quite useless once the sun rays stop reaching the surface of the panel.
To fight against this issue, solar trackersmechanisms are normally employed with solar panels so that the panels keep generating electrical power at the most efficient rates throughout the day irrespective of the sun’s position in the sky.
This also facilitates the incorporation of relatively smaller sized solar panels because now the optimal voltage can be selected just close to the actual requirement and does not need to be twice or thrice than the actual need.
Tuesday, March 12, 2013
How to Make a Non Contact AC Mains Phase Detector – Measure AC Field Strength Wirelessly
The circuit discussed in this article is of a non-contact mains AC field detector which displays the presence of a mains AC field from a distance of more an 6 inches. The circuit can be used for locating faults in house wiring without the need of making physical contact with the inner conductor of the wire and becomes useful in locating the breaks in a wire by pin pointing the area where the AC mains may be blocked due to a breakage.

The circuit is basically high gain non inverting amplifier which is configured using a few opamps and a few other inexpensive passive electronic components.
Just a couple of opamps have been incorporated here from the IC 324 for the required operations.

Looking at the figure we notice the following things:
The non-inverting input of the IC is grounded making the sensitivity of the configuration to the maximum.
Similarly a feed back loop created by connecting the output of the opamps to the inverting input helps to increase the gain of the set up many folds.
The input is applied to the inverting input 2 of the IC through a blocking capacitor.
The signals entering via the antenna is quickly picked up by the opamp inverting input and sent to the preceding circuit for the required processing and amplification.
It may be interesting to note that the sensitivity of the design can be simply varied by changing the value of the feedback resistor R1, for maximum sensiticity this resistor can be omitted.
However this can make the circuit a bit unstable and might provide false results.
The next stage includes another identical amplifier which is just the repetition of the previous input stage. This stage has been included in order to make the response of the circuit instant and so that the circuit is able to pick even the slightest of RF or the AC field within a certain range.
In case the circuit is intended to be used for detecting mains phase only at touching proximities, the sensitivity may be reduced to the required levels or the second stage may be excluded from the design.
The LED connected at the output is used for displaying the presence of the AC field; an illuminated LED identifies the presence of the field while no light from it provides the opposite conclusion.
By connecting a 1V FSD moving coil meter at the output, the device can be used to detect and measure the average strength of the AC mains present in that particular vicinity.


Parts List
R1 = 2M2,
R2 = 100K,
R3 = 1K,
C1 = 0.01uF
A1, A2 = IC 324
Monday, March 11, 2013
How to Build a Simple Room Temperature Monitor Circuit
A very simple yet highly precise air temperature sensor gauge circuit has been presented here. The use of the highly versatile and accurate IC LM 308 makes the circuit respond and react superbly to the smallest temperature changes happening over its surrounding atmosphere. Diode 1N4148 is used as an active ambient temperature sensor here.
The electronic air temperature sensor gauge circuit presented here is very accurate in its function, categorically due to its minimum level of hysteresis. Complete circuit description and construction clues included herein.
Circuit Description
The present circuit of an electronic air temperature sensor gauge circuit is outstandingly accurate and can be very effectively used to monitor the atmospheric temperature variations. Let’s briefly study its circuit functioning:
Here as usual we use the very versatile “garden diode” 1N4148 as the sensor due to its typical drawback (or rather an advantage for the present case) of changing its conduction characteristic in the influence of a varying ambient temperature. The diode 1N4148 is comfortably able to produce a linear and an exponential voltage drop across itself in response to a corresponding increase in the ambient temperature. This voltage drop is around 2mV for every degree rise in temperature. This particular feature of 1N4148 is extensively exploited in many low range temperature sensor circuits.
Referring to the figure we see that, IC1 is wired as an inverting amplifier and forms the heart of the circuit.
Its non inverting pin # 3 is held at a particular fixed reference voltage with the help of Z1, R4, P1 and R6.
Transistor T1 and T2 are used as a constant current source and helps in maintaining higher accuracy of the circuit.
The inverting input of the IC is connected to the sensor and monitors even the slightest change in the voltage variation across the sensor diode D1. These voltage variations as explained, is directly proportional to the changes in the ambient temperature.
The sensed temperature variation is instantly amplified into a corresponding voltage level by the IC and is received at its output pin #6.
The relevant readings are directly translated into degree Celsius through a 0-1V FSD moving coil type meter.
Parts List
R1, R4 = 12K,
R2 = 100E,
R3 = 1M,
R5 = 91K,
R6 = 510K,
P1 = 10K PRESET,
P2 = 100K PRESET,
C1 = 33pF,
C2, C3 = 0.0033uF,
T1, T2 = BC 557,
Z1= 4.7 V, 400mW,
D1 = 1N4148,
IC1 = LM308,
General Purpose Board as per size.
B1 and B2 = 9V PP3 battery.
M1 = 0 – 1 V, FSD moving coil type voltmeter
Setting Up the Circuit
The procedure is a bit critical and requires special attention. To complete the procedure you will need two accurately known temperature sources (hot and cold) and an accurate mercury-in-glass thermometer.
The calibration may be completed through the following points:
Initially keep the presets set at their midways. Connect a voltmeter (1 V FSD) at the output of the circuit.
For the cold temperature source, water at about room temperature is used here.
Dip the sensor and the glass thermometer into the water and record the temperature in the glass thermometer and the equivalent voltage outcome in the voltmeter.
Take a bowl of oil, heat it to about 100 degrees Celsius and wait until its temperature stabilizes down to about 80 degrees Celsius.
As above, immerse the two sensors and compare them with the above result. The voltage reading should be equal to the temperature change in the glass thermometer times 10 mill volt. Didn’t get it? Well, let’s read the following example.
Suppose, the cold temperature source water is at 25 degrees Celsius (room temperature), the hot source, as we know is at 80 degrees Celsius. Thus, the difference or the temperature change between them is equal to 55 degrees Celsius. Therefore the difference in the voltage readings should be 55 multiplied by 10 = 550 mill volts, or 0.55 volts.
If you don’t quite get the criterion satisfied, adjust P2 and continue to repeat the steps, until finally you achieve it.
Once the above rate of change (10 mV per 1 degree Celsius) is set, just adjust P1 so that the meter shows 0.25 volts at 25 degrees (sensor held in water at room temperature).
This concludes the setting of the circuit.
This air temperature sensor gauge circuit can also be effectively used as an electronic room thermometer unit.
Sunday, March 10, 2013
How to Build a Simple PWM Controlled DC to DC Cell Phone Charger Circuit – Science Fair Project
The explained circuit can be easily made at home by any school kid and used for displaying in his science fair exhibition. The circuit is a simple cell phone charger that may be operated in conjunction with any DC source, from a car or a motorcycle battery or from any ordinary 12 V AC DC adapter.
Nowadays we find most of the vehicles have their in built cell phone battery charger units which surely becomes very handy for travelers who mostly remain outdoors travelling in their vehicle.
The proposed cell phone charger circuit is as good as the conventional chargers which come fitted inside the cars and bikes.
Moreover the circuit can be simply integrated to ones own vehicle if the feature is not originally available in the vehicle.
Alternatively one may think of manufacturing the present unit and selling them in the market as an automobile cell phone charger and earn some hard bucks.
Circuit Description
Cell phones as we all know are highly sophisticated gadgets by nature and when it comes to charging cell phones the parameters no doubt also needs to be of very high standards.
The AC/DC cell phone chargers which come with the cell phones are all SMPS based and are extremely good with their outputs and that’s why the cell phone gets so efficiently charged by them.
However if we try to make our own version, it may fail altogether and the cell phones may just not respond to the current and display a “not charging” on the screen.
Cell phone battery cannot just be charged by supplying DC 4 volts, unless the current is optimally dimensioned the charging won’t initiate.
Using voltage regulator IC for making a DC to DC charger, which I myself have discussed in one of my earlier article is a good approach, but the IC tends to become too hot while charging the cell phone battery and therefore requires adequate heatsinking for remaining cool and operative.
This makes the unit a bit bulkier and moreover some significant amount of power is wasted in the form of heat, so the design cannot be considered very efficient.
The present PWM controlled DC to DC cell phone charger circuit is outstanding in its respect because, the involvement of PWM pulses helps to keep the output very suitable to the cell phone circuitry and also the concept involves no heating of the output device, making the entire circuit truly efficient.

Looking at the circuit we find that again the work horse IC 555 comes to our rescue and performs the important function of generating the required PWM pulses.
The input to the circuit is supplied through some standard DC source, ideally from an automobile battery.
The voltage powers the IC which instantly starts generating the PWM pulses and feeds it to the components connected at its output pin #3.
At the output the power transistor is used for switching the DC voltage at its collector directly to the cell phone.
However only the average DC voltage is finally fed to the cell phone due to the presence of the 100uF capacitor, which effectively filters the pulsating current and provides a stable, standard 4 volts to the cell phone.
After the circuit is built, the two pots will need to be optimized perfectly so that a well dimensioned voltage is produced at the output which may be ideally suited for charging the cell phone.
Parts List
R1, R2, R3 = 1K,
P1, P2 = 47K,
C2 = 1n,
C3, C1 = 100uF/25V
IC1 = 555
D1, D2, D3 = 1N4007
T1 = TIP127
T1 = TIP127
How to Make a Ghost Detector Circuit
Do you believe in the existence of ghosts? Well some of you may answer positively while some may just nod their heads showing sheer skepticism regarding the issue. Whatever may be the reactions; nobody just can’t deny or ignore the responses delivered from the circuit explained in this article. Here we are discussing a super simple yet super sensitive paranormal activity sniffer circuit, which can be effectively and possibly used for detecting ghosts or similar supernatural existence within a range of 10 meters. Many of these circuits may be built and posted at definite intervals for securing a certain premise having a large area. The circuit incorporates an alarm at the output which sounds immediately on detecting a paranormal intrusion. The circuit is ideally suited for areas that are prone to ghosts or likely of getting infested with similar para-natural sneakers.
WARNING 1 – THE DEVICE HAS BEEN TESTED WITH POSITIVE RESULTS AND IS PROVED TO BE EXTREMELY ACCURATE WITH THE DISCUSSED DETECTIONS. FOLKS WITH WEAK HEARTS OR TENDER PERSONALITY ARE ADVISED NOT TO GO ABOUT WITH THIS DEVICE, BECAUSE THE DEVICE NOT ONLY DETECTS BUT ALSO COINCIDENTALLY HAS THE ABILITY OF ATTRACTING THE PARABEINGS.
WARNING 2 – THE DEVICE CAN BE TESTED IN MORGUES, GRAVEYARDS, cemeteries etc. ZOMBIES ARE THE ONES WHICH ARE INSTANTLY DETECTED BY THIS DEVICE EVEN FROM DISTANCES MORE THAN 50 METERS. NO DOUBT CREATURE LIKE ZOMBIES WILL HATE THIS DEVICE….BEWARE.
Concept
It has been found through experiments by many researchers that paranormal occupancy is strongly accompanied by RF disturbances ranging from a few Hertz to many Kilohertz.
These signals may be directly proportional to the hostile nature of the ghost. Zombies are found to be emitting the strongest signals and are therefore considered the most horrible among the lot.
The circuit of a ghost detector discussed here is typically configured for capturing the above RF emissions from these creatures and transforming them into more human understandable electronic indications.
Circuit Description
A single versatile IC 324 is involved in the whole operation.
The IC is a quad opamp IC, meaning four opamps in one package.

Referring to the figure, the opamps can be seen configured as hi gain non inverting amplifiers.
All the opamps are configured as high gain signal amplifiers.
Tiny electromagnetic or RF disturbances which are typically found being generated during the presence of ghosts or paranormal activities are instantly picked up by the antenna of the circuit and are fed to the input of the first opamp stage at pin #9.
The signals get instantly amplified and are transferred to the subsequent stages for further amplification and enhancement.
The output of the last opamp is connected to an opto-coupler.
The optocoupler is a homemade type, incorporating an LED and an LDR fixed such that their emitting and detecting surfaces are placed face to face inside a light proof enclosure.
Here, the optocoupler is used for sensing the LED illumination that may occur when a certain paranormal activity is sensed.
The illumination produced over the LED is tracked by the LDR whose resistance falls with the LED light.
The fall in the resistance of the LDR activates the connected transistor at the output, which in turn actuates a buzzer or a horn indicating a possible ghost intrusion.
The whole circuit may be built over a small piece of vero-board and should be strictly operated with a 9 volt battery.
The whole system may be enclosed inside a plastic box with the antenna kept protruding out of the box.
Parts List
R1 = 100K,
R2 = 2M2,
R3, R4 = 1K,
C1 = 0.01uF ceramic
C1 = 0.01uF ceramic
OP1 = LED/LDR assembly inside a light proof enclosure,
T1 = BC557,
B1 = Piezo Electric Buzzer
READERS ARE REQUESTED TO SHARE THEIR EXPERIENCES WITH THIS DEVICE. A PHOTO OR A VIDEO PROOF WILL BE GREATLY APPRECIATED....
READERS ARE REQUESTED TO SHARE THEIR EXPERIENCES WITH THIS DEVICE. A PHOTO OR A VIDEO PROOF WILL BE GREATLY APPRECIATED....
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