Schematic | Circuit guide | Manual Wiring diagram | Electronic
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Showing posts with label for. Show all posts

Dual Oscillator For Microcontrollers

Posted by Unknown Saturday, January 11, 2014 0 comments
The MAX7378 contains two oscillators and a power-on reset circuit for microprocessors. The Speed input selects either 32.768 kHz (LF) or a higher frequency, which is pre-programmed. The type number corresponds to the standard pre-programmed value and the value of the reset threshold. There is a choice of two threshold values: 2.56 V and 4.29 V.

Both thresholds are available with all standard frequencies, which are 1 MHz, 1.8432 MHz, 3.39545 MHz, 3.6864 MHz, 4 MHz, 4.1943 MHz, and 8 MHz. However, any frequency between 600 kHz and 10 MHz is also possible. An internal synchronization circuit ensures that no glitches occur when switching between the two oscillators. The Reset output of the MAX7378 is available in three different options.


Two of the options are push-pull types, either active low or active high. The third option is open drain, which thus requires an external pull-up resistor. That is the only standard option (which is why a resistor in dashed outline is shown connected to the Reset output). The Reset signal remains active for 100 µs after the supply voltage rises above the threshold voltage.

The Reset signal becomes active immediately if the voltage drops below the threshold. The IC is powered via two separate pins. The VL pin powers the reset and oscillator circuitry, while the VCC pin powers the remainder of the chip. The two pins must always have the same potential. Good decoupling in the form of two 100-nF ceramic capacitors (SMD types) is also necessary.

The IC is housed in the tiny 8-pin µMAX package and has dimensions of only 3.05 × 5.03 mm including pins, with a pin pitch of only 0.65 mm. Unfortunately, the accuracy of the oscillators is not especially good. The HF oscillator has an error of ±2% at 25 °C with a 5-V supply voltage and a maximum temperature coefficient of +325 ppm, which doesn’t exactly correspond to crystal accuracy, but it is certainly usable for most non-time-critical applications.

The error over the full supply voltage range (2.7–5.5 V) is twice as large. The 32.768-kHz oscillator is more accurate, with an error of only 1% at 5 V and 25 °C, although this is still a bit too much for time measurements. The error can be as much as ±3% over the entire supply voltage range. The maximum current consumption is 5.5 mA, which is relatively low.

When looking for a quality laser pointer

Posted by Unknown Sunday, December 22, 2013 0 comments
When looking for a quality laser pointer, the first thing that you should do is to ask yourself on what standards of quality you are looking for in such products. Many people want a pointer that will last for a long time. This means that they will no longer be bothered by always changing the device. Aside from that, having a quality product that will give quality results for a long time can actually save you money. If you want to be sure about the quality of the laser pointer that you are going to buy, you have to do a simple research about the products. It is not about what the manufacturers say about the product but it is about what the customers say about it.

Laser pointers of today are truly amazing. With such design and features that are really high-technology, there is no way that you will not buy if you can afford it. In fact, many people already have this device especially when they really need it in their work or industry. So if you think you want to be cool by having this device, this is your opportunity to have it and show it off to your friends.

But remember, you have to also be careful in using this for it can be hazardous without following its safety instructions.I can still remember my first laser pointer when I was in college. I was a prankster then and I used to make my classmates laugh by pointing it in the forehead of my teacher and the class started to laugh. Good thing that teacher was telling corny jokes and he was amazed that many of us laughed. He was unaware that we were not laughing at his joke but at the red dot seen on his head. Yes, the pointers available then were only red. But now, you can choose from various colors available.

Going back to the uses of these laser products, many people are benefiting from the light that it gives nowadays. The intensity of the light emitted by these products is brighter than before where they can go on a frequency up to 532nm. In fact, this is the fastest selling today can beam up to 80 miles reach. That can be an awesome ability that a pointer can give. It means that the light is intense that it can even burn easily combustible materials such as dry paper. In those years of its development, many professionals and students have been using this little piece of laser technology. It is typically used as a pointer in presentations and lectures. Aside from that, they are also used in night adventures, researches, and more.

Petrol Gas Switch For A Pajero

Posted by Unknown Monday, October 7, 2013 0 comments

My current vehicle, a Pajero, was modified for dual fuel - ie, petrol and gas. However, its necessary to run the vehicle on petrol at regular intervals to stop the injectors from clogging up. This simple circuit allows the vehicle to be started using petrol and then automatically switches it to gas when the speed exceeds 45km/h and the brake pedal is pressed. Alternatively, the vehicle may be run on petrol simply by switching the existing petrol/gas switch to petrol. You can also start the vehicle on gas by pressing the brake pedal while starting the vehicle. The circuit is based on an LM324 dual op amp, with both op amps wired as comparators. It works like this: IC1a buffers the signal from the vehicles speed sensor and drives an output filter network (D1, a 560kO resistor and a 10µF capacitor) to produce a DC voltage thats proportional to the vehicles speed.

Circuit diagram:

petrol-gas-switch-for-a-pajero Circuit

This voltage is then applied to pin 5 of IC1b and compared with the voltage set by trimpot VR1. When pin 7 of IC1b goes high, transistor Q1 turns on. This also turns on transistor Q2 when the brake pedal is pressed (pressing the brake pedal applies +12V from the brake light circuit to Q2s emitter). And when Q2 turns on, relay 1 turns on and its contacts switch to the gas position. Trimpot VR1 must be adjusted so that IC1bs pin 7 output switches high when the desired trigger speed is reached (ie, 45km/h). In effect, the speed signal is ANDed with the brake light signal to turn on the relay. The vehicle has been running this circuit for several years now and is still running well, with no further injector cleans required.

Author: J. Malnar - Copyright: Silicon Chip Electronics

Source : www.extremecircuits.net

Pump Controller For Solar Hot Water System

Posted by Unknown Saturday, October 5, 2013 0 comments
This circuit optimizes the operation of a solar hot water system. When the water in the solar collector is hotter than the storage tank, the pump runs. The circuit comprises two LM335Z temperature sensors, a comparator and Mosfet. Sensor 1 connects to the solar collector panel while Sensor 2 connects to the hot water panel. Each sensor includes a trimpot to allow adjustment of the output level. In practice, VR1 and VR2 are adjusted so that both Sensor 1 and Sensor 2 have the same output voltage when they are at the same temperature. The Sensor outputs are monitored using comparator IC1.

When Sensor 1 produces a higher voltage than Sensor 2, which means that sensor 1 is at a higher temperature, pin 1 of IC1 goes high and drives the gate of Mosfet Q1. This in turn drives the pump motor. IC1 includes hysteresis so that the output does not oscillate when both sensors are producing a similar voltage. Hysteresis comprises the 1MO feedback resistor between output pin 1 and non-inverting input pin 3 and the input 1kO resistor. This provides a nominal 12mV hysteresis so that voltage at Sensor 1 or Sensor 2 must differ by 12mV for changes in the comparator output to occur.

Pump controller for solar hot water system circuit schematic

Since the outputs of Sensor 1 and Sensor 2 change by about 10mV/°C, we could say that there is a degree of hysteresis in the comparator. Note that IC1 is a dual comparator with the second unit unused. Its inputs are tied to ground and pin 2 of IC1 respectively. This sets the pin 7 output high. Since the output is an open collector, it will be at a high impedance. Mosfet Q1 is rated at 60A and 60V and is suitable for driving inductive loads due to its avalanche suppression capability. This clamps any inductively induced voltages exceeding the voltage rating of the Mosfet.

The sensors are adjusted initially with both measuring the same temperature. This can be done at room temperature; adjust the trimpots so that the voltage between ground and the positive terminal reads the same for both sensors. If you wish, the sensors can be set to 10mV/°C change with the output referred to the Kelvin scale which is 273K at 0°C. So at 25°C, the sensor output should be set to (273 + 25 = 298) x 10mV or 2.98V.

Note:

The sensors will produce incorrect outputs if their leads are exposed to moisture and they should be protected with some neutral cure silicone sealant. The sensors can be mounted by clamping them directly to the outside surface of the solar collector and on an uninsulated section of the storage tank. The thermostat housing is usually a good position on the storage tank.

LED Brake Rear Light Specifically for motorcycles Circuit diagram

Posted by Unknown Tuesday, October 1, 2013 0 comments
LEDs are used more and more in motor vehicles, replacing the standard incandescent lamps because they are more energy efficient and have a much longer life expectancy. In this article we describe a simple LED tail light that has been specifically designed for motorcycles, scooters and mopeds. There appears to be a significant need among motorcyclists for rear lights with LEDs, as evidenced by the many messages on this topic that turn up in various internet forums. The circuits that accompany these messages are often very rudimentary and therefore not very robust.

Mini project:


When designing an LED light for a motorcycle the following criteria need to be considered:

• Large variations of on-board voltage, this has a significant influence on light intensity.
• The circuit has to be (mechanically) robust.
• High light output is required (visibility = safety).
• Clearly visible difference in light intensity between rear light and brake light function.

After reading some of the literature concerning the use of LEDs in motor vehicles, it appears that the most common reason why LEDs still fail is the incorrect and/or insufficient use of series resistors.
In poorly implemented circuits there are often a number of LEDs connected in parallel which are all fed from a single series resistor. Because of small variations between LEDs, one LED can quickly give up the ghost. This causes an increase in current through the remaining LEDs and can easily lead to a domino effect, ultimately resulting in the failure of the entire circuit.With high-intensity LEDs, a small variation in current is immediately obvious as a large variation in light output.

This has to be taken into account when designing a circuit. This is important because when the engine rev speed goes up, the on-board voltage increases significantly. It would appear that you were braking when you actually opened the throttle instead.LEDs need mainly a constant current.That is why most circuits choose to drive LEDs from a constant-current source.

Circuit

This circuit has been designed to operate both as a motorcycle rear light and as a brake light. This requires two different currents. Because the voltages measured on the author’s motorcycle varied from 10.5 to 15 V and because two different currents are required for the total of 17 high-intensity LEDs it was not possible to use only one constant-current source.

Circuit diagram:

The idea was to turn the strongly varying DC voltage into a nice constant voltage first and then turn that into a constant current through a number of series resistors. The problem that is highlighted in many forums is the fact that the signal for the brake light is a positive voltage. It would require a lot of work on the motorcycle to change this. That is why the decision was made for a de sign that regulates the voltage on the chassis side, with the aid of a negative voltage regulator, a 7908. The disadvantage of this arrangement is that an additional chassis wire is required; normally the minus side of the lamps is directly connected to the chassis of the motorcycle.

However, the advantage is that both the + from the rear light as well as the + from the brake light can be directly connected to the LEDs.The ‘lamp’ con sists of a centre part with nine round, red,5-mm LEDs (HLMP EG08 Y200) wi th positioned around that eight oval ,r e d L E D s HLMP AD61 of 5 mm.The round LEDs D12 through D20 which have qui te a narrow radi ation angle are connected in series in sets of 3. Three of the se ‘strings’ are connected in parallel and each string has its own series resistor.

The oval LEDs D4 to D11 which have a wide radiation pattern are connected with two in series, so there are therefore four strings connected in parallel. These ensure with their wide radiation angle of 110 degrees that the rear/brake-light is also clearly visible from the side.The oval and round strings are connected to the brake contact via diodes. When the brake is operated all the strings are presented with the +12V from the battery via the series resistors. The light intensity therefore depends on the current that flows as a result of the series resistor (and the voltage drop across the diodes).

When the brake is not operated, the LEDs strings are still connected to the positive voltage of the battery, but this time via additional resistors R1 and R2.Because of the value of these resistors,the current is much lower and therefore also the light intensity. The intensity of the brake light can be adjusted using the series resistors (R3 to R9) in each of the individual strings,the brightness of the rear light is selected with the additional series resistors R1 and R2.Diode D1 has been added to protect the circuit from reverse connection of the power supply voltage.Electrolytic capacitors finally provide filtering for the fairly large varying,and not so clean, voltage.

The circuit was built into a silver coloured tube by the author. The electronics are mounted on two pieces of prototyping board, one behind the other,in the tube. The front (visible) PCB holds the LEDs and the series resistors. The LEDs are arranged as indicated next to the schematic. The 9 round LEDs are mounted in the middle of the rear light in a square pattern. The oval LEDs are mounted in a circle around the square.

The second PCB contains the remaining parts and the regulator.You can modify the circuit to your heart’s content by adding more strings, each fitted with its own diode and two resistors (a series resistor such as R3) and a resistor to +12 V (such as R1).The total current (when braking), must not exceed the maximum rating of the voltage regulator, this amounts to 1 A.

Author : Marcel Ulrich Copyright : elektor

Preamplifier For Soundcard

Posted by Unknown Monday, September 23, 2013 0 comments
This circuit can be used for inductive pick-up elements and dynamic microphones Most soundcards have a ‘line’ input and one for an electret (condenser) microphone. To be able to connect an inductive tape-recorder head or a dynamic microphone, an add-on preamplifier is needed. Even in this day and age of integrated microelectronics, a transistorised circuit built from discrete part has a right of existence. The preamplifier described in this short article goes to show that it will be some time before discrete transistors are part of the silicon heritage. The preamplifier is suitable for use with a soundcard or the microphone input of a modem. As you will probably know, most sound-cards have input sockets for signals at line level (stereo), as well as one for a (mono) electret microphone.

For the applications we have in mind, connecting-up an inductive pick-up element or a dynamic microphone, both inputs are in principle suitable, provided the source signal is amplified as required. The author eventually chose the microphone input on the soundcard. Firstly, because the line inputs are usually occupied, and secondly, because the bias voltage supplied by the micro-phone input eliminates a separate power supply for the preamplifier. The microphone input of a soundcard will typically consist of a 3.5-mm jack socket in stereo version, although only one channel is available. The free contact is used by the soundcard to supply a bias voltage to the mono electret microphone. This voltage is accepted with thanks by the present preamplifier, and conveniently obviates an external (mains adaptor) power supply.

Preamplifier For SoundcardA classic design:

In true transistor-design fashion, the preamplifier consists of three stages. Capacitor C1 decouples the signal received from the microphone or pick-up element, and feeds it to the input of the first stage, a transistor in emitter configuration, biased to provide a current amplification of about 300 times. Together with the source impedance of the microphone or pick-up element, capacitors C2 and C3 form a low-pass filter which lightly reduces the bandwidth. In addition, the output low-pass, R2-C3, reduces the dynamic collector resistance at higher frequencies. In this way, the filter reduces the gain in the higher part of the frequency spectrum and so helps to eliminate any oscillation tendencies.

The first, high-gain, stage is terminated by T2. Unlike T1, this transistor does not add to the overall gain, because the output signal is taken from the emitter (common-collector circuit). T2 thus acts as an impedance converter, with C4 reducing any tendency to oscillation. The output stage around T3 is a common-emitter circuit again. In it, preset P1 determines the voltage amplification. T3 is biased by means of a direct-current feedback circuit based on components R7 and C5. To this is added an ‘overruling’ dc feedback path back to the input transistor, via R6. This measure guarantees good dc stability in the preamplifier. The circuit is small enough to be built on a piece of veroboard or stripboard, and yet remain reasonably compact.

To prevent interference from external sources, the completed board should be mounted in a properly screened (metal) enclosure, with the connections to the input source and the sound card made in screened cable. The preamplifier provides a frequency-linear response. In case the source signal is marked by frequency correction (e.g., RIAA), then a matching linearization circuit should be used if the relevant signals are used by the computer.

Dual Power Supply For Amplifiers

Posted by Unknown Sunday, September 22, 2013 0 comments
A power supply suitable for use with the 60W amplifier presented in the predeeding project is perfectly simple, and no great skill is required to build (or design) one. There are a few things one should be careful with, such as the routing of high current leads, but these are easily accomplished. The first thing to choose is a suitable transformer. I suggest toroidal transformers rather than the traditional "EI" laminated types because they radiate less magnetic flux and are flatter, allowing them to be installed in slimmer cases.

They do have some problems, such as higher inrush current at switch on, which means that slow blow fuses must be used. For the 60W amplifier, a nominal (full load) supply of +/- 35V is required, so a 25-0-25 secondary is ideal - however, see Updates, below. The circuit for the supply is shown below, and uses separate rectifiers, capacitors and fuses for each channel. Only the transformer is shared, so channel interactions are minimised. A single ±35V supply (i.e. using only a single bridge and set of filter capacitors) will work just as well in the majority of cases.

Dual Power Supply circuit diagram For AmplifiersThe 5A slow-blow fuse shown is suitable for a 300VA transformer, if a 120VA transformer is used, this should be reduced to 2.5A (or 3A if 2.5A proves too hard to get). If you are even a little bit concerned about the fuse rating, contact the transformer manufacturer for the recommended value for the transformer you will use. The correct fuse is critical to ensure safety from electrical failure, which could result in the equipment becoming unsafe or causing a fire.

The capacitance used is not critical, but is somewhat dependent upon ones budget. I suggest 10,000uF capacitors, but they are rather expensive so at a pinch 4,700uF caps should be fine - especially in the arrangement shown. When unloaded (or with only light load), the voltage will normally be somewhat higher than 35 Volts. This is Ok, and should not cause distress to any amp. The voltage will fall as more current is drawn, and may drop below 35V if a small transformer (or one with unusually poor regulation) is used.

Two parts of this circuit are critical:
  • Mains wiring must be cabled using approved 240V rated insulated cable, and all terminations must be insulated to prevent accidental contact. The mains earth must be securely fastened to the chassis, after scraping away any paint or other coating which might prevent reliable contact.
  • The centre-tap of the transformer and the ground points of each capacitor must be connected to the main signal earth point via heavy duty copper wire, or (preferably) a copper bus-bar. Large currents flow in this part of the circuit, containing nasty current waveforms which are quite happy to invade your amplifier. The supply voltages must be taken from the capacitors (not the bridge rectifiers) to prevent unwanted hum and noise.
When wiring the bridge rectifiers to the transformer, connect exactly as shown to ensure that ripple voltages (and currents) are in phase for each amp. If not, mysterious hum signals may be injected into the amps signal path from bypass capacitors and the like. This is somewhat unlikely unless huge caps are used on the amp board(s) - not recommended, by the way - but why take the risk?

Bridge rectifiers should be the big bolt-down 35A types (or something similar) to ensure lowest possible losses (these will not require an additional heatsink - the chassis will normally be quite sufficient). The transformer primary voltage will obviously be determined by the supply voltage in your area (i.e. 120, 220 or 240) and be suited to the local supply frequency. Note that all 50Hz transformers will work just fine at 60Hz, but some 60Hz devices will overheat if used at 50Hz.

The transformer should be rated at a minimum of 120VA (Volt-Amps) for home use, but a 300VA transformer is recommended due to its superior regulation. Going beyond 300VA will serve no useful purpose, other than to dim the lights as it is turned on. Where it is possible, the signal and power ground should be the same (this prevents the possibility of an electric shock hazard should the transformer develop a short circuit between primary and secondary. Where this will give rise to ground loops and hum in other equipment, use the method shown.

The resistor R1 (a 5W wirewound resistor is suggested) isolates the low-voltage high-current ground loop circuit, and the diodes D1 & D2 provide a protective circuit in the event of a major problem. These diodes need only be low voltage, but a current rating of 5A or greater is required. The 100nF capacitor (C1) acts as a short circuit to radio frequency signals, effectively grounding them. This should be a device with very good high frequency response, and a monolithic ceramic is recommended.

Updates:

The transformer secondary voltage will probably need to be higher than described above. I tested some stock and custom transformers I have, and found that unless the transformer has extraordinarly good regulation, a nominal 28-0-28 secondary will be needed, more with an average (i.e. poor) regulation unit. Also be careful when you test, since a relatively small (10%) variation in the mains voltage makes a big difference to measured output power - the secondary voltage also falls by 10%, so 60W becomes 48W if the mains is 10% low.

You also need to remember that the output voltage of transformers is typically quoted at full power with a resistive load. This means two things:
  1. The no load voltage will be higher than expected
  2. The loaded voltage will be lower than expected
The first point is true because there is no loading, so the output voltage must rise. The second is more complex, but happens because the conventional rectifier circuit uses a capacitor input filter (the rectifier feeds directly into the capacitor(s)). Since the diodes only conduct at the peak of the waveform, the current is much higher, so the transformer and supply line impedance will cause the peak voltage to fall, and the DC voltage cannot exceed the peak output voltage (less two diode forward voltage drops).
Source: http://sound.westhost.com/project04.htm

Wiring Diagrams Application for Any Vehicle

Posted by Unknown Tuesday, August 6, 2013 0 comments

Shiftlight does not respond to buttons being pressed. The engine must be running in order to set the pre-shift and shift points on the shiftlight. The unit requires an input signal (tachometer, coil negative, crank angle sensor)if there is no input signal the unit will not respond whenbuttons pressed. MITSUBISHI RVR N23W 4G63 1992 – 97 GM – 2 President G50 VH45DE 1990 – GN – 4 Infinity Q45 G50 VH45DE 1989 – 97.

Pajero V23W 6G72 1991 – GM – 2 N74W 4G64 GM – 3 N73W 4G63 M/T GM – 3 N71W 4G93 N61W 1997 – GM – 3 Cinma III FGY33 VH41DE 1996 – 98 GN – 6 FHY33 VQ30DET GN – 5 Cinma II FGY32 VH41DE 1991 – 96 GN – 4 FPY32 VG30DET 1993 – 96 Cinma I FPY31 VG30DET 1989 – 91 FPY31 VG30DE FPY31 VG30DET 1988 -89 GN – 1 FPY31 VG30DE.

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How much do the fuel tanks capacities and tank codes for the 1990 Chevrolet Cheyene 2500

Posted by Unknown Wednesday, July 31, 2013 0 comments



How much do the fuel tanks capacities and tank codes for the 1990 Chevrolet Cheyene 2500?


Answer: The short bed is 26 gallon while the long bed is a 34 gallon. You can find the data in the owner’s manual under capacities. A sticker in the glove box should contain all of the RPO codes for your truck.

SW Converter for AM Radio

Posted by Unknown Tuesday, July 30, 2013 0 comments
Apart from chucking it in the bin, what can you do with outdated AM automobile radio or clock radio in your junkbox? How about fliping it right into a crystal managed, secure, quick wave radio receiver, for a minimal funding in time and money? Read on. The coronary heart of the circuit shown here is an IC which works by the title NE602, NE612 or SA612. It is a double balanced mixer that features an oscillator that can be crystal-controlled, free working or even pushed externally from a PLL, and many others. It was once in the beginning designed for cellular telephones and is most probably to be had in junked car telephones from the tip. The NE602/612 accommodates a differential input amplifier (called a Gilbert Cell), an oscillator/buffer, a temperature compensated bias community and a energy regulator. Typical frequency response is in far more than 500 MHz for the input and 100 MHz for the oscillator.
Circuit diagram :
SW Converter for AM Radio Circuit Diagram
 
Supply present is 2.4 mA and the absolute maximum provide voltage is 9 V. Input and output impedances are approx. 1.5 kΩ. As you'll find from the circuit diagram, the enter from the aerial is handed through a ten.7 MHz IF (intermediate frequency) transformer. This offers isolation from the aerial and cut backs the effect of sturdy local AM radio step forward.The transformer may also be salvaged from a dead FM radio or stereo or even the FM component to an previous clock radio. (The AM part is what we want to use anyway so ratting just a little from the FM section keeps cost). A selection of 10.7 MHz IF coils from Toko and other far-Eastern manufacturers may be used, together with the 94AES30465N and 94ANS30466N, but obtaining these as new phases may be more pricey than an entire radio rescued from the tip. There is on a standard basis a small capacitor under the IFT coil, between the pins. If so, do away with it by means of crushing it with a pair of pliers and ripping out the remains. The capacitor will no longer be wanted as we add an exterior one in step with the band wished. The input sign is fed into the balanced input of the IC.
 
The crystal is hooked up to pin 6. It oscillates at its fundamental frequency and that is mixed with the input signal giving a selection of outputs. The mixer output signal appears on pins four and 5. Here, handiest pin 5 is used for the output. By the way, the enters and outputs are interiorly biased with pull-up resistors, so there's no have to tie the unused pins to ground or energy. The 220 pF capacitor offers isolation to any DC into the AM radio aerial input. Note also that the same circuit can be used to increase the selection of an present short wave radio receiver in precisely the identical method. The AM radio is used as a tuneable intermediate frequency amplifier, with a tuning vary of about 1.6 MHz. You can are attempting different prices for C1 to get resonance on the NE602 input: a hundred and fifty pF for up to 5 MHz, forty seven pF for up to 8 MHz, and no capacitor for as a lot as 10 MHz. In apply however 33 pF will have to do for all ranges. Almost any crystal can be utilized. The creator tried many varieties from FT-243 WW2 surplus ones to 27 MHz, third overtone CB crystals. Every crystal tried worked. TV sub-carrier crystals work well, as do large oven varieties. Several crystals can additionally be linked through a switch, giving a convenient manner of swaping bands. Keep the leads to the swap as short as that that you can think of though to forestall radiation of the crystal oscillator. There are many tips on how to construct the circuit. You could make it right into an external metallic field that can be related to a quantity of radio’s, depending in your location. For instance, if you're a traveller, make it in a small box with an internal 9-volt battery, and leave sufficient wire on the output to wrap a few dozen flips across the clock radio in your Hotel room.


This gives you your quick-wave reception on the go. It can also be imaginable to construct the converter proper into the auto radio. Any form of development method can be used, from a small piece of perforated board that I used, to a extra problematic printed circuit board and even simply lash all of the small components beneath the IC socket. A small swap is additionally used to alter from AM to short-wave. Connect the circuit to the car radio with screened cable to stop or lessen the impact of robust station step forward. To couple the output of the converter to a radio with out an external AM aerial enter, wind several turns of wire round the interior ferrite rod aerial. As steered before, winding a dozen or so turns across the plastic radio case will additionally couple the converter to the radio. This will work at the fee of increased AM sign breakthrough. Connect the positive power lead to the switch on the radio so that it changees the converter on and off as well.

The quick-wave aerial can be 2 to a few meters of wire strung across the room, but better outcomes can be received with a outdoor aerial. The take a look at aerial was about one hundred meters lengthy and 10 meters high. At evening there is a lot of job on the short waves after darkish. Find a weak station round 1 MHz on the AM dial and alter the core of the IFT for minimal extent from the broadcast station. That’s the simplest alterment. SSB alerts can additionally be heard, but as no beat frequency oscillator is fitted, you hear the “duck talk” of the signal. The 10 kHz bandwidth of the radio means that on the ham bands, signals do overlap, however it also makes the broadcast stations sound higher as most of them do broadcast with cheap high quality audio. Digital tuned AM radios are on a regular basis no longer appropriate for the circuit as introduced, because the tuning steps are 9 or 10 kHz apart and we wish a lot smaller steps. The previous manually tuned varieties of automotive radio are what you wish to have. The idea of the circuit is to no lengthyer get too complicated, but to just experience listening on a simple, stable, low cost, brief wave receiver. Experiment and experience!


Author : P. Laughton, VK2XAN – Copyright: Elektor Electronics

Contrast Control for LCDs

Posted by Unknown Thursday, April 11, 2013 0 comments
The adjustment control for the contrast of an LC-Display is typically a 10-k potentiometer. This works fine, provided that the power supply voltage is constant. If this is not the case (for example, with a battery power supply) then the potentiometer has to be repeatedly adjusted. Very awkward, in other words. The circuit described here offers a solution for this problem. 

The aforementioned potentiometer is intended to maintain a constant current from the contrast connection (usually pin 3 or Vo) to ground. A popular green display with 2x16 characters ‘supplies’ about 200 µA. At a power supply voltage of 5 V there is also an additional current of 500 µA in the potentiometer itself. Not very energy efficient either. Now there is an IC, the LM334, which, with the aid of one resistor, can be made into a constant current source. The circuit presented here ensures that there is a current of 200 µA to ground, independent of the power supply voltage. By substituting a 2.2-k? potentiometer for R1, the current can be adjusted as desired.

Circuit diagram:The value of R1 can be calculated as follows: R1 = 227x10-6 x T / I. Where T is the temperature in Kelvin and I is the current in ampères. In our case this results in:
R1 = 227x10-6 x 293 /
(200x10-6)
R1 = 333R

Note that the current supplied by the LM334 depends on the temperature. This is also true for the current from the display, but it is not strictly necessary to have a linear relationship between these two. Temperature variations of up to 10° will not be a problem however. This circuit results in a power saving of over 25% with an LCD that itself draws a current of 1.2 mA. In a battery powered application this is definitely worth the effort! In addition, the contrast does not need to be adjusted as the battery voltage reduces. When used with LCDs with new technologies such as OLED and PLED it is advisable to carefully test the circuit first to determine if it can be used to adjust the brightness.

Circuit diagram:
contrast-control-for-lcd-circuit-diagramw
Contrast Controller Circuit Diagram For LCDs

The value of R1 can be calculated as follows: R1 = 227x10-6 x T / I. Where T is the temperature in Kelvin and I is the current in ampères. In our case this results in:
  • R1 = 227x10-6 x 293 /
  • (200x10-6)
  • R1 = 333R
Note:
  • The current supplied by the LM334 depends on the temperature. This is also true for the current from the display, but it is not strictly necessary to have a linear relationship between these two. Temperature variations of up to 10° will not be a problem however. This circuit results in a power saving of over 25% with an LCD that itself draws a current of 1.2 mA. In a battery powered application this is definitely worth the effort! In addition, the contrast does not need to be adjusted as the battery voltage reduces. When used with LCDs with new technologies such as OLED and PLED it is advisable to carefully test the circuit first to determine if it can be used to adjust the brightness.
     
     
    http://www.ecircuitslab.com

Preamplifier For Soundcard

Posted by Unknown Wednesday, April 10, 2013 0 comments
This circuit can be used for inductive pick-up elements and dynamic microphones Most soundcards have a ‘line’ input and one for an electret (condenser) microphone. To be able to connect an inductive tape-recorder head or a dynamic microphone, an add-on preamplifier is needed. Even in this day and age of integrated microelectronics, a transistorised circuit built from discrete part has a right of existence. The preamplifier described in this short article goes to show that it will be some time before discrete transistors are part of the silicon heritage. The preamplifier is suitable for use with a soundcard or the microphone input of a modem. As you will probably know, most sound-cards have input sockets for signals at line level (stereo), as well as one for a (mono) electret microphone.

For the applications we have in mind, connecting-up an inductive pick-up element or a dynamic microphone, both inputs are in principle suitable, provided the source signal is amplified as required. The author eventually chose the microphone input on the soundcard. Firstly, because the line inputs are usually occupied, and secondly, because the bias voltage supplied by the micro-phone input eliminates a separate power supply for the preamplifier. The microphone input of a soundcard will typically consist of a 3.5-mm jack socket in stereo version, although only one channel is available. The free contact is used by the soundcard to supply a bias voltage to the mono electret microphone. This voltage is accepted with thanks by the present preamplifier, and conveniently obviates an external (mains adaptor) power supply.

Preamplifier For Soundcard Circuit diagram:


A classic design:
In true transistor-design fashion, the preamplifier consists of three stages. Capacitor C1 decouples the signal received from the microphone or pick-up element, and feeds it to the input of the first stage, a transistor in emitter configuration, biased to provide a current amplification of about 300 times. Together with the source impedance of the microphone or pick-up element, capacitors C2 and C3 form a low-pass filter which lightly reduces the bandwidth. In addition, the output low-pass, R2-C3, reduces the dynamic collector resistance at higher frequencies. In this way, the filter reduces the gain in the higher part of the frequency spectrum and so helps to eliminate any oscillation tendencies.

The first, high-gain, stage is terminated by T2. Unlike T1, this transistor does not add to the overall gain, because the output signal is taken from the emitter (common-collector circuit). T2 thus acts as an impedance converter, with C4 reducing any tendency to oscillation. The output stage around T3 is a common-emitter circuit again. In it, preset P1 determines the voltage amplification. T3 is biased by means of a direct-current feedback circuit based on components R7 and C5. To this is added an ‘overruling’ dc feedback path back to the input transistor, via R6. This measure guarantees good dc stability in the preamplifier. The circuit is small enough to be built on a piece of veroboard or stripboard, and yet remain reasonably compact.

To prevent interference from external sources, the completed board should be mounted in a properly screened (metal) enclosure, with the connections to the input source and the sound card made in screened cable. The preamplifier provides a frequency-linear response. In case the source signal is marked by frequency correction (e.g., RIAA), then a matching linearization circuit should be used if the relevant signals are used by the computer.

Source : http://www.ecircuitslab.com/2011/07/preamplifier-for-soundcard-circuit.html

Radio Control for toy car

Posted by Unknown Sunday, April 7, 2013 0 comments
Radio Control for toy car
Play toy cars controlled by radio signals is an interesting game. The much-loved toy cars children, plus a simple circuit would be ideal for toy cars. This series of families use traditional digital CMOS IC which requires a very small electric current, so it does not impose on the performance of the original toy cars.
In this system, radio signals emitted not continuously but only generated when the controller sends a command left / right or forward / backward, and even then only a radio frequency of an intermittent, so it is sending pulses of radio wave frequency.
Number of pulses sent represents a command is sent, the command GO is represented by 8 pulses, represented by 16 pulses LEFT, RIGHT DOWN 32 pulses and 64 pulses. Command sent to a combination of two orders once gus, which is a combination of command forward / backward and right / left, for example, could be sent forward command and left once gus, in this case the number of pulses sent is 24, which is the sum of the forward command command as much as 8 pulses and left as many as 16 pulses.
Once a command is sent, the system stops sending commands in a certain time lag, the lag time it takes the receiver circuit will have sufficient time to execute properly. Frequency pulses were visible on the right side of Figure 1.

How it works The transmitter
Radio signals generated by the oscillator circuit formed by transistors Q1 9016, the working frequency of the oscillator is determined by the crystal Y1 is worth 27.145 MHz. A very critical part of this oscillator circuit is T1, L1 and L2, which specifically dealt with separately at the end of this article.
Work of the oscillator is controlled by a NOR gate U2D 14001, while the output gate (pin 3) is worth 1 , the oscillator will work and transmit radio frequency 27.145 MHz, and at the output U2D value 0 the oscillator will stop working.
U2D NOR gate receives the clock signal from the NOR gates U2B. NOR gate CMOS type with the help of resistors R4 and R5 and capacitor C8 to form a low frequency oscillator circuit to control the clock shaper of existing digital circuits. Working from the clock generator is controlled via the input leg 6, the circuit will generate the input clock that is berlevel 0 .
NOR gate U2A and U2C form a latch circuit (RS Flip Flop), due to the influence of resistor R2 and capacitor C11 which is fed to pin 9 on U2C, when the circuit gets power supply output U2C must be 1 and U2A output (pin 3) to 0 . This situation resulted EUIS clock generator generating a clock U2B work and release the reset state of the enumerator 14 024 IC (U1), so that the U1 start chopping and 27.145 MHz oscillator circuit to send pulses of the clock generator frequency during work.
At the start chopping, all the output IC 14 024 enumerators in kedaan 0 , after chopping the 8 pulse output Q4 (pin 6) will be 1, after chopping 16 Q5 pulse output (pin 5) to 1 , after chopping 32 Q6 output pulse (pin 4) to 1 , after 64 counts pulses output Q7 (pin 3) to 1.
Outputs are used to control the voltage above 9 feet U2C through diode D1 and D2, as long as it remains one of the output value 0 then the plant U2B clock still works, it will continue until dankatode D2 D1 cathode to 1 so that the foot 9 U2C a 1 as well. This situation will lead to 3 feet U2A output to 1 , which stops the clock generator and reset U2B enumerator 14 024 danberhenti is sending pulses of frequency 27 145 MHz.
To generate the lag time for the receiver circuits have enough time to perform the command, used a series of 9014 Q2, the resistor R7 and capacitor C10. The magnitude of the delay time is determined by the value of R7 and C10. The switch to send the command forward / backward and to send the command left / right are two separate switches. Each switch has three positions, the center position means that the scalar does not send commands.
How It Works Recipients
Figure 2 is a recipient of a series of paired images dimobil toy, serves to receive signals from the transmitter to control the motor cars, so cars can move forward / backward and left / right. Transistor Q1 with the help of resistors; capacitors and T1 form as a series of 27.145 MHz radio signal receiver. T1 in series with a T1 is exactly the same used in the transmitter circuit, how to make it are discussed below.
Transistor Q2 perlangkapannya formed following a series of pulses to change the radio frequency received from the transmitter into the box pulses that can be accepted as a digital signal by the CMOS IC. Digital signal will be received as the clock had to be chopped by enumerator 14 024 IC (U2). Output of 14 024 would correspond to the number of pulses sent by the transmitter, forward command and left (which is used as an example in the discussion of the transmitter) is the pulse number of 24, the enumeration of these pulses resulted in 14 024 to be output Q4 = 1 , Q5 = 1, Q6 = 0 and Q7 = 0.
The received digital signal other than U2 used as counter clock IC 14 024 discussed above, is also used to move the 3 pieces of the time delay circuit to generate pulses which controls the sequence of work.
The first control pulse will appear after submission frequency pulse stopped because the lag time between sending the code, this pulse count function to record the results of 14 024 to 14 042 U3 (D Flip Flop), so that the final condition of 14 024 will be retained to control the motor. After the results were recorded for 14 024 14 042, 14 042 counter is reset by the second pulse, so that after the lag time counter counts up starting from 14 042 to 0 again.
Circuit formed by transistors Q3, Q4, Q7, Q8, Q9 and Q10 H Bridge is named as a series, this series is very powerful to drive the DC motor. With this circuit the DC motor can be rotated to the right-to-left or stop motion. The main requirement is the use of this circuit Q7 and the base voltage of Q10 base voltage must be opposed, for example, the base Q7 = 1 and the base of Q10 = 0 motor rotates to the left, the base of Q7 = 0 and the base of Q10 = 1 motor will turning to the right, the base Q7 = 0 and Q10 base = 0 motor stop motion, but should not be happening base Q7 = 1 and the base Q10 = 1.
Similarly, Q5, Q6, Q11, Q12, Q13 and Q14 form an H Bridge. H Bridge to the left in Figure 2 is used to control a motor that regulates the movement of cars left / right, while the H Bridge to the right is used to control a motor that regulates the movement forward / backward cars.
The relationship between outpur enumerator 14 042 and input D Flip Flop 14 024 is arranged such that the signal is fed to each of the H Bridge can not be all 1 simultaneously.


Manufacture of transformer TX and RX
Transformer T1 in the series transmitter and receiver, is the same stuff, and have made ​​themselves. Transformer was built using a plastic transformer Koker (spare part radio) that has a step that appears 5 lines that can be filled with coils of wire, as shown in the photograph. Wearing this Koker facilitate wire transformer windings. Otherwise it could be similar Koker, just the usual wear. Koker is a small transformer and feritnya also small (3 mm) as that used to be used for the assembly of CB 27 MHz radio.
Can wear a wire to wire the transformer in the unloading of Koker, carefully open coil of wire that already exist in the Koker because the wire is quite smooth and quite easy to break.
Step 1: rolls of wire which is numbered 5 feet to 4 feet in the direction of h (CW) for 3 rolls right on level 1 (pathway level above the bottom line)
Step 2: Roll the wire from 1 foot to 2 feet in a clockwise direction as much as 4 rolls right on level 2.
Step 3: Continue the roll (from step 2) in a clockwise direction as much as three quarter roll to 3 feet on three levels. (Can be determined exactly a quarter of the roll, because it has a track kokernya split into 4).
Manufacture of coil L1
Roll of copper wire diameter from 0.3 to 0.5 mm by 10 quarter rolls on Koker diameter of about 4 mm (which will be released) is also in a clockwise direction.
Manufacture of coil L2
Roll of copper wire 0.1 mm diameter by 50 rolls in plastic Koker without ferrite diameter of about 3.5 - 4 mm (look for the plastic material from scrap) is also in a clockwise direction. Long section on liputi rolls along the 5 mm.

Watch Dog For Telephones

Posted by Unknown 0 comments
Most of the telephone security devices available in market are simple but quite expensive. These devices provide blinking or beeping type line-tap/misuse indications. Quite often they do not offer guaranteed protection against unauthorized operation. A very simple and unique circuit of a telephone watch-dog to safeguard subscriber telephone lines against any fraud is described here. This little circuit keeps continuous watch over the telephone lines and sounds an alarm in case of any misuse. In addition it transmits a loud tone through the telephone lines to prevent further misuse. When switch S1 is turned on, the normal (on-hook) telephone line voltage at the output of bridge-rectifier diodes D1 to D4 is approximately 48 volts, which being well above the break-down voltage of zener diode D5, the diode conducts.

Watch-Dog For Telephones  Circuit DiagramAs a result transistor T2 gets forward biased. This effectively grounds the base of transistor T1 which is thus cut off and the remaining circuit does not get any power supply. In this state, only a small (negligible) current is taken by the circuit, which will not affect the telephone line condition. However, when handset of any telephone connected to the telephone lines is lifted (off-hook), line voltage suddenly drops to about 10 volts. As a result, transistor T2 is switched off and transistor T1 gets forward biased via resistor R1. Now, the astable multivibrator built around timer IC1 starts oscillating and the speaker starts sounding.

Output of the astable multivibrator is also connected to the base of transistor T1 through capacitor C5. As a result, only a loud (and irritating) tone is heard in the ear-piece of the unauthorized telephone instrument. This circuit can be constructed on a veroboard using easily available low-cost components and it can be connected to any telephone line without the fear of malfunctioning. No extra power supply is required as it draws power from the telephone line for operation.

Note:
  • Please disconnect the gadget when you are yourself using the telephone as it cannot distinguish between authorized and unauthorized operation.

Diode Radio For Low Impedance Headphones

Posted by Unknown Friday, April 5, 2013 0 comments
If you ever look at construction notes for building old detector type radios the type of headphones specified always have an impedance of 2 × 2000Ω. Nowadays the most commonly available headphones have an impedance of 2 × 32 Ω, this relatively low value makes them unsuitable for such a design. However, with a bit of crafty transformation these headphones can be used in just such a design. To adapt them, you will need a transformer taken from a mains adapter unit, the type that has a switchable output voltage (3/4.5/6/9/12 V) without the rectifying diodes and capacitor. Using the different taps of this type of transformer it is possible to optimize the impedance match.

Diode Radio Circuit Diagram For Low Impedance HeadphonesFor the diode radio (any germanium diode is suitable in this design) the key to success is correct impedance matching so that none of the received signal energy is lost. The antenna coil on the 10 mm diameter by 100 mm long ferrite rod is made up of 60 turns with a tap point at every 10 turns; this is suitable for medium wave reception. If a long external aerial is used it should be connected to a lower tap point to reduce its damping effect on the circuit. You can experiment with all the available tapping points to find the best reception. With such a simple radio design, the external aerial will have a big influence on its performance.

Tip:
If your house has metal guttering and rain water pipes, it will be possible to use these as an aerial, as long as they are not directly connected to earth. Those who live in the vicinity of a broadcast transmitter may be able to connect a loudspeaker directly to the output or if the volume is too low, why not try connecting the active speaker system from your PC?