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

How Regulator with 2 Photocoupler

0 comments
Working of Regulator with 2 Photocoupler that is :
  • Photocoupler N901 - used as a coupling-off control on the regulator by mikrokontrol. Which is set high and low voltage B + (st-by at the B + voltage is low). Control of the pin-37 POWER mikrokontrol → V610 → VD913 V908 → N901.
  • Photocoupler N903 - used to control on-off the regulator of X-ray circuit protector. X-ray protector circuit of flyback → VD451 → VD452 → SCR VS472. If the flyback voltage regulator over the job will automatically be turned off by N903
  • To disable the X-ray circuit protector, it can be temporarily removed photocoupler N903 first. In normal conditions the voltage at the transistor V474 should be zero.

Regulator Schematics
Trobelshuting there is no voltage for 5v st-by on the secondary :

  1. Disable by removing the first circuit protectors N903
  2. Check the voltage of 300V
  3. Check all transistors
  4. Check the start voltage of 300V by R909 >> R906 to the base of transistor power regulator
  5. Check the feedback C910 >> R904 (to oscillate)
Continue reading[...]

12 Volt Charger Circuit with LM350

0 comments
The strength supply routine structure is developed as a resource of continuous present with adverse heat range coefficient. Transistor Q1 (BD 140) is used as a heat range indicator. transistor Q2 is used to avoid the strength supply from discharging through R1 when strength is out of stock. Getting routine is developed depending on the LM350 present regulator IC. The result present of the battery charger can be altered between 13-15 V by various the POT R6.



LM350 will try to keep the present decrease between the feedback pin and result pin at a continuous value of 1.25V. So there will be a continuous present circulation through resistor R1. Q1 act here as a heat range indicator with the help of R6/R3/R4 elements that are more or less manages the platform present of Q1. As relationship emitter / platform of transistor Q1, the same as other semiconductors, containing the heat range coefficient of-2mV / ° C, the present result will also display a bad heat range coefficient. This one is just a aspect of 4 huge, because the difference of the emitter / platform of Q1 is increased by a aspect of category P1/R3/R4. This causes some-8mV / ° C. LED will lighting whenever strength is available.
Continue reading[...]

Solar tracker With AT89S52

0 comments
AT89S52 With solar tracker is a tool used to control the direction of the panel Solar Cell for always getting sunlight. AT89S52 With solar tracker uses a light sensor as a light detector. AT89S52 With solar tracker uses dc motors for Solar Cell panels menegendalikan direction. Broadly speaking AT89S52 With Solar tracker may be analogous as a tool to adjust the position of the exposure to the sun solar cell  direction by Ensor sensing light and a DC motor which is controlled using a microcontroller AT89S52.

Solar tracker With AT89S52

Solar


Pictured above is a series that could be used for the light sensor on the solar tracker With AT89S52. The light sensor on AT89S52 With Solar tracker can use the LDR. Configuring LDR on Solar Tracker With AT89S52 using OP-Amp as a signal conditioner output of the LDR.
Continue reading[...]

Timer with about 10 minutes

0 comments
Applications of 555 timer IC is very diverse, one series of 10 Minute Timer with IC 555. 10 Minute Timer This circuit uses IC NE555 is set as a monostable multivibrator. The timing of the timer circuit 10 minutes with the IC 555 is governed by the configuration of C2, R4 and R5. The greater the value of C2 at 10-minute timer circuit with IC 555 timer is active then the time will stay longer. 

Total resistance value between R4 and R5 also determine the active circuit 10 minute timer with IC 555, where the greater the value the longer time was also active. The core active setting the timer on the set of C2 charging time for 10 minutes on the timer circuit with IC 555. So, with the value of C2 remain so with time on the circuit timing Timer 10 minutes by IC 555 can be set by changing the resistance value R 4 + R 5. Indicators of active timer at 10 minute timer circuit with IC 555 uses the LED D2 and D3 will light up only one course to identify the active timer and the timer has not been met.


Figure 10 Minute Timer circuit with IC 555


Description:

S1 is used to set / reset timer
R5 is used to set the timer to the desired time
Continue reading[...]

Drive Stepper Motor with IC UCN5804

0 comments
IC IC UCN5804 is designed specifically for the purpose of stepper motor drivers. Stepper motor driver IC UCN5804 with this very simple and uses only 2 additional components as current-limiting resistors which flows into the stepper motor, it also can be removed so that the stepper motor driver is a pure IC UCN5804 only use only. UCN5804 IC can be used for stepper motor driver with 5-20VDC voltage. Source voltage required for a series of stepper motor driver IC dengn this UCN5804 follow steppernya motor voltage. Picture a series of stepper motor driver ICs with UCN5804 in detail can be seen in the following figure.

Drive Stepper Motor circuit UCN5804

Drive

In the series of stepper motor drivers with IC UCN5804 above to run a DC motor takes 2 inputs ie, the input signal and the input logic stepper direction of rotation. The input signal is a pulse stepper with a certain frequency where the frequency of these pulses that determines the speed of stepper motor puter. Then the input logic is a stepper motor rotating direction input logic 0 and 1 that is given to the IC UCN5804 to adjust the stepper motor rotating direction.
Continue reading[...]

Ramp Generator With 555 Timer IC

0 comments
We apperceive that if a capacitor is answerable from a voltage antecedent through a resistor, an exponential waveform is produced while charging of a capaci­tor from a connected accepted antecedent produces a ramp. This is the abstraction abaft the circuit. The circuit of a access architect application timer 555 is apparent in figure. Here the resistor of previ­ous circuits is replaced by a PNP transistor that produces a connected charging current.

Charging current produced by PNP constant current source is

iC = Vcc-VE / RE

where VE = R2 / (R1 + R2) * VCC + VBE

When a trigger starts the monostable multivibrator timer 555 as shown in figure, the PNP current source forces a constant charging into the capacitor C. The voltage across the capacitor is, therefore, a ramp as illustrated in the figure. The slope of the ramp is given as
Continue reading[...]

10 000x With One Transistor Diagram Circuit

0 comments
For a collector follower with emitter resistor, you’ll often find that the gain per stage is no more than 10 to 50 times. The gain increases when the emitter resistor is omitted. Unfortunately, the distortion also increases. With a ubiquitous transistor such as the BC547B, the gain of the transistor is roughly equal to 40 times the collector current (Ic), provided the collector current is less than a few milliamps. This value is in theory equal to the expression q/KT, where q is the charge of the electron, K is Boltzmann’s constant and T is the temperature in Kelvin.

For simplicity, and assuming room temperature, we round this value to 40. For a single stage amplifier circuit with grounded emitter it holds that the gain Uout /Uin (for AC voltage) is in theory equal to SRc. As we observed before, the slope S is about 40Ic. From this follows that the gain is approximately equal to 40I cRc. What does this mean? In the first instance this leads to a very practical rule of thumb: that gain of a grounded emitter circuit amounts to 40·I c·Rc, which is equal to 40 times the voltage across the collector resistor.

If Ub is, for example, equal to 12 V and the collector is set to 5V, then we know, irrespective of the values of the resistors that the gain will be about 40R(12–5) = 280. Notable is the fact that in this way the gain can be very high in theory, by selecting a high power supply voltage. Such a voltage could be obtained from an isolating transformer from the mains. An isolating transformer can be made by connecting the secondaries of two transformers together, which results in a galvanically isolated mains voltage.Circuit diagram:

That means, that with a mains voltage of 240 Veff there will be about 340 V DC after rectification and filtering. If in the amplifier circuit the power supply voltage is now 340 V and the collector voltage is 2 V, then the gain is in theory equal to 40 x (340–2). This is more than 13,500 times! However, there are a few drawbacks in practice. This is related to the output characteristic of the transistor. In practice, it turns out that the transistor does actually have an output resistor between collector and emitter.

This output resistance exists as a transistor parameter and is called ‘hoe’. In normal designs this parameter is of no consequence because it has no noticeable effect if the collector resistor is not large. When powering the amplifier from 340 V and setting the collector current to 1 mA, the collector resistor will have a value of 338 k. Whether the ‘hoe’-parameter has any influence depends in the type of transistor. We also note that with such high gains, the base-collector capacitance in particular will start to play a role.

As a consequence the input frequency may not be too high. For a higher bandwidth we will have to use a transistor with small Cbc, such as a BF494 or perhaps even an SHF transistor such as a BFR91A. We will have to adjust the value of the base resistor to the new hfe. The author has carried out measurements with a BC547B at a power supply voltage of 30 V. A value of 2 V was chosen for the collector voltage. Measurements confirm the rule of thumb. The gain was more than 1,000 times and the effects of ‘hoe’ and the base-collector capacitance were not noticeable because of the now much smaller collector resistor.
Author: Gert Baars
Copyright: Elektor Electronics
Continue reading[...]

PIC 16F88 based 4 digit Up Down counter circuit with explanation

0 comments

This is a 4 digit decimal counter which can operate as a free running counter or in count and hold mode with manual reset. In either mode the counter can be preset to count to a specified value. Clock edge and leading zero suppression can also be configured. The 7-segment display and indicator LEDs are multiplexed. It will drive most common anode 7 segment LEDs. I used four single digit LEDs but a four digit LED module could also be used. In free running mode the overflow output resets on the next clock pulse. Therefore the pulse duration is directly related to the input clock frequency.

Read Source:http://picprojects.org.uk/projects/counter/counter.htm

Continue reading[...]

Flashing LED Battery status Indicator circuit with explanation

0 comments
Signals when an on-circuit battery is exhausted

5V to 12V operating voltage

A Battery-status Indicator circuit can be useful, mainly to monitor portable Test-gear instruments and similar devices.
LED D1 flashes to attire the user’s attention, signaling that the circuit is running, so it will not be left on by mistake. The circuit generates about two LED flashes per second, but the mean current drawing will be about 200µA.
Transistors Q1 and Q2 are wired as an uncommon complementary astable multivibrator: both are off 99% of the time, saturating only when the LED illuminates, thus contributing to keep very low current consumption.

The circuit will work with battery supply voltages in the 5 – 12V range and the LED flashing can be stopped at the desired battery voltage (comprised in the 4.8 – 9V value) by adjusting Trimmer R4. This range can be modified by changing R3 and/or R4 value slightly.
When the battery voltage approaches the exhausting value, the LED flashing frequency will fall suddenly to alert the user. Obviously, when the battery voltage has fallen below this value, the LED will remain permanently off.
To keep stable the exhausting voltage value, diode D1 was added to compensate Q1 Base-Emitter junction changes in temperature. The use of a Schottky-barrier device (e.g. BAT46, 1N5819 and the like) for D1 is mandatory: the circuit will not work if a common silicon diode like the 1N4148 is used in its place.

Parts:
R1,R7__________220R 1/4W Resistors
R2_____________120K 1/4W Resistor
R3_______________5K6 1/4W Resistor
R4_______________5K 1/2W Trimmer Cermet or Carbon
R5______________33K 1/4W Resistor
R6_____________680K 1/4W Resistor
R8_____________100K 1/4W Resistor
R9_____________180R 1/4W Resistor
C1,C2____________4µ7 25V Electrolytic Capacitors
D1____________BAT46 100V 150mA Schottky-barrier Diode
D2______________LED Red 5mm.
Q1____________BC547 45V 100mA NPN Transistor
Q2____________BC557 45V 100mA PNP Transistor
B1_______________5V to 12V Battery supply

Read more Source: http://www.redcircuits.com/Page135.htm

Continue reading[...]

Fuel Tank Pressure Sensor Circuit with explanation

0 comments
The control module monitors the fuel tank pressure (FTP) sensor signal in order to detect vacuum decay and excess vacuum during the enhanced evaporative emission (EVAP) diagnostic. The Fuel Tank Pressure Sensor responds to changes in the fuel tank pressure or vacuum. This information is used in order to detect vacuum decay or an excessive vacuum during EVAP diagnostic routing. The fuel tank pressure sensor signal voltage to the VCM varies from a minimum of about 0.1 volts with pressure in the fuel tank to above 4.0 volts with a high vacuum in the fuel tank.

The following schematic shows the Typical Fuel Tank Pressure Sensor Circuit Diagram.
 fuel tank pressure sensor circuit with explanation

Continue reading[...]

12 Volt 20 Ampere Regulator circuit with explanation

0 comments

A heavy duty 13.8V power supply is a fine thing to have in the shack, but unless you acquire one secondhand, is an expensive little beastie to buy. This means building one should be considered, not only for the cost savings, but also because you can brag about it on air to your mates. Of course, careful consideration must be given to the properties of the completed supply, and after talking to a few of my friends who have built their own and fallen into all the traps, here are the printable ones : RF proof, easy to make, commonly available parts used, but above all CHEAP.

Well, last things first. Breaking down the construction costs of a heavy duty regulated supply, they are in order:

  • The transformer (around $A80)
  • The main filter electrolytics – around $A80
  • The case – a metal case is well beyond the workshop capabilities of many amateurs and is quite expensive to buy (if you can).
  • The meter – around $A20-$27 (either digital or analogue)
  • The electronics – transistors, resistors, diodes, etc.
  • All the bits – fuseholders, terminals, switches, solder tags, nuts and bolts, power cords, etc.
  • Continue reading[...]

    Speed limit Alert circuit Wireless portable unit Adaptable with most internal combustion engine vehicles

    0 comments
    Speed-limit

    Parts:

    R1,R2,R19_______1K 1/4W Resistors
    R3-R6,R13,R17_100K 1/4W Resistors
    R7,R15__________1M 1/4W Resistors
    R8_____________50K 1/2W Trimmer Cermet
    R9____________470R 1/4W Resistor
    R10___________470K 1/4W Resistor
    R11___________100K 1/2W Trimmer Cermet (see notes)
    R12___________220K 1/4W Resistor (see notes)
    R14,R16________68K 1/4W Resistors
    R18____________22K 1/4W Resistor
    R20___________150R 1/4W Resistor (see notes)

    C1,C7_________100µF 25V Electrolytic Capacitors
    C2,C3_________330nF 63V Polyester Capacitors
    C4-C6___________4µ7 25V Electrolytic Capacitors

    D1,D5______Red LEDs 3 or 5mm.
    D2,D3________1N4148 75V 150mA Diodes
    D4________BZX79C7V5 7.5V 500mW Zener Diode

    IC1__________CA3140 or TL061 Op-amp IC
    IC2____________4069 Hex Inverter IC
    IC3____________4098 or 4528 Dual Monostable Multivibrator IC

    Q1,Q2_________BC238 25V 100mA NPN Transistors

    L1_____________10mH miniature Inductor (see notes)

    BZ1___________Piezo sounder (incorporating 3KHz oscillator)

    SW1____________SPST Slider Switch

    B1_______________9V PP3 Battery (see notes)

    Clip for PP3 Battery

    Device purpose:

    This circuit has been designed to alert the vehicle driver that he/she has reached the maximum fixed speed limit (i.e. in a motorway). It eliminates the necessity of looking at the tachometer and to be distracted from driving.
    There is a strict relation between engines RPM and vehicle speed, so this device controls RPM, starting to beep and flashing a LED once per second, when maximum fixed speed is reached.
    Its outstanding feature lies in the fact that no connection is required from circuit to engine.

    Circuit operation:

    IC1 forms a differential amplifier for the electromagnetic pulses generated by the engine sparking-plugs, picked-up by sensor coil L1. IC2A further amplifies the pulses and IC2B to IC2F inverters provide clean pulse squaring. The monostable multivibrator IC3A is used as a frequency discriminator, its pin 6 going firmly high when speed limit (settled by R11) is reached. IC3B, the transistors and associate components provide timings for the signaling part, formed by LED D5 and piezo sounder BZ1. D3 introduces a small amount of hysteresis.

    Notes:

    • D1 is necessary at set-up to monitor the sparking-plugs emission, thus allowing to find easily the best placement for the device on the dashboard or close to it. After the setting is done, D1 & R9 can be omitted or switched-off, with battery savings.
    • During the preceding operation R8 must be adjusted for better results. The best setting of this trimmer is usually obtained when its value lies between 10 and 20K.
    • You must do this first setting when the engine is on but the vehicle is stationary.
    • The final simplest setting can be made with the help of a second person. Drive the vehicle and reach the speed needed. The helper must adjust the trimmer R11 until the device operates the beeper and D5. Reducing vehicles speed the beep must stop.
    • L1 can be a 10mH small inductor usually sold in the form of a tiny rectangular plastic box. If you need an higher sensitivity you can build a special coil, winding 130 to 150 turns of 0.2 mm. enameled wire on a 5 cm. diameter former (e.g. a can). Extract the coil from the former and tape it with insulating tape making thus a stand-alone coil.
    • Current drawing is about 10mA. If you intend to use the car 12V battery, you can connect the device to the lighter socket. In this case R20 must be 330R.
    • Depending on the engines cylinders number, R11 can be unable to set the device properly. In some cases you must use R11=200K and R12=100K or less.
    • If you need to set-up the device on the bench, a sine or square wave variable generator is required.
    • To calculate the frequency relation to RPM in a four strokes engine you can use the following formula:
      Hz= (Number of cylinders * RPM) / 120.
      For a two strokes engine the formula is: Hz= (Number of cylinders * RPM) / 60.
      Thus, for a car with a four strokes engine and four cylinders the resulting frequency @ 3000 RPM is 100Hz.
    • Temporarily disconnect C2 from IC1 pin 6. Connect the generator output across C2 and Ground. Set the generator frequency to e.g. 100Hz and trim R11 until you will hear the beeps and LED D5 will start flashing. Reducing the frequency to 99 or 98 Hz, beeping and flashing must stop.
    • Please note that this circuit is not suited to Diesel engines.
    Continue reading[...]

    20W Car Audio Amplifier with LM1875

    0 comments
    This is just addition 20W audio amplifier circuit , but this time based on the LM1875 audio amplifier IC from National Semiconductors. With a 25V bifold ability accumulation LM1875 can bear 20W of audio ability into a 4 ohm speaker. The LM1875 requires actual beneath external components and has actual low distortion.

    The IC is aswell arranged with a lot acceptable appearance like fast bulk rate, advanced accumulation voltage range, top achievement current, top achievement voltage swing, thermal aegis etc. The IC is accessible in TO-220 artificial ability amalgamation and is able-bodied acceptable for a array of applications like audio systems, servo amplifiers, home theatre systems etc.Notes.
    • Assemble the circuit on a good quality PCB.
    • Use +/-25V DC dual supply for powering the circuit.
    • K1 can be 4 ohm, 20W speaker.
    • A proper heat sink is necessary for the IC.
    • F1 and F2 are 2A 
    Continue reading[...]

    12V Powered 12V Lead Acid Battery Charger with Indicator

    0 comments
    Some of you might wonder why a charger is needed at all, to charge a 12 Volt battery from a 12 Volt source! Well, firstly the "12 Volt" source will typically vary anywhere from 11 Volt to 15 Volt, and then a battery needs a controlled charge current and voltage, which cannot result from connecting it directly to a voltage source. The charger described here is intended for charging small 12 Volt lead acid batteries, such as the gelled or AGM batteries of capacities between about 2 and 10 Ah, using a cars electrical system as power source, regardless of whether the car engine is running or not. I built this charger many years ago, I think I was still in school back then. On request of a reader of my web site, Im publishing it now, despite being a rather crude circuit.12V
    It works, it is uncritical to build, and uses only easy-to-find parts, so it has something in its favor. The downside is mainly the low efficiency: This charger wastes about as much power as it puts into the battery. The charger consists of two stages: The first is a capacitive voltage doubler, which uses a 555 timer IC driving a pair of transistors connected as emitter followers, which in turn drive the voltage doubler proper. The doubler has power resistors built in, which limit the charging current. The second stage is a voltage regulator, using a 7815 regulator IC. Its output is applied to the battery via a diode, which prevents reverse current and also lowers the voltage a bit.12V
    The resulting charge voltage is about 14.4V, which is fine for charging a gelled or AGM battery to full charge, but is too high as a trickle charger, so dont leave this charger permanently connected to a battery. If you would like to do just that, then add a second diode in series with D3! There is a LED connected as a charge indicator. It will light when the charge current is higher than about 150mA. The maximum charge current will be roughly 400mA. There is an auxiliary output, that provides about 20V at no load (depending on input voltage), and comes down as the load increases. I included this for charging 12V, 4Ah NiCd packs, which require just a limited current but not a limited voltage for charging.12V
    Note that if the charge output is short-circuited, the overcurrent protection of U2 will kick in, but the current is still high enough to damage the diodes, if it lasts. So, dont short the output! If instead you short the auxiliary output, the fuse should blow. I built this charger into a little homemade aluminum sheet enclosure, using dead-bug construction style. Not very tidy, but it works. Note the long leads on the power resistors. They are necessary, because with shorter leads the resistors will unsolder themselves, as they get pretty hot! The transistors and the regulator IC are bolted to the case, which serves as heat sink. The transistors dont heat up very much, but the IC does.

    Source: Homo Ludens
    Continue reading[...]

    Low drop Regulator with Indicator

    0 comments
    Even today much logic is still powered from 5 volts and it then seems obvious to power the circuit using a standard regulator from a rectangular 9-V battery. A disadvantage of this approach is that the capacity of a 9-V battery is rather low and the price is rather high. Even the NiMH revolution, which has resulted in considerably higher capacities of (pen-light) batteries, seems to have escaped the 9-V battery generation. It would be cheaper if 5 volts could be derived from 6 volts, for example. That would be 4 ‘normal’ cells or 5 NiMH- cells. Also the ‘old fashioned’ sealed lead- acid battery would be appropriate, or two lithium cells.
     
    Circuit diagram : 
    Low-drop Regulator with Indicator Circuit Diagram
     
    Using an LP2951, such a power supply is easily realised. The LP2951 is an ever- green from National Semiconductor, which you will have encountered in numerous  Elektor Electronics designs already. This IC can deliver a maximum current of 100 mA at an input voltage of greater than 5.4 V. In addition to this particular version, there are also versions available for 3.3 and 3 V output, as well as an adjustable version.  In this design we have added a battery indicator, which also protects the battery from too deep a discharge. As soon as the IC has a problem with too low an input voltage, the ERROR output will go low and the regulator is turned off via IC2d, until a manual restart is provided with the RESET pushbutton.
     
    The battery voltage is divided with a few resistors and compared with the reference voltage (1.23 V) of the regulator IC. To adapt the indicator for different voltages you only need to change the 100-k resistor. The comparator is an LP339. This is an energy-friendly version of the LM339. The LP339 consumes only 60 µA and can sink 30 mA at its output. You can also use the LM339, if you happen to have one around, but the current consumption in that case is 14 times higher (which, for that matter, is still less than 1 mA).
     
    Finally, the LP2951 in the idle state, consumes about 100 µA and depend- ing on the output current to be deliv- ered, a little more.
    Continue reading[...]

    Schematic diagram for the One Transistor FM Radio with Improved Audio Gain

    0 comments
    Schematic diagram for the One Transistor FM Radio with Improved Audio Gain
    One Transistor FM Radio with improved audio gain.
    Some wiring notes:
    Unless you have experience with super-regenerative radios, I highly recommend using the FAR Circuits printed circuit board.

    Connect the two sections of the variable capacitor (C3) in series to linearize the tuning somewhat. That is, use the connections on either end of C3 and dont use the middle lead.
    L2, the RF choke should not be near a ground. The same is true for L1. Capacitance to ground will disturb the feedback.

    The gain is just enough to drive an earphone. If you live too far away from radio stations, you might have trouble hearing one. There is no option here for an external antenna (that would require and extra transistor).

    You can drive a speaker if you add an external audio amplifier.
    If you want a little more audio gain, or you cannot locate a TL431CLP chip, you can use some other audio amplifier in the circuit where pins 1 and 2 of D1 normally connect. You can use an LM386 or a TDA7052 audio amplifier. Quasar DIY project kit #3027 is a complete TDA7052 audio amplifier kit and it works fine in this application. 
    Continue reading[...]
    Blog host by Blogger.com & | Supported by you