12 volt diode bridge circuit - instructions and assembly

Power supplies for radio and electrical equipment almost always use rectifiers designed to convert alternating current to direct current. This is due to the fact that almost all electronic circuits and many other devices must be powered from DC sources. A rectifier can be any element with a nonlinear current-voltage characteristic, in other words, passing current differently in opposite directions. In modern devices, planar semiconductor diodes are usually used as such elements.

Planar semiconductor diodes

Along with good conductors and insulators, there are many substances that occupy an intermediate position in conductivity between these two classes. Such substances are called semiconductors. The resistance of a pure semiconductor decreases with increasing temperature, unlike metals, whose resistance increases under these conditions.

By adding a small amount of impurity to a pure semiconductor, its conductivity can be significantly changed. There are two classes of such impurities:

Figure 1. Planar diode: a. diode device, b. designation of a diode in electrical circuits, c. appearance of planar diodes of various powers.

The layer at the interface of p- and n-type semiconductors (pn junction) has one-way conductivity? conducts current well in one (forward) direction and very poorly in the opposite (reverse) direction. The structure of a planar diode is shown in Figure 1a. The basis ? a semiconductor plate (germanium) with a small amount of donor impurity (n-type), on which a piece of indium, which is an acceptor impurity, is placed.

Once heated, indium diffuses into the adjacent regions of the semiconductor, converting them into a p-type semiconductor. A pn junction occurs at the boundary of regions with two types of conductivity. The terminal connected to the p-type semiconductor is called the anode of the resulting diode, the opposite? its cathode. An image of a semiconductor diode on circuit diagrams is shown in Fig. 1b, appearance of planar diodes of various powers? in Fig. 1st century

The simplest rectifier

Figure 2. Current characteristics in various circuits.

The current flowing in a conventional lighting network is variable. Its magnitude and direction change 50 times within one second. A graph of its voltage versus time is shown in Fig. 2a. Positive half-cycles are shown in red, ? negative.

Since the current value varies from zero to the maximum (amplitude) value, the concept of the effective value of current and voltage is introduced. For example, in a lighting network the effective voltage value is 220 V? in a heating device connected to this network, the same amount of heat is generated over equal periods of time as in the same device in a 220 V DC circuit.

But in fact, the network voltage changes in 0.02 s as follows:

the first quarter of this time (period)? increases from 0 to 311 V,
second quarter of the period? decreases from 311 V to 0,
third quarter of the period? decreases from 0 to 311 V,
last quarter of the period? increases from 311 V to 0.

In this case, 311 V? voltage amplitude Uо. The amplitude and effective (U) voltages are related to each other by the formula:

When a series-connected diode (VD) and load are connected to an alternating current circuit (Fig. 2b), current flows through it only during positive half-cycles (Fig. 2c). This happens due to the one-way conductivity of the diode. Is such a rectifier called half-wave? During one half of the period there is current in the circuit, during the second? absent.

The current flowing through the load in such a rectifier is not constant, but pulsating. You can turn it almost constant by connecting a filter capacitor Cf of a sufficiently large capacity in parallel with the load. During the first quarter of the period, the capacitor is charged to the amplitude value, and in the intervals between pulsations it is discharged to the load. The tension becomes almost constant. The greater the capacitor capacity, the stronger the smoothing effect.

Diode bridge circuit

More advanced is the full-wave rectification circuit, when both positive and negative half-cycles are used. There are several varieties of such schemes, but the most commonly used is pavement. The diode bridge circuit is shown in Fig. 3c. The red line on it shows how current flows through the load during positive times, and the blue line? negative half-cycles.

Figure 4. 12 volt rectifier circuit using a diode bridge.

In both the first and second half of the period, the current through the load flows in the same direction (Fig. 3b). The amount of pulsation within one second is not 50, as with half-wave rectification, but 100. Accordingly, with the same filter capacitor capacity, the smoothing effect will be more pronounced.

As you can see, to build a diode bridge you need 4 diodes? VD1-VD4. Previously, diode bridges on circuit diagrams were depicted exactly as in Fig. 3c. The image shown in Fig. 1 is now generally accepted. 3g. Although there is only one picture of a diode, it should not be forgotten that the bridge consists of four diodes.

The bridge circuit is most often assembled from individual diodes, but sometimes monolithic diode assemblies are also used. They are easier to mount on the board, but if one arm of the bridge fails, the entire assembly is replaced. The diodes from which the bridge is mounted are selected based on the amount of current flowing through them and the amount of permissible reverse voltage. This data can be obtained from diode instructions or reference books.

The complete circuit of a 12 volt rectifier using a diode bridge is shown in Fig. 4. T1? step-down transformer, the secondary winding of which provides a voltage of 10-12 V. Fuse FU1? This is a useful detail from a safety point of view and should not be neglected. The brand of diodes VD1-VD4, as already mentioned, is determined by the amount of current that will be consumed from the rectifier. Capacitor C1? electrolytic, with a capacity of 1000.0 μF or higher for a voltage of at least 16 V.

Output voltage? fixed, its value depends on the load. The higher the current, the lower the voltage. To obtain a regulated and stable output voltage, a more complex circuit is required. Obtain the regulated voltage from the circuit shown in Fig. 4 can be done in two ways:

It is hoped that the descriptions and diagrams given above will provide practical assistance in assembling a simple rectifier for practical needs.

There is an inconsistency in electrical engineering. On the one hand, it is more convenient to transmit energy over long distances if it is in the form of alternating voltage. On the other hand, direct current is required to power smartphones, LEDs in light bulbs, circuit boards in TVs and similar household appliances. This problem is successfully solved by a family of radio components such as rectifier diodes.

Principle of operation

Let's start with the fact that the laboratory power supply uses a transformer with a secondary winding of 24V/3A, which is connected through input terminals 1 and 2 (the quality of the output signal is proportional to the quality of the transformer). The AC voltage from the secondary winding of the transformer is rectified by a diode bridge formed by diodes D1-D4. The ripples of the rectified DC voltage at the output of the diode bridge are smoothed by a filter formed by resistor R1 and capacitor C1. The circuit has some features that make this power supply different from other units in its class.

Instead of using feedback to control the output voltage, our circuit uses an op-amp to provide the required voltage for stable operation. This voltage drops at the output of U1. The circuit operates thanks to the D8 - 5.6 V Zener diode, which here operates at zero temperature coefficient of current. The voltage at the output of U1 drops across the diode D8 turning it on. When this happens, the circuit stabilizes and the voltage of the diode (5.6) drops across resistor R5.

The current that flows through the opera. the amplifier changes slightly, which means the same current will flow through resistors R5, R6, and since both resistors have the same voltage value, the total voltage will be summed up as if they were connected in series. Thus, the voltage obtained at the output of the opera. amplifier will be equal to 11.2 volts. Chain from oper. amplifier U2 has a constant gain of approximately 3, according to the formula A = (R11 + R12) / R11 increases the voltage of 11.2 volts to approximately 33 volts. Trimmer RV1 and resistor R10 are used to set the voltage output so that it does not drop to 0 volts, regardless of the value of other components in the circuit.

Another very important characteristic of the circuit is the ability to obtain the maximum output current that can be obtained from the psu. To make this possible, the voltage drops across the resistor (R7), which is connected in series with the load. The IC responsible for this circuit function is U3. An inverted signal to input U3 equal to 0 volts is supplied through R21. At the same time, without changing the signal of the same IC, you can set any voltage value through P2. Let's say that for a given output the voltage is several volts, P2 is set so that there is a signal of 1 volt at the input of IC. If the load is amplified, the output voltage will be constant and the presence of R7 in series with the output will have little effect due to its low magnitude and due to its position outside the feedback loop of the control circuit. As long as the load and output voltage are constant, the circuit operates stably. If the load is increased so that the voltage on R7 is greater than 1 volt, U3 is turned on and stabilizes to its original parameters. U3 operates without changing the signal to U2 through D9. Thus, the voltage through R7 is constant and does not increase above a predetermined value (1 volt in our example), reducing the output voltage of the circuit. This device is capable of maintaining the output signal constant and accurate, which makes it possible to obtain 2 mA at the output.

Capacitor C8 makes the circuit more stable. Q3 is needed to control the LED whenever you use the limiter indicator. To make this possible for U2 (changing the output voltage down to 0 volts) it is necessary to provide a negative connection, which is done through the circuit C2 and C3. The same negative connection is used for U3. Negative voltage is supplied and stabilized by R3 and D7.

To avoid uncontrollable situations, there is a kind of protection circuit built around Q1. The IC is internally protected and cannot be damaged.

U1 is a reference voltage source, U2 is a voltage regulator, U3 is a current stabilizer.

What are diodes

A diode is a semiconductor element based on a silicon crystal. Previously, these parts were also made of germanium, but over time this material was forced out due to its shortcomings. The electrical diode functions as a valve, i.e. it allows current to flow in one direction and blocks it in the other. Such capabilities are built into this part at the level of the atomic structure of its semiconductor crystals.

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One diode cannot obtain a full constant voltage from an alternating voltage. Therefore, in practice, more complex combinations of these elements are used. An assembly of 4 or 6 parts, combined according to a special circuit, forms a diode bridge. He is already quite capable of coping with full current rectification.

Interesting. Diodes have parasitic sensitivity to temperature and light. Transparent rectifiers in a glass case can be used as light sensors. Germanium diodes (approx. D9B) are suitable as a temperature-sensitive element. Actually, due to the strong dependence of the properties of these elements on temperature, they stopped producing them.

How to make a gas water heater ignition block with your own hands

Buying a ready-made block is not the most expensive investment, but it pays off over time. However, if you want to spend a minimum of money on such a modification, you can make a power supply yourself.

This process, although it seems complicated, does not take that much time. And the money spent on purchasing materials for such a product will pay off within a year.

To make a power supply for a speaker with your own hands, you need to know how to solder. If this is your first soldering experience, we advise you to first practice on some product that is not so expensive, like a gas water heater. Once you are sure that you have acquired the soldering skill, you can get to work.

To make a gas water heater ignition unit, you need to have relevant experience

First of all, you will need to purchase a power supply with suitable parameters. The best option is considered to be an electrical unit with characteristics of 220V/3V/500MA. Next, you need two female-male connectors. You can purchase all the necessary materials at an electronics store. In addition to materials, you will need some tools, namely a soldering iron and soldering materials, a construction knife, and electrical tape.

How to make a power supply for a geyser yourself:

From the battery compartment in the column, remove the two wires from the connectors and lead them down from the device. These connectors usually have female halves.
Determine which of the two wires is responsible for the plus and which for the minus. Mark the wires with a marker.
Cut off the plug from the power supply. Solder the male connectors to the wires that appear.
Connect the mother speakers to the power supply men.
Connect the speaker's power supply to the mains.

Just like that, you can replace the batteries in a gas water heater with a power supply. This modification will allow you to use electric ignition without changing batteries.

Single-phase and three-phase diode bridge

There are two main types of straightening assemblies:

Single-phase bridge. Most often used in household electrical appliances. Has 4 outputs. Two of them are supplied with alternating voltage, i.e. phase (L) and zero (N). The permanent one is removed from the remaining two, i.e. plus (+) and minus (-).
Three-phase bridge. It is found in powerful industrial installations and equipment powered by a 380 volt network. Three phases are supplied to its input (L1, L2, L3). The constant voltage is also removed from the output. Such bridges are distinguished by their large size and impressive currents that they are capable of passing through themselves.

Operating principle of a diode bridge

You can understand how a bridge performs its task by understanding how a separate diode behaves. Initially there are only two wires with alternating voltage (L and N). It has the shape of a sinusoid (Fig. a). If you add one diode to the circuit, then it will transmit only the positive half-wave (Fig. b), if this component is deployed, then the negative component (Fig. c). This voltage will no longer be variable. However, it is not suitable for powering serious electrical appliances. There are moments in it when there is no current at all. The use of four diodes will allow you to obtain a constant voltage without any interruptions (Fig. d). Three-phase bridges are straightened using the same method. However, they do this with three sine waves at the same time.

Rectifier

The voltage obtained after the diode bridge has the shape of a sinusoid, in which the negative component is reflected relative to the time axis. In simple terms, it is shaped like hills and is called pulsating. This voltage is positive. Does not contain moments when current does not flow. But it is still unstable. For example, at point “a” it is early 0 volts, and at “b” it has a maximum value. This rectifier cannot be considered complete.

To solve this problem, a smoothing electrolytic capacitor is required. On the board it is usually located in the same place as the diode assembly. The capacitance accumulates energy at those moments when it has peak values (point b), and releases it at moments of dips (a). The output is a straight line - full-fledged direct current, suitable for powering subsequent electronic components, processors, microcircuits, etc.

The advantage of a power supply as an analogue of batteries

Installing a geyser is an excellent prospect for switching to the method of individual water heating. In addition, this allows you to significantly save on utility bills. Installing a gas flow-through heater makes you independent from the boiler house and water utility and allows you to get hot water at any time. Thus, regular shutdowns of hot water due to summer maintenance work will no longer be a problem.

Batteries for a 1.5 V instantaneous gas water heater Source sat-oskol.ru

Disadvantages of a full bridge

A full-fledged full-wave bridge has disadvantages:

The current is forced to flow not through one diode, but through two at once, connected in series. Therefore, the voltage drop across the rectifier element doubles. For low-power bridges on silicon diodes it can reach 2 volts. In powerful rectifiers - about 10 V. Hence, significant power losses on the rectifying element and its increased heating.
If one or four diodes fail, the bridge continues to operate. This defect may not be noticeable without special measurements. However, it creates the risk of more serious damage to the device, which is powered through a faulty bridge.

Design

The circuit of any rectifier bridge includes diodes. They can be separately soldered onto a printed circuit board or located in the same housing. Regarding the size, rectifiers are miniature, for example, imported MB6S or Soviet KTs405A. The latter are popularly called “ka-tseshki” or “chocolates”.

There are samples with impressive dimensions. For example, a three-phase rectifier bridge made in China. The device is designed for currents of hundreds of amperes, therefore it has screw fastening for power wires and a flat metal heat-conducting surface with holes for fixing on the cooling radiator.

Transformer

The transformer consists of a core made of a ferromagnetic material, as well as primary and secondary windings. 220 volts comes to the primary winding, and in this case, 12 are removed from the secondary winding, going to the rectifier. The cores in this type of power supply are mostly made in W- and U-shapes.

The arrangement of the windings is allowed either one on top of the other on a common coil, or separately. For example, a U-shaped core has a pair of coils, each of which has half of the windings wound on it. When connecting a transformer, the terminals are connected in series.

Rectifier markings

There are no generally accepted rules according to which manufacturers label their diode bridges. Everyone has the right to name their product as they see fit, i.e. according to its own nomenclature.

However, most of these parts have similar features that help visually determine the purpose of their pins. In the photo of a three-phase bridge (see above), the alternating current symbol is highlighted separately - a wavy line. It indicates that a sinusoidal input voltage is connected to this pin. Also on some bridge models, the input terminals are marked with the letters AC (Alternative Current), indicating alternating current. In this case, the output contacts from which direct current is removed are indicated by the symbols DC (Direct Current) or the traditional “+” and “-”. Additionally, on some rectifiers, one of the corners is “filed” on the plus side. An extended pin can also indicate “+”. This type of marking is common to many electronic components and is called a key.

How to connect a power supply for a geyser

The process of creating a power supply is not as simple as you might think. Therefore, if you are not confident in your abilities, you can purchase a ready-made block in an online store.

At the moment, the choice of such devices is very large. There are products from domestic companies, models from foreign manufacturers, and Chinese electrical goods. Of course, the last option from China is the most economical in terms of purchase, but it is not a fact that such a power supply will work for you for a long time.

To connect the power supply for a gas water heater, you need to do everything according to the instructions

If you decide to purchase a ready-made 3-volt power supply instead of batteries, you need to understand how to connect it correctly. This is a completely simple task that you can handle even if you have no experience in electrical work.

How to connect a power supply to a geyser instead of batteries:

Remove the battery compartment from the speaker. It usually snaps right into your hand very easily.
Connect the terminals of the block with the terminals of the battery box. It is very important to maintain the polarity of the contacts.
Plug in the power supply. Use the column as before.

As you can see, the method of replacing batteries with a ready-made unit is very simple. The main thing here is to follow the instructions exactly and carefully follow all its points.

DIY diode bridge

To assemble the rectifier yourself, you will need 4 diodes of the same type. At the same time, they must be suitable in terms of reverse voltage, maximum current and operating frequency. Connections must be made in accordance with the diagram below. A positive voltage is removed between the two cathodes and a negative voltage between the anodes. An alternating voltage source is connected to the points at which opposite terminals of the diodes are connected. The entire circuit can be soldered by surface mounting in a couple of minutes, or you can work hard and make it in the form of a small printed circuit board.

Additional Information. The reverse voltages of diodes connected in a series circuit are added to each other.

Transformerless power supply for LEDs

The essence of such a unit is to use a ballast (quenching) capacitor. On our website there is a detailed article about such a power supply, in which you can find a calculator for calculating the capacitor. In general, the scheme looks like this:

This option has a lot of disadvantages:

No output voltage stabilization;
no galvanic isolation (transformer);
There is no discharge resistor on the ballast capacitor, so there is a risk of electric shock from C1.

Having accepted these shortcomings and modified the circuit, we get the following transformerless power supply for 12V LEDs.

Instead of D1, the L7812 linear stabilizer microcircuit, any other one can be installed at the required voltage (7805, etc., as well as domestic KREN stabilizers).

An alternative version of the power supply circuit for an LED strip, when assembling it yourself, is to use a zener diode or a parametric stabilizer made of a zener diode and a transistor instead of a linear stabilizer. The advantage of this solution is the flexibility in setting the stabilization voltage, because if you do not have a suitable zener diode, you can connect the other two in series and achieve the desired voltage value.

To make a homemade power supply for an LED strip, a domestic zener diode of the D818D series, designed for a voltage of about 12-13 V, is suitable.

Another way of stabilization is to assemble a current stabilizer using two transistors. The stabilization current is set by resistor R2.

R2 = 0.7 * Ist; R1 = 3.9 kOhm.

The current stabilizer strives to produce a given current; this is the best option for transformerless power supply of individual LEDs.

Selecting a build type

For each task there is its own optimal version of the rectifier diode assembly. All of them can be divided into 3 types:

Rectifier with one diode. It is used in the simplest and cheapest circuits where there is no c.l. requirements for the quality of the output voltage, as, for example, in night lights.
Dual diode. These parts look similar to transistors, because they are produced in the same packages. They also have 3 pins. Essentially, these are two diodes placed in one housing. One of the conclusions is average. It can be the common cathode or the anode of the internal diodes.
Full diode bridge. 4 parts in one case. Suitable for devices with high currents. It is mainly used on the inputs and outputs of various power supplies and chargers.

Additional Information. Rectifiers are also used in cars. They are needed to convert the alternating voltage coming from the generator to direct voltage. This, in turn, is necessary to charge the battery. A conventional gas generator produces alternating current.

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Do I need a stabilizer?

After the parameters of the power supply have been determined, the availability of its stabilized and unstabilized voltage should be considered. The solution to this issue is relevant due to the fact that the network supplying a gas instantaneous water heater must have a stable voltage, without jumps in one direction or another.

Power supply with stabilizer Source oboiman.ru

Important! If there is no suitable power supply and you have to buy one, you can provide for this nuance already at the stage of selecting an adapter. There are models that stabilize the voltage or supply it as received.

The operation of the geyser involves receiving electrical power from batteries. The latter, in turn, (provided they are well charged) are a source of high-quality current and do not require additional stabilizing devices. Manipulations to change the element that powers the heater and does not have a stabilization unit; the piezoelectric element may not operate stably.

Structural elements of a gas flow-through heater Source turbo-yandex-ru.

Checking elements

In most cases, it is not necessary to unsolder the bridge from the board for testing. It should be tested in the same way as a 4 pn junction with a diode bridge connection. This measurement is so common that its capability is implemented in any multimeter. The test device must be switched to diode continuity mode.

The forward voltage drop across a working rectifier diode is 500-700 mV. Otherwise, the device will display “1”. A burnt part most often shows “0” in both directions, i.e. short circuit. Less often, a complete breakage of the element occurs (also in both directions). All measurements should be repeated for each diode included in the bridge. Total 8 measurements, i.e. 4 in forward direction and 4 in reverse. If a Schottky diode is tested, then this parameter is 200-400 mV.

Using the Schottky barrier

The use of a Schottky diode is justified in two cases. Firstly, when you need to rectify high-frequency current. The Schottky barrier is ideal for such a task, because it has a low junction capacitance and, accordingly, is fast-acting. Secondly, when it is necessary to rectify a large current of tens or hundreds of amperes. In this case, the part performs well due to the low voltage drop and low heat generation.

Diode bridges in the world of electronics play the role of a matching element. With their help, you can connect devices that require direct current to a network of alternating voltage convenient for transmission. There are a lot of such devices in everyday life; they are extremely important for a person’s comfortable life.

The main element used to create a rectifier unit is a diode. Its operation is based on the electron-hole transition (pn).

The generally accepted definition says: a pn junction is a region of space located at the boundary of the junction of two semiconductors of different types. In this space, an n-type to p-type transition is formed. The value of conductivity depends on the atomic structure of the material, namely on how tightly the atoms hold electrons. Atoms in semiconductors are arranged in a lattice, and electrons are bound to them by electrochemical forces. This material itself is a dielectric. It either conducts current poorly or does not conduct it at all. But if atoms of certain elements are added to the lattice (doping), the physical properties of such a material change radically.

Mixed atoms begin to form, depending on their nature, free electrons or holes. The resulting excess electrons form a negative charge, and the holes form a positive charge.

An excess charge of one sign causes carriers to repel each other, while an area with an opposite charge tends to attract them towards itself. An electron, moving, occupies a free space, a hole. At the same time, a hole also forms in its old place. As a result, two flows of charge movement are created: one main and the other reverse. A material with a negative charge uses electrons as majority carriers and is called an n-type semiconductor, while a material with a positive charge using holes is called a p-type semiconductor. In both types of semiconductors, minority charges generate a current opposite to the movement of the main charges.

In radio electronics, germanium and silicon are used from materials to create pn junctions. When crystals of these substances are doped, a semiconductor with different conductivity is formed. For example, the introduction of boron leads to the appearance of free holes and the formation of p-type conductivity. Adding phosphorus, on the other hand, will create electrons and the semiconductor will become n-type.

Diode operating principle

A diode is a semiconductor device that has low resistance to current in one direction and prevents it from flowing in the opposite direction. Physically, the diode consists of one pn junction. Structurally, it is an element containing two outputs. The terminal connected to the p-region is called the anode, and the terminal connected to the n-region is called the cathode.

When a diode operates, there are three states:

A forward potential is a signal when the positive pole of the power source is connected to the p-type region of the semiconductor, in other words, the polarity of the external voltage coincides with the polarity of the main carriers. With reverse potential, the negative pole is connected to the p-region and the positive pole to the n region.

There is a potential barrier in the area where the n- and p-type material joins. It is formed by a contact potential difference and is in a balanced state. The height of the barrier does not exceed tenths of a volt and prevents the movement of charge carriers deep into the material.

If direct voltage is connected to the device, then the magnitude of the potential barrier decreases and it practically does not resist the flow of current. Its value increases and depends only on the resistance of the p- and n-regions. When a reverse potential is applied, the barrier value increases, since electrons leave the n-region and holes leave the p-region. The layers become depleted and the barrier's resistance to the passage of current increases.

The main indicator of an element is the current-voltage characteristic. It shows the relationship between the potential applied to it and the current flowing through it. This characteristic is presented in the form of a graph, which indicates the forward and reverse current.

Physical processes

The operating principle of a diode bridge is based on the ability of a pn junction to pass current in only one direction. A pn junction is understood as a contact between two semiconductors with different types of conductivity. The boundary separating the regions is characterized by the width of the forbidden zone, which prevents the passage of charges. On one side there is the p region, in which the main carriers are holes (positive charge), and on the other, the n region, where the majority carriers are electrons (negative charge).

Being isolated from each other, in each region the elementary particles perform random thermal vibrations, due to which their released energy is compensated and the resulting current is zero. When these areas come into contact, diffusion currents arise due to the attraction of charges to each other. As a result, the particles collide and recombine (disappear). In the contact zone, carriers become depleted and their movement stops. A state of dynamic equilibrium is established.

When an electric field is applied to the pn junction, the picture changes. With forward bias, that is, when the positive pole of the power source is connected to the p region, and the negative pole to the n region, the main carriers are introduced into the region. Because of this, the bandgap width decreases, and particles freely begin to pass through the barrier, forming a current. If the polarity of the power source is changed, then even greater depletion of the layers will occur, as a result, the barrier will increase, and the current will not arise.

Thus, depending on the polarity of the signal applied to the junction, the band gap increases or decreases. If an alternating signal is applied to an element whose operation is based on a pn junction, then as a result, forward and reverse voltage will be alternately applied to it. Accordingly, it will delay part of the signal and transmit part of it.

If you take a measuring device that can show the waveform (oscilloscope), then at the output of the radio element you can see pulses, the duration of which is determined by the half-wave period. That is why the diode is called a rectifier, although the name pulse converter is more suitable for it. That is, a device that converts an alternating signal into a burst of pulses.

It’s also important to know: 3 nuances about operation

The homemade product differs somewhat in its method of operation from the factory version. This is explained by the fact that the purchased unit has built-in functions that help with operation. They are difficult to install on a device assembled at home, and therefore you will have to adhere to several rules during operation.

A self-assembled charger will not turn off when the battery is fully charged. That is why it is necessary to periodically monitor the equipment and connect a multimeter to it to monitor the charge.
You need to be very careful not to confuse “plus” and “minus”, otherwise the charger will burn out.
The equipment must be turned off when connecting to the charger.

By following these simple rules, you will be able to properly recharge the battery and avoid unpleasant consequences.

Simple rectifier circuit

Sinusoidal voltage is a periodic signal that varies over time. From a mathematical point of view, it is described by a function in which the origin corresponds to time equal to zero. The signal consists of two half-waves. The half-wave located in the upper part of the coordinates relative to zero is called a positive half-cycle, and in the lower part - negative.

When an alternating voltage is applied to the diode through a load connected to its terminals, current begins to flow. This current is due to the fact that at the moment the positive half-cycle of the input signal arrives, the diode opens. In this case, a positive potential is applied to the anode and a negative potential to the cathode. When the wave changes to a negative half-cycle, the diode is turned off, as the polarity of the signal at its terminals changes.

Thus, it turns out that the diode, as it were, cuts off the negative half-wave, without passing it to the load, and a pulsating current of only one polarity appears on it. Depending on the frequency of the applied voltage, and for industrial networks it is 50 Hz, the distance between the pulses also changes. This type of current is called rectified, and the process itself is called half-wave rectification.

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By rectifying the signal using a single diode, you can power a load that does not have special requirements for voltage quality. For example, a filament. But if you power up, for example, a receiver, a low-frequency hum will appear, the source of which will be the gap that occurs between the pulses. To some extent, to get rid of the disadvantages of half-wave rectification, a capacitor connected in parallel with the load is used together with a diode. This capacitor will charge when pulses arrive and discharge when there are no pulses to the load. This means that the larger the capacitance value of the capacitor, the smoother the current across the load will be.

But the highest signal quality can be achieved if two half-waves are used simultaneously for rectification. The device that allows this to be realized is called a diode bridge, or in other words, a rectifier bridge.

Setting the output voltage and charging current

There are two trimming resistors installed on the DC-DC converter board, one allows you to set the maximum output voltage, the other allows you to set the maximum charging current.

Plug in the charger (nothing is connected to the output wires), the indicator will show the voltage at the device output and the current is zero. Use the voltage potentiometer to set the output to 5 volts. Close the output wires together, use the current potentiometer to set the short circuit current to 6 A. Then eliminate the short circuit by disconnecting the output wires and use the voltage potentiometer to set the output to 14.5 volts.

24 V DC voltage stabilizer

In the wide field of radio-electronic devices, the KR 142 EN 9B microcircuit as a stabilizer with three terminals with a constant voltage of 24 V can be used to connect logic circuits, as well as measuring instruments, audio devices with high-quality playback.

External elements can be used to speed up transition processes. An input capacitor is needed only in cases where the regulator is located at a distance of no more than five centimeters from the capacitor, which acts as a power supply filter.

Main technical parameters:

Internal fault current limiter.
Transistor output protection.
Internal thermal protection.
No need for external elements.
Allowable output current 1 ampere.

Entrance.
Grounding.
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Diode bridge

Such a device is an electrical device used to convert alternating current into direct current. The phrase “diode bridge” is formed from the word “diode”, which implies the use of diodes in it. The diode bridge rectifier circuit depends on the AC network to which it is connected. The network can be:

Depending on this, the rectifier bridge is called a Graetz bridge or a Larionov rectifier. In the first case, four diodes are used, and in the second, the device is assembled using six.

The first rectifier circuit was assembled using radio tubes and was considered a complex and expensive solution. But with the development of semiconductor technology, the diode bridge has completely replaced alternative methods of signal rectification. Selenium pillars are rarely used instead of diodes.

Device designs and characteristics

Structurally, the rectifier bridge is made of a set of individual diodes or a cast housing with four terminals. The body can be flat or cylindrical. According to the accepted standard, icons on the device body mark the terminals for connecting alternating voltage and the output constant signal. Rectifiers with a housing with a hole are designed for mounting on a radiator. The main characteristics of the rectifier bridge are:

Highest forward voltage . This is the maximum value at which the device parameters do not go beyond the permissible limits.
Highest permissible reverse voltage . This is the maximum pulse voltage at which the bridge operates for a long time and reliably.
Maximum operating rectification current . Indicates the average current flowing through the bridge.
Maximum frequency . The frequency of voltage supplied to the bridge at which the device operates efficiently and does not exceed the permissible heating.

Exceeding the rectifier's characteristics leads to a sharp reduction in its service life or breakdown of pn junctions. It should be noted that all diode parameters are indicated for an ambient temperature of 20 degrees. The disadvantages of using a bridge rectification circuit include a higher voltage drop compared to a half-wave circuit and a lower efficiency value. To reduce losses and reduce heating, bridges are often made using fast Schottky diodes.

Device connection diagram

On electrical circuits and printed circuit boards, a diode rectifier is indicated by a diode icon or in Latin letters. If the rectifier is assembled from individual diodes, then next to each is placed the designation VD and a number indicating the serial number of the diode in the circuit. VDS or BD labels are rarely used.

The diode rectifier can be connected directly to a 220 volt network or after a step-down transformer, but its connection circuit remains unchanged.

When a signal arrives in each half-cycle, current will only be able to flow through its own pair of diodes, and the opposite pair will be blocked for it. For a positive half-cycle, VD2 and VD3 will be open, and for a negative half-cycle, VD1 and VD4. As a result, the output will be a constant signal, but its pulsation frequency will be doubled. In order to reduce the ripple of the output signal, a parallel connection of capacitor C1 is used, as in the case of one diode. Such a capacitor is also called a smoothing capacitor.

But it happens that the diode bridge is placed not only in an alternating network, but is also connected to an already rectified one. Why a diode bridge is needed in such a circuit will become clear if you pay attention to which circuits use such a connection. These circuits involve the use of radioelements that are sensitive to power reversal. Using a bridge allows for simple but effective foolproof protection. In case of incorrect connection of the power polarity, the radio elements installed behind the bridge will not fail.

Functionality check

This type of electronic device can be checked without desoldering it from the circuit, since no shunting is used in the device designs. In the case of a rectifier assembled from diodes, each diode is checked separately. And in the case of a monolithic case, measurements are carried out on all four of its terminals.

The essence of the test comes down to checking the diodes for a short circuit with a multimeter. To do this, perform the following steps:

The multimeter switches to diode or resistance vertebrae mode.
The plug of one wire (black) is inserted into the common socket of the tester, and the second (red) into the resistance test socket.
With the probe connected to the black wire, touch the first leg, and with the probe of the red wire, touch the third pin. The tester should show infinity, and if you change the polarity of the wires, the multimeter will show the transition resistance.
The minus of the tester is fed to the fourth leg, and the plus to the third. The multimeter will show resistance; when changing polarity, infinity.
Minus on the first leg, plus on the second. The tester will show an open transition, and when changing, a closed one.

Such tester readings indicate the serviceability of the rectifier. If you don't have a multimeter, you can use a regular voltmeter. But in this case you will have to supply power to the circuit and measure the voltage on the smoothing capacitor. Its value should exceed the input value by 1.4 times.

List of elements.

R1 = 2.2 kOhm 1W R2 = 82 Ohm 1/4W R3 = 220 Ohm 1/4W R4 = 4.7 kOhm 1/4W R5, R6, R13, R20, R21 = 10 kOhm 1/4W R7 = 0.47 Ohm 5W R8, R11 = 27 kOhm 1/4W R9, R19 = 2.2 kOhm 1/4W R10 = 270 kOhm 1/4W R12, R18 = 56 kOhm 1/4W R14 = 1.5 kOhm 1/4W R15, R16 = 1 kOhm 1/4W R17 = 33 Ohm 1/4W R22 = 3.9 kOhm 1/4W RV1 = 100K trimmer P1, P2 = 10KOhm linear potentiometer C1 = 3300 uF/50V electrolytic C2, C3 = 47uF/50V electrolytic C4 = 100nF polyester C5 = 200nF polyester C6 = 100pF ceramic C7 = 10uF/50V electrolytic C8 = 330pF ceramic C9 = 100pF ceramic D1, D2, D3, D4 = 1N5402,3,4 diode 2A - RAX GI837U D5, D6 = 1N4148 D7, D8 = 5.6V Zener D9, D10 = 1N4148 D11 = 1N4001 diode 1A Q1 = BC548, NPN transistor or BC547 Q2 = 2N2219 NPN transistor - (Replace with KT961A - everything works) Q3 = BC557, PNP transistor or BC327 Q4 = 2N3055 NPN power transistor ( replace with KT 827A ) U1, U2, U3 = TL081, op. amplifier D12 = LED diode

As a result, I assembled a laboratory power supply myself, but in practice I encountered something that I considered necessary to correct. Well, firstly, this is the power transistor Q4 = 2N3055 ; it must be urgently crossed out and forgotten. I don’t know about other devices, but it is not suitable for this regulated power supply. The fact is that this type of transistor fails instantly if there is a short circuit and the current of 3 amperes does not draw at all!!! I didn’t know what was wrong until I exchanged it for our native Soviet KT 827 A. After installing it on the radiator, I didn’t know any grief and never returned to this issue.

As for the rest of the circuitry and parts, there are no difficulties. With the exception of the transformer, we had to wind it. Well, this is purely out of greed, half a bucket of them is in the corner - don’t buy it =))

Well, in order not to break the good old tradition, I post the result of my work to the general court

Practical circuit of a diode bridge for 12 volts