Which Stirling engine has the best design with maximum efficiency. Which Stirling engine has the best design with maximum efficiency Devices with very high circuit efficiency

65 nanometers is the next goal of the Zelenograd plant Angstrem-T, which will cost 300-350 million euros. Application for receiving preferential loan The company has already submitted a request to Vnesheconombank (VEB) for modernization of production technologies, Vedomosti reported this week with reference to the chairman of the board of directors of the plant, Leonid Reiman. Now Angstrem-T is preparing to launch a production line for microcircuits with a 90nm topology. Payments on the previous VEB loan, for which it was purchased, will begin in mid-2017.

Beijing crashes Wall Street

Key American indices marked the first days of the New Year with a record drop; billionaire George Soros has already warned that the world is facing a repeat of the 2008 crisis.

The first Russian consumer processor Baikal-T1, priced at $60, is being launched into mass production

The Baikal Electronics company promises to launch into industrial production the Russian Baikal-T1 processor costing about $60 at the beginning of 2016. The devices will be in demand if the government creates this demand, market participants say.

MTS and Ericsson will jointly develop and implement 5G in Russia

Mobile TeleSystems PJSC and Ericsson have entered into cooperation agreements in the development and implementation of 5G technology in Russia. In pilot projects, including during the 2018 World Cup, MTS intends to test the developments of the Swedish vendor. At the beginning of next year, the operator will begin a dialogue with the Ministry of Telecom and Mass Communications on the formation of technical requirements for the fifth generation of mobile communications.

Sergey Chemezov: Rostec is already one of the ten largest engineering corporations in the world

The head of Rostec, Sergei Chemezov, in an interview with RBC, answered pressing questions: about the Platon system, the problems and prospects of AVTOVAZ, the interests of the State Corporation in the pharmaceutical business, spoke about international cooperation in the context of sanctions pressure, import substitution, reorganization, development strategy and new opportunities in difficult times.

Rostec is “fencing itself” and encroaching on the laurels of Samsung and General Electric

The Supervisory Board of Rostec approved the “Development Strategy until 2025”. The main objectives are to increase the share of high-tech civilian products and catch up with General Electric and Samsung in key financial indicators.

Today we will look at several circuits of simple, one might even say simple, pulse converters DC-DC voltage(DC voltage converters of the same magnitude, in constant voltage different size)

What are the benefits of pulse converters? Firstly, they have high efficiency, and secondly, they can operate at an input voltage lower than the output voltage. Pulse converters are divided into groups:

  • - bucking, boosting, inverting;
  • - stabilized, unstabilized;
  • - galvanically isolated, non-insulated;
  • - with narrow and wide range input voltages.

To make homemade pulse converters, it is best to use specialized integrated circuits- they are easier to assemble and not capricious when setting up. So, here are 14 schemes for every taste:

This converter operates at a frequency of 50 kHz, galvanic isolation is provided by transformer T1, which is wound on a K10x6x4.5 ring made of 2000NM ferrite and contains: primary winding- 2x10 turns, secondary winding - 2x70 turns of PEV-0.2 wire. Transistors can be replaced with KT501B. Almost no current is consumed from the battery when there is no load.

Transformer T1 is wound on a ferrite ring with a diameter of 7 mm, and contains two windings of 25 turns of wire PEV = 0.3.


Push-pull unstabilized converter based on a multivibrator (VT1 and VT2) and a power amplifier (VT3 and VT4). The output voltage is selected by the number of turns of the secondary winding of the pulse transformer T1.

Stabilizing type converter based on the MAX631 microcircuit from MAXIM. Generation frequency 40…50 kHz, storage element - inductor L1.


You can use one of the two chips separately, for example the second one, to multiply the voltage from two batteries.

Typical circuit for connecting a pulse boost stabilizer on the MAX1674 microcircuit from MAXIM. Operation is maintained at an input voltage of 1.1 volts. Efficiency - 94%, load current - up to 200 mA.

Allows you to obtain two different stabilized voltages with an efficiency of 50...60% and a load current of up to 150 mA in each channel. Capacitors C2 and C3 are energy storage devices.

8. Switching boost stabilizer on the MAX1724EZK33 chip from MAXIM

Typical connection diagram specialized chip from MAXIM. It remains operational at an input voltage of 0.91 volts, has a small-sized SMD housing and provides a load current of up to 150 mA with an efficiency of 90%.

A typical circuit for connecting a pulsed step-down stabilizer on a widely available TEXAS microcircuit. Resistor R3 regulates the output voltage within +2.8…+5 volts. Resistor R1 sets the current short circuit, which is calculated by the formula: Ikz(A)= 0.5/R1(Ohm)

Integrated voltage inverter, efficiency - 98%.

Two isolated voltage converters DA1 and DA2, connected in a “non-isolated” circuit with a common ground.

The inductance of the primary winding of transformer T1 is 22 μH, the ratio of turns of the primary winding to each secondary is 1: 2.5.

Typical circuit of a stabilized boost converter on a MAXIM microcircuit.

Single-ended converters with high efficiency, 12/220 volts

Some common household electrical appliances, such as a lamp daylight, photo flash and a number of others, sometimes it is convenient to use in a car.

Since most devices are designed to be powered from a network with an operating voltage of 220 V, a step-up converter is needed. An electric razor or a small fluorescent lamp consumes no more than 6...25 W of power. Moreover, such a converter is often not required alternating voltage on the way out. The above household electrical appliances operate normally when powered by direct or unipolar pulsating current.

The first version of a single-cycle (flyback) pulsed DC voltage converter 12 V/220 V is made on an imported UC3845N PWM controller chip and a powerful N-channel field-effect transistor BUZ11 (Fig. 4.10). These elements are more affordable than their domestic counterparts, and make it possible to achieve high efficiency from the device, including due to the low source-drain voltage drop across an open field-effect transistor (the efficiency of the converter also depends on the ratio of the width of the pulses transmitting energy to the transformer to the pause).

The specified microcircuit is specially designed for single-cycle converters and has all the necessary components inside, which allows reducing the number of external elements. It has a high-current quasi-complementary output stage specifically designed for direct power control. M-channel field-effect transistor with insulated gate. The operating pulse frequency at the output of the microcircuit can reach 500 kHz. The frequency is determined by the ratings of the elements R4-C4 and in the above circuit is about 33 kHz (T = 50 μs).

Rice. 4.10. Circuit of a single-cycle pulse converter that increases voltage

The chip also contains a protection circuit to shut down the converter when the supply voltage drops below 7.6 V, which is useful when powering devices from a battery.

Let's take a closer look at the operation of the converter. In Fig. Figure 4.11 shows voltage diagrams that explain the ongoing processes. When positive pulses appear at the gate of the field-effect transistor (Fig. 4.11, a), it opens and resistors R7-R8 will receive the pulses shown in Fig. 4.11, c.

The slope of the top of the pulse depends on the inductance of the transformer winding, and if at the top there is a sharp increase in the voltage amplitude, as shown by the dotted line, this indicates saturation of the magnetic circuit. At the same time, conversion losses increase sharply, which leads to heating of the elements and deteriorates the operation of the device. To eliminate saturation, you will need to reduce the pulse width or increase the gap in the center of the magnetic circuit. Usually a gap of 0.1...0.5 mm is sufficient.

When the power transistor is turned off, the inductance of the transformer windings causes voltage surges to appear, as shown in the figures.

Rice. 4.11. Voltage diagrams at circuit control points

With proper manufacturing of transformer T1 (sectioning the secondary winding) and low-voltage power supply, the surge amplitude does not reach a value dangerous for the transistor and therefore, in this circuit, special measures in the form of damping circuits in the primary winding of T1 are not used. And in order to suppress surges in the current signal feedback, coming to the input of the DA1.3 chip, a simple RC filter is installed from elements R6-C5.

The voltage at the converter input, depending on the condition of the battery, can vary from 9 to 15 V (which is 40%). To limit the change in output voltage, input feedback is removed from the divider of resistors R1-R2. In this case, the output voltage at the load will be maintained in the range of 210...230 V (Rload = 2200 Ohm), see table. 4.2, i.e. it changes by no more than 10%, which is quite acceptable.

Table 4.2. Circuit parameters when changing supply voltage

Stabilization of the output voltage is carried out by automatically changing the width of the pulse that opens transistor VT1 from 20 μs at Upit = 9 V to 15 μs (Upit = 15 V).

All elements of the circuit, except for capacitor C6, are placed on a single-sided printed circuit board made of fiberglass with dimensions of 90x55 mm (Fig. 4.12).

Rice. 4.12. Topology printed circuit board and arrangement of elements

Transformer T1 is mounted on the board using an M4x30 screw through a rubber gasket, as shown in Fig. 4.13.

Rice. 4.13 Mounting type of transformer T1

Transistor VT1 is installed on the radiator. Plug design. XP1 must prevent erroneous supply of voltage to the circuit.

The T1 pulse transformer is made using the widely used BZO armor cups from the M2000NM1 magnetic core. At the same time, in the central part they should have a gap of 0.1...0.5 mm.

The magnetic core can be purchased with an existing gap or it can be made using coarse sandpaper. It is better to select the gap size experimentally when tuning so that the magnetic circuit does not enter the saturation mode - this is convenient to control by the shape of the voltage at the source VT1 (see Fig. 4.11, c).

For transformer T1, winding 1-2 contains 9 turns of wire with a diameter of 0.5-0.6 mm, windings 3-4 and 5-6 each contain 180 turns of wire with a diameter of 0.15...0.23 mm (wire type PEL or PEV). In this case, the primary winding (1-2) is located between two secondary windings, i.e. First, winding 3-4 is wound, and then 1-2 and 5-6.

When connecting the transformer windings, it is important to observe the phasing shown in the diagram. Incorrect phasing will not damage the circuit, but it will not work as intended.

The following parts were used during assembly: adjusted resistor R2 - SPZ-19a, fixed resistors R7 and R8 type S5-16M for 1 W, the rest can be of any type; electrolytic capacitors C1 - K50-35 for 25 V, C2 - K53-1A for 16 V, C6 - K50-29V for 450 V, and the rest are of the K10-17 type. Transistor VT1 is installed on a small (by the size of the board) radiator made of duralumin profile. Setting up the circuit consists of checking the correct phrasing of connecting the secondary winding using an oscilloscope, as well as setting resistor R4 to the desired frequency. Resistor R2 sets the output voltage at the XS1 sockets when the load is on.

The given converter circuit is designed to work with a previously known load power (6...30 W - permanently connected). At idle, the voltage at the circuit output can reach 400 V, which is not acceptable for all devices, as it can lead to damage due to insulation breakdown.

If the converter is intended to be used in operation with a load of different power, which is also turned on during operation of the converter, then it is necessary to remove the voltage feedback signal from the output. A variant of such a scheme is shown in Fig. 4.14. This not only allows you to limit the output voltage of the circuit to idling 245 V, but will also reduce power consumption in this mode by about 10 times (Ipotr = 0.19 A; P = 2.28 W; Uh = 245 V).

Rice. 4.14. Single-cycle converter circuit with maximum no-load voltage limitation

Transformer T1 has the same magnetic circuit and winding data as in the circuit (Fig. 4.10), but contains an additional winding (7-4) - 14 turns of PELSHO wire with a diameter of 0.12.0.18 mm (it is wound last). The remaining windings are made in the same way as in the transformer described above.

To manufacture a pulse transformer, you can also use square cores of the series. KV12 made of M2500NM ferrite - the number of turns in the windings in this case will not change. To replace armor magnetic cores (B) with more modern square ones (KB), you can use the table. 4.3.

The voltage feedback signal from winding 7-8 is supplied through a diode to the input (2) of the microcircuit, which makes it possible to more accurately maintain the output voltage in a given range, as well as provide galvanic isolation between the primary and output circuits. The parameters of such a converter, depending on the supply voltage, are given in table. 4.4.

Table 4.4. Circuit parameters when changing supply voltage

The efficiency of the described converters can be increased a little more if the pulse transformers are secured to the board with a dielectric screw or heat-resistant glue. A variant of the printed circuit board topology for assembling the circuit is shown in Fig. 4.15.

Rice. 4.15. PCB topology and arrangement of elements

Using such a converter you can power from on-board network car electric razors "Agidel", "Kharkov" and a number of other devices.

This article will talk about the familiar, but many do not understand, term efficiency factor (efficiency). What is this? Let's figure it out. Efficiency factor, hereinafter referred to as efficiency, is a characteristic of the efficiency of the system of any device in relation to the conversion or transmission of energy. It is determined by the ratio of the useful energy used to the total amount of energy received by the system. Is it usually indicated? (" this"). ? = Wpol/Wcym. Efficiency is a dimensionless quantity and is often measured as a percentage. Mathematically, the definition of efficiency can be written as: n=(A:Q) x100%, where A is useful work, and Q is expended work. Due to the law of conservation of energy, efficiency is always less than or equal to unity, that is, it is impossible to obtain useful work more than the energy expended! Looking through different sites, I am often surprised how radio amateurs report, or rather, praise their designs for high efficiency, without having any idea what it is! For clarity, let’s use an example to consider a simplified converter circuit and find out how to find the efficiency of the device. A simplified diagram is shown in Fig. 1

Let's say we took as a basis a step-up DC/DC voltage converter (hereinafter referred to as PN), from unipolar to increased unipolar. We connect the ammeter RA1 into the power supply circuit break, and the voltmeter RA2 parallel to the power supply input PN, the readings of which are needed to calculate the power consumption (P1) of the device and the load together from the power source. At the output of the PN in the load supply break we also connect an ammeter RAZ and a voltmeter RA4, which are required to calculate the power consumed by the load (P2) from the PN. So, everything is ready to calculate the efficiency, then let's get started. We turn on our device, take measurements of instrument readings and calculate the powers P1 and P2. Hence P1=I1 x U1, and P2=I2 x U2. Now we calculate the efficiency using the formula: efficiency (%) = P2: P1 x100. Now you have found out approximately the real efficiency of your device. Using a similar formula, you can calculate PN with a two-polar output using the formula: Efficiency (%) = (P2+P3) : P1 x100, as well as a step-down converter. It should be noted that the value (P1) also includes current consumption, for example: PWM controller and (or) control driver field effect transistors, and other structural elements.


For reference: car amplifier manufacturers often indicate the output power of the amplifier is much higher than in reality! But you can find out the approximate real power of a car amplifier using a simple formula. Let’s say there is a +12v fuse on the car amplifier in the power supply circuit, there is a 50 A fuse. We calculate, P = 12V x 50A, and in total we get a power consumption of 600 W. Even in high-quality and expensive models, the efficiency of the entire device is unlikely to exceed 95%. After all, part of the efficiency is dissipated in the form of heat on powerful transistors, transformer windings, rectifiers. So let's go back to the calculation, we get 600 W: 100% x92=570W. Consequently, this car amplifier will not produce any 1000 W or even 800 W, as the manufacturers write! I hope this article will help you understand such a relative value as efficiency! Good luck to everyone in developing and repeating designs. The invertor was with you.

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