How to calculate a resonant switching power supply. Resonant power supply. Andreev's resonant choke on an W-shaped core from a transformer. How to turn a choke into an electricity generator

How to calculate a resonant switching power supply. Resonant power supply. Andreev's resonant choke on an W-shaped core from a transformer. How to turn a choke into an electricity generator

This high voltage source was made a long time ago, but I found it on the shelf and decided to describe it. This is practically an ordinary half-bridge (in their network huge pile) on IR2153 with the exception of a few points.

Firstly, the line transformer here operates at a resonant frequency, which means it produces a very high voltage. To prevent the liner from breaking through, it must not be turned on without a load! I think we need to make a protective arrester.

Secondly, “heavy” transistors (stw29nk50, there were such ones) that are quite unusual for such circuits are used at a fairly high frequency - about 120 kHz. In order to enable the IR2153 to control them, buffers are introduced. And in general, IR2153 is unloaded as much as possible. Voltage stabilization is external, buffers are also external. Mikruha's life has turned into a fairy tale)

Thirdly, the IR2153 powers itself after startup. The heating of resistor R4 is greatly reduced, and it can output more current to the gates. Another advantage of this approach is that if the source outputs are short-circuited for a long time, the power supply to ir2153 drops below the UVLO response threshold, it turns off, and is periodically turned on by the network resistor. Thus, the probability of removal from the short circuit is approximately zero.

Scheme (clickable)

The number of turns in the primary is 45, in the IR power supply winding – 4.

The transistors are placed on top of the radiator.

Assembled circuit

The liner himself didn’t want to fit into the body, so I had to file the body a little, and to make it look nice, I made a red cap with a big exclamation mark; I didn’t have enough talent to draw a lightning bolt))

Power consumption – 120W, short circuit. It can withstand loads without problems.

Video

My brother seems to have gotten used to the fact that I take away his camera in order to take pictures of my crafts. Therefore, here it is:

Why is the arc so dead? When it appears, the half-bridge goes out of resonance, and, because of this, the output power decreases. Power can always be increased by lowering the operating frequency and reducing the number of turns. Fortunately, transistors allow you to do this.

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The mains power supply is one of the most critical components in the structure of electronic equipment. The most important parameters of a network converter are: operating range of input voltage, power consumption in standby mode, overall dimensions, reliability, electromagnetic compatibility and cost. The vast majority of modern mains-powered equipment uses switching power supplies.

Introduction

The problems of energy saving and energy efficiency are among the most pressing in the global energy sector. One of the most important ways to increase the efficiency of a device is to increase the efficiency of switching power supply converters. Increasing efficiency and power density are the dominant factors in the design of AC/DC converters.

A feature of computer power supplies, as well as other power supplies of consumer electronic equipment, is that consumption varies within a wide range depending on the operating mode and activity of different system modules. A personal computer implements a power management mode by lowering the clock frequency, turning off power to the display, hard drive, or putting the PC into standby or sleep mode. The consumption range is from several watts (standby mode) to several hundred watts. In LCD TVs with dynamic LED backlighting or plasma panels, the current consumption is determined by the brightness of the current image on the screen. Ensuring high conversion efficiency for all modes is not an easy task.

Energy efficient electronics

Over the past ten years, a number of government organizations and initiative associations have developed criteria for assessing the efficiency of power supplies for electronic equipment. The main goal of the requirements is to control and significantly reduce the level of consumption of modern consumer electronic equipment. Equipment manufacturers must certify their products in accordance with these requirements.

Energy Star Program

Energy Star is a joint program of the US Environmental Protection Agency (EPA) and the Department of Energy. The goal of the program is to ensure the efficient use of generated electrical energy and reduce the harmful impact on the environment. One of the areas of the Energy Star program is the development of basic requirements for certification of consumption of consumer electronic equipment, in particular, computers, monitors, fax machines, copiers, televisions, audio systems, air conditioning systems, refrigerators and other household appliances. The development of new threshold requirements for the consumption of consumer electronic devices has forced manufacturers to use new energy-saving solutions, which has led to the emergence of a new class of electronic devices with reduced power consumption. For example, already in 2002, thanks to the active implementation of Energy Star standards, more than 100 billion kWh of electricity was saved in the United States alone.

Energy Star documents regulating energy efficiency requirements for electronic equipment:

  • Energy Star v5.0 Desktop Computers and Workstations (with 80 PLUS certified power supplies);
  • Energy Star v1.0 Datacenter Servers (with 80 PLUS certified power supplies);
  • Energy Star v5.0 LCD Monitors.

80 PLUS - new standards for power supply efficiency

Previously, the efficiency of most system unit power supplies was about 80%. Thanks to the work of the 80 PLUS Committee initiative group, a new unified system of efficiency standards for power supply manufacturers was adopted. These companies were forced to improve their performance indicators in order to obtain certification to enter the markets of leading countries.

The documents define the desired levels of conversion efficiency for three different converter load conditions (20, 50 and 100%) (table). In accordance with these levels, four classes of appliance efficiency are defined: bronze, silver, gold and platinum:

  • 80 PLUS E-Star 4.0 - 80% efficiency at all power supply load levels.
  • 80 PLUS Bronze - 82% efficiency at light (20%) and heavy (100%) power supply load and 85% efficiency at medium (50%) power supply load.
  • 80 PLUS Silver - 85% efficiency at light and heavy load on the power supply and 88% efficiency at average load on the power supply.
  • 80 PLUS Gold - 87% efficiency at light and heavy load on the power supply and 90% efficiency at average load on the power supply.

Table. 80 PLUS performance certification levels

80 PLUS Test type 115 V without internal redundancy 230 V with internal redundancy
Load level 20% 50% 100% 20% 50% 100%
80 PLUS 80% 80% 80% Not defined
80 PLUS Bronze 82% 85% 82% 81% 85% 81%
80 PLUS Silver 85% 88% 85% 85% 89% 85%
80PLUS Gold 87% 90% 87% 88% 92% 88%
80PLUS Platinum 90% 92% 89% 90% 94% 91%

In 2006, Energy Star included 80 PLUS requirements in its Energy Star 4.0 computer specifications. Already in November 2006 and February 2007, HP and Dell certified their computer power supplies to meet 80 PLUS requirements.

Switching Power Supply Architecture

A typical network computer ATX switching mode power supply (SMPS) should provide an output voltage of 12 V and a current of 20 A.

The main area of ​​application is the power supply for computer equipment (PC system unit), other computer devices, telecommunications equipment, LCD TVs, plasma panels, LED lamps and chargers. The main goal is efficient conversion, reduction in size, EMI level, as well as power loss and heat generation.

Initial data

The universal input voltage range is from 90 to 265 V AC at a frequency of 47-63 Hz. This means that the source will be able to operate in any country with any mains voltage rating, as well as with deviations from the nominal voltage and frequency. Output voltage and current - 12 V/20 A. Mains consumption - 50 mA in off mode; 100 mA in sleep mode; 5 A in active mode.

The proposed architecture shown in Fig. 1, has a three-stage structure:

  1. Power factor corrector.
  2. Controller of pulse voltage converter.
  3. Synchronous rectifier of the secondary circuit source.

Rice. 1. Block diagram of a 240 W switching power supply

The chosen architecture is based on the use of three efficient energy conversion stages. The first stage is a universal input active power factor corrector with an output voltage of 385 V on the NCP1397B controller. The second stage is a half-bridge resonant LLC converter. The +12 V secondary circuit of this source uses a synchronous rectification circuit built on the NCP4303 ON Semiconductor controller chip.

The architecture chosen for this project optimizes system resources to ensure maximum power conversion efficiency and meet the original power supply requirements. The architecture also allows to reduce the price, reduce the complexity of the device and increase its reliability.

First stage. Power factor corrector

The use of power factor correction (PFC) technology is one of the key aspects in the development of efficient and powerful network power supplies. The overwhelming number of household and industrial consumers of electricity currently use pulsed network converters and AC/DC converters. The typical structure of a network converter contains a diode bridge, a capacitive filter, and output stabilized voltage converters. If necessary, AC/DC converters can also contain galvanic isolation from the network.

The conversion efficiency is determined by the efficiency of the basic units - a rectifier with a filter and DC/DC converters. The “diode bridge - capacitor” link is weak in terms of energy transmission efficiency. The capacitance is charged and, therefore, energy consumption from the network occurs only in short phases during the “peaks” of the sinusoids of the network voltage. And the transfer of energy from the storage tank to the load may occur unevenly over time.

To provide the required current load, the capacitance of the capacitor must be quite large. As the converter power increases, the problem becomes critical. When charging a large storage capacity, current surges occur in the network in a short period of time. And at the initial moment the source is connected to the network, current surges can reach hundreds of amperes. This leads to distortion of the mains voltage waveform. The inclusion of non-linear loads in the network, for example, lamps with gas-discharge lamps, controlled electric motors, power supplies with a capacitive filter, etc., leads to the fact that the current consumed by these devices is pulsed in nature with a high percentage of high harmonics, due to which Electromagnetic compatibility problems may arise when operating various equipment.

Power Factor Corrector and Standards

The main task of the PFC is to reduce to zero the lag of the consumed current from the network voltage while maintaining the sinusoidal shape of the current. To do this, it is necessary to take current from the network not at short intervals, but throughout the entire period of operation. The power taken from the source must remain constant even if the network voltage changes. This means that when the network voltage decreases, the load current must be increased, and vice versa. From the network side, the power supply will look like a purely active resistance. The power factor corrector is a voltage converter with an inductive storage and energy transfer in reverse. The PFC stage in the structure of a powerful AC/DC converter is an intermediate source of stabilized voltage, from which other voltage converters are powered.

Active power factor correction is widely used in all modern high-power power supplies. The use of a power factor correction stage can increase conversion efficiency and reduce the level of network interference. The need for a power factor corrector (PFC) in powerful network sources of secondary power supply is regulated by the electromagnetic compatibility requirements of GOST R 51317-2000. The standards for harmonic components of current consumption and power factor for power supply systems with a power of more than 50 W and all types of lighting equipment are determined by the IEC standard IEC 1000-3-2. For power supply devices for communication equipment, since March 2001, the Ministry of Communications of the Russian Federation introduced OST 45.188-20-01, which states that the power factor of power supply equipment must be at least 0.95 for devices with power correction.

Structure of the power corrector module

The power factor corrector module (Fig. 2) contains a PFC controller chip, an inductor, a powerful MOSFET switch, a rectifier diode, feedback sensor circuits and an output capacitance.

Rice. 2. Structure of power factor corrector

Regulation and stabilization of the output voltage is carried out by a PWM signal. The diagram does not show the power supply circuits, control modes and protection thresholds. The circuit is practically no different from the classic circuits of pulsed voltage converters. Just a few features are worth noting. To meet the requirements of electromagnetic compatibility standards, the conversion in the correctors is always carried out at a constant frequency. Typically above 200 W, most PFCs are designed as booster converters operating in continuous conduction mode (CCM) or Continuous Current Mode (CCM).

NCP1605 - power factor correction controller

NCP1605 is a power factor correction controller chip. It operates at a fixed conversion frequency and in the Critical Conduction Mode control mode. For 240 W output power, the most efficient Frequency Clamped Critical Conduction Mode (FCCrM) is selected because it provides not only high conversion efficiency, but also low EMI levels. The NCP1605 controller operates in this mode. The circuit also has built-in protection, both against current overload and for load-off mode.

Second stage. Half-bridge resonant LLC converter

The SMPS switching power supply stage uses a half-bridge LLC resonant topology, which significantly improves conversion efficiency and allows for reduced EMI levels and improved isolation transformer utilization compared to traditional topologies (Figure 3). LLC uses two inductances (LL) connected in series - inductor + primary winding of the transformer, and one capacitance (C).

Rice. 3. Structure of a half-bridge resonant LLC converter

The half-bridge resonant converter has an LLC topology and belongs to the subtype of series resonant converters (SRC). It is widely used in applications where high power density is required.

The half-bridge resonant LLC converter circuit is an excellent alternative to the traditional Half Bridge (HB) topology for several reasons:

  • Switching occurs when the voltage crosses zero (Zero Voltage Switching, ZVS) over a wide range of loads. Since switching occurs at low switch drain voltage, switching losses are minimized. This also allows for a significant reduction in EMI levels compared to the HB (half bridge) topology, which requires switching under more severe conditions.
  • Low current during switching. The switch closes at low throughput current, resulting in low energy loss compared to that of an HB topology.
  • Low turn-off current on the secondary circuit diodes: when the converter operates in high output current mode, the output rectifier goes into the off state under the condition of low current flow, which reduces the EMI level.
  • The circuit topology does not increase the number of components. The total number of components remains the same as in the classic half-bridge topology.

In Fig. Figure 4 shows a block diagram of a half-bridge resonant converter. Half-bridge switches operate with a duty cycle of 50% and provide the formation of high-voltage rectangular pulses with an amplitude from 0 to the input voltage V IN, which enters the resonant circuit. By adjusting the frequency via a voltage controlled oscillator (VCO), tracking feedback is provided. The frequency varies depending on the load size.

Rice. 4. Block diagram of a half-bridge resonant voltage converter

NCP1397 - LLC converter controller

The heart of the half-bridge resonant LLC converter is the NCP1397 controller chip. Featuring proprietary high-voltage technology, this controller contains a MOSFET driver for a half-bridge output circuit. The supply voltage of the half-bridge circuit is up to 600 V.

The controller has multi-level built-in protection, including blocking the output in the event of a loss of input voltage, loss of a feedback signal from an optocoupler, etc. This allows you to improve the reliability of the stage without complicating the design and additional components.

Secondary circuit of the power supply. Synchronous rectifier

Why is synchronous rectification needed? The use of a synchronous rectification circuit makes it possible to reduce rectification losses at high current and load values. When using a conventional diode circuit, even with Schottky diodes, at high currents the voltage drop increases significantly and, accordingly, losses increase.

In Fig. Figure 5 shows the advantages of using synchronous rectifier at high output current compared to a conventional diode rectifier circuit.

Rice. 5. Comparison of losses on a synchronous rectifier and a conventional diode rectifier (losses on Schottky diodes will be greater at higher currents than on the open channel of a MOSFET transistor)

However, it can be noted that the synchronous rectification mode becomes ineffective in the zone of low currents in the load. To maintain efficiency over a wide load range, the synchronous rectifier module automatically turns off at low currents. In Fig. Figure 6 shows the control circuit for NCP4303 synchronous rectifiers with a shutdown circuit for low load currents.

I usually adhere to the principle that the fewer parts in a circuit, the simpler it is, the more reliable it is. But this case is an exception. Those who have designed and assembled circuits for powerful step-up voltage converters from 12/24 volts to 300 (for example), know that classical approaches do not work well here. The currents in low voltage circuits are too high. The use of PWM circuits leads to switching losses, which instantly overheat and damage the power transistors. The internal resistance of power switches is a serious obstacle to the use of circuits with design limitation of switching losses, such as bridge and half-bridge circuits.

The above circuit is based on separating the function of increasing the voltage and stabilizing it in different stages. With this approach, we get the opportunity to force the most problematic unit - the inverter - to work in resonant mode with minimal losses on the power switches and the rectifier bridge in the high-voltage part of the circuit. And the output voltage is stabilized in the block ST, which is assembled using a simple boosting topology. Now its diagram is not given; there will be a separate article about it. A stable required voltage is removed from its output.

Schematic diagram of a resonant voltage converter

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Half-bridge quasi-resonant power supply

To improve the characteristics of switching power supplies assembled on the basis of bridge and half-bridge converters, in particular, to reduce the likelihood of through current and increase efficiency, the authors propose to transfer such sources to a quasi-resonant operating mode. The described article provides a practical example of such a power supply.

Often, to reduce size and weight, power supplies (PS) with a network transformer are replaced with pulse voltage converters. The benefit from this is obvious: lower weight and dimensions, significantly lower copper consumption for winding products, high efficiency of the power supply. However, pulsed power supplies also have disadvantages: poor electromagnetic compatibility, the possibility of through current appearing through transistors in push-pull converters, the need to introduce overcurrent protection circuits, and the difficulty of starting a capacitive load without taking special measures to limit the charging current.

Let us consider, using the example of a push-pull half-bridge self-oscillating voltage converter, how these disadvantages can be eliminated or reduced to a certain extent by changing its operating mode. Let's switch the converter to a quasi-resonant operating mode by introducing a resonant circuit. The shape of the current through the primary winding of the pulse transformer in this case is shown in Fig. 1.

In Fig. Figure 2 shows the voltage and current waveforms for one of the switching transistors. From the figures it can be seen that the converter operates in a quasi-resonant mode - there is no through current in this case.

The voltage at the base of the switching transistor decreases and becomes zero at the end of the pulse. Thus, the transition to a quasi-resonant operating mode completely eliminates dynamic losses in switching transistors and problems associated with the electromagnetic compatibility of sensitive devices with pulsed power supply, since the spectrum of generated oscillations is sharply narrowed.

A half-bridge converter differs from a push-pull bridge converter in the smaller number of transistors used; from a push-pull with a middle output - half the voltage on the transistors. A self-generating converter differs from converters with a master oscillator, first of all, in the minimum number of elements, the maximum possible efficiency, and the use of a saturable auxiliary transformer is guaranteed to exclude the possibility of through current.

The circuit of a half-bridge quasi-resonant power supply, devoid of the listed disadvantages, is shown in Fig. 3.

(click to enlarge)

Main technical characteristics

  • Supply voltage change interval, V....198...264
  • Maximum efficiency, %......92
  • Output voltage, V, with a load resistance of 36 Ohms......36
  • Operating frequency conversion interval, kHz......12...57
  • Maximum output power, W......70
  • Maximum amplitude of output voltage ripple with operating frequency, V......2.2

The IP contains the following components: noise suppression filter C1C2L1, which prevents the penetration of high-frequency ripples created by the converter into the supply network; network rectifier VD1 with filter capacitor C3; protection circuits against overload and short circuits in the load R1R2VD2K1U1VD3VD4R6R7C7. The protection circuit consumes insignificant current, therefore it has little effect on the overall efficiency of the source, but if necessary, the efficiency can be increased slightly by replacing the zener diode VD2 with a higher voltage one. Resistors R6 and R7 form a voltage divider necessary to turn on the emitting diode of the thyristor optocoupler. If these fixed resistors are replaced with one variable resistor, the protection threshold can be adjusted within very wide limits. If you intend to power a load with a large capacitance (more than 5000 μF), to eliminate false protection triggers, you should increase the capacitance of capacitor C7, however, the waiting time before turning on the source will increase in this case.

Elements R3, R4, C4, C5 form a voltage divider. Resistors R3, R4 are necessary to discharge the capacitors of filter C3 and divider C4C5 after turning off the power supply. Capacitor C6 and inductor L2 are a resonant circuit. The triggering circuit is exactly the same as in the device described in the article. It consists of transistor VT3, resistors R10-R12 and capacitor C10. Transistor VT3 operates in avalanche mode. The triggering pulse opens transistor VT2, providing initial asymmetry.

Diodes VD5-VD8 - output rectifier with filter capacitors C8, C9. LED HL1 indicates the presence of voltage at the output of the IP. Self-generation of oscillations occurs as a result of positive feedback from winding III of transformer T1 to winding III of transformer T2 through current-limiting resistor R9. As its resistance decreases, the conversion frequency decreases, which leads to a shift in the maximum efficiency of the source towards a higher load power.

The device uses capacitors K73-17 (C1, C2, C6, C9, C10), K73-11 (C4, C5), K50-32 (C3), K50-24 (C7, C8). All resistors are C2-23. Instead of the specified capacitors and resistors, it is possible to use other components, however, capacitors should be selected with a minimum dielectric loss tangent in the operating frequency range of the power supply conversion.

Diode bridge VD1 - any with a permissible forward current of more than 1 A and a permissible reverse voltage of at least 400 V, for example BR310. It is also possible to use discrete diodes, for example KD202R, connected via a bridge circuit. It is best to use the KT315G (VT3) transistor in the device - the triggering circuit will work with it immediately, the KT315B transistor will have to be selected, and it is better not to use the KT315A, KT315V transistors. Transistors KT826V (VT1, VT2) are interchangeable with any of the KT826 or KT812A, KT812B series. Due to low losses, transistors can not be installed on heat sinks. The diodes of the output rectifier KD213A (VD5-VD8) can be replaced with KD213B, KD213V or the KD2997, KD2999 series. They should be installed on a heat sink with a cooling surface area of ​​at least 10 cm2.

The IP uses an electromagnetic DC relay GBR10.1-11.24 with an operating voltage of 24 V, capable of switching an alternating current of 8 A in circuits with voltages up to 250 V. It can be replaced by any other with a permissible switched alternating current of at least 1 A in circuits with voltage 250 V. However, it is advisable to use a relay with a minimum switching current to increase the efficiency of the power supply, since the lower the switching current, the greater the resistance of resistors R1, R2 and the less power will be dissipated on them.

Chokes L1, L2 and transformer T1 were used ready-made - from the old EC1060 computer: L1 - I5, L2 - 4777026 or 009-01, T1 - 052-02. You can make them yourself. Inductor L1 is wound (two windings at the same time) on a ring magnetic core K28x16x9 made of ferrite (for example, grades M2000NM-A or M2000NM1-17) or alsifer. Its windings contain 315 turns of PEV-2 0.3 wire.

The resonant choke L2 is wound on a ring magnetic core K20x10x5 made of M2000NM-A ferrite. Its winding contains 13 turns of PEV-2 0.6 wire.

Transformer T1 is wound on a ring magnetic core K45x28x8 made of M2000NM1-17 ferrite. Winding I contains 200 turns of PEV-2 0.6 wire, winding II - 35 turns of PEV-2 1 wire, winding III - 5 turns of PEV-2 0.6 wire. The order of winding the windings on the magnetic circuit is arbitrary. Between the windings it is necessary to lay a layer of insulation, for example, fluoroplastic tape. In addition, the transformer should be impregnated, for example, with paraffin from candles or ceresin. This will not only increase the dielectric strength of the insulation, but also reduce the hum created by the source at idle.

Transformer T2 is wound on a ring magnetic core K20x10x5 made of M2000NM-A ferrite. Windings I and II each contain seven turns of PEV-2 0.3 wire (they are wound simultaneously into two wires), and winding III contains nine turns of PEV-2 0.3 wire.

The design of the IP can be arbitrary; the relative position of the elements on the board is not critical. It is only important to ensure good air flow to the semiconductor devices by natural convection or install the power supply inside the powered device near the fan.

The described IP practically does not require adjustment, although it is worth making sure that the converter operates in a quasi-resonant mode. To do this, an equivalent load is connected to the output of the power supply - a resistor with a power of 100 W and a resistance of 36 Ohms. An additional resistor with a resistance of 0.1...1 Ohm and a power of 1...2 W is connected in series with capacitor C6. The oscilloscope probes are connected to an additional resistor: common - to the midpoint of the voltage divider R3R4C4C5, signal - to capacitor C6. It is necessary to ensure that the oscilloscope is not galvanically connected to the network. If connected, it should be connected to the network through an isolation transformer with a transformation ratio of 1:1. In any case, safety regulations must be followed. By applying power to the IP, make sure that there are bell-shaped current pulses with a pause at zero. If the pulse shape differs from that shown in Fig. 1, it is necessary to select the number of turns of inductor L2 until resonance is obtained.

On an additional resistor with a resistance of 0.1 Ohm, the pulse amplitude should be about 0.1 V. Now you should compare the shape of the current and voltage on the switching transistor VT2 with those shown in Fig. 2 graphs. If they are close in shape, the IP operates in a quasi-resonant mode.

The protection threshold can be changed. To do this, select the resistance of resistor R7 so ​​that the protection operates at the required load current. If it is necessary for the power supply to be turned off when the load power is less than 70 W, the resistance of resistor R7 should be reduced.

To limit the charging current of capacitor C3 at the moment of switching on, we recommend connecting a resistor with a resistance of 5.6 ... 10 Ohms with a power of 2 W to the gap of any network wire.

Literature

  1. Baraboshkin D. Improved economical power supply. - Radio, 1985, No. 6, p. 51.52.
  2. Konovalov E. Quasi-resonant voltage converter. - Radio, 1996, No. 2, p. 52-55.

See other articles section.