Bc337 amplifier circuit

Small form factor 2 x 7W Hi-Fi stereo amplifier, built from discrete parts. This is a fairly standard amplifier circuit that provides excellent audio quality, due to its simplicity, low power requirements and use of modern, high-quality semiconductors. The input stage T1, T2 was built with ultra high-gain, low-noise MPSA18 transistors; the current mirror T5, T6 further increases the open loop gain and forces the input stage to the fully balanced state, thus increasing linearity and drastically reducing the offset voltage on the output.

The voltage amplification stage T9 was built with the medium-gain BC transistor, though theoretically better performance can be achieved with the low-noise versions BC, BC The Miller-capacitor C3 is pF foil-type. The amplifier stops oscillating with a 33pF Miller-cap, and with pF, it's still able to deliver 5Vpp kHz sharp square wave signal on its output, full of upper harmonics. Physically, the Vbe multiplier should be mounted near to the driver transistors T3, T11 but far away from the output transistors T12, T4in order to ensure the best thermal stability.

The output stage T3, T12, T11, T4 was built with compound Sziklai pairs, this arrangement has several practical advantages over the more commonly used Darlington pair e. With a 2x9V 30VA toroid transformer, the idle voltage is approximately 2x13V at the output of the rectifier and buffer caps.

The input impedance is relatively low 2k ohmthe amplifier works very well with the headphone output of any sound source smart TV, phone, mp3 player, laptop. The voltage amplification is approximately 22x which gives a 22Vpp at 1Vpp nominal input. The amplifier was designed to drive ohm speakers, but is able to drive 4 ohm speakers at a somewhat reduced performance.

Using 1kHz sine wave and 6. Noise: The amplifier noise including hum 60Hz is probably less than 2mVpp. There is no audible noise on the speakers, even if listening closely. Cheap ceramic caps may be used for C2 and C7, as these parts are non-critical.

C15 and C19 are aluminum electrolytic caps, rated at min 25V. Tantalum capacitors should be avoided. R8 and R9 have to withstand low-mid loads, ideally these parts should be rated at 0. R10 and R11 are high-power wirewound resistors, rated at 3W; R18 is a wirewound resistor, rated at 1W. All other low power resistors are non-critical, they can be plain 0. The amplifier with the rectifier and buffer caps fits on a small 3" x 2" perforated PCB. The high-current wires and the legs of associated parts e.

Where that was impossible, I used thin wrap-wire. The wonderfully simple idea of using thick cables to connect the chassis-mounted power transistors to the circuit instead of soldering them directly onto the board came from the inglorious Videoton Hi-Fi amps.

These steps can be used as a general guide to bring up any similar class-AB audio amplifier by an average builder, without any special tools or instruments. The main goal of this process is to ensure that the amp will work according to the specs, and to eliminate any adverse behaviour.This is the circuit diagram of 2 Watt mini audio amplifier. This circuit is inexpensive, easy and quite simple.

This is general audio amplifier which can be used for computer, CD player or other devices which have headphone output. The circuit was deliberately designed using no ICs and in a rather old-fashioned manner in order to obtain good harmonic distortion behaviour and to avoid hard to find components. The amplifier s can be conveniently supplied by a 12V wall plug-in transformer. Closing SW1 a bass-boost is provided but, at the same time, volume control must be increased to compensate for power loss at higher frequencies.

In use, R9 should be carefully adjusted to provide minimal audible signal cross-over distortion consistent with minimal measured quiescent current consumption; a good compromise is to set the quiescent current at about mA. To measure this current, wire a DC current meter temporarily in series with the collector of Q3. Has anyone built this and does it work? Do you need heatsinks for the transistors? Mine get very very hot. Hi there,I have a Minelab S.

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I would like to have an external speaker instead of headphones. Would this amp do the job.

bc337 amplifier circuit

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Learn how your comment data is processed. Leave a Reply Cancel reply Your email address will not be published. Popular Search. Recent Circuit Search. Random Search Terms. SPST switch.Operational amplifiers, commonly known as opamps are the most common type of building block in analog electronics.

And has a single output. The first input is called inverting because the output voltage is inverse of the voltage applied at inverting input, times the gain of the amplifier circuit.

Design a Simple Common Emitter Amplifier

If we apply the signal to the non-inverting input we get the same signal on the output, times gain. Most opamp circuits use negative feedback to limit the ideal infinite gain of an opamp to the desired value.

This feedback allows for great control of opamp gain so that the gain of a circuit utilizing negative feedback is not determined by the gain of the device used opamp or transistor but by the feedback itself as long as the gain defined by feedback is considerably lower than the gain of the device used. An ideal opamp has infinite gain without feedback open-loopzero noise, infinite input resistance, zero output resistance, infinite slew rate, and infinite bandwidth.

Noise parameters vary a lot from opamp to opamp. The slew rate is how fast the opamps can swing their outputs. LM has a slew rate of around 0. This type of amplifier is a special one because no negative feedback is used to limit the gain. The signal can be applied at either input, but the other input has to be grounded. This much gain is seldom needed on its own, it also provides an opportunity for parasitic oscillations to occur.

If the open-loop gain parameter is not tightly controlled during manufacturing, opamps of the same type can give different open-loop gain. The open-loop amplifier can also be used as an analog comparator. In fact, comparators are basically opamps with a different name. The non-inverting amplifier uses negative feedback to reduce the gain to a required value. This way the gain of the circuit is not governed by the open-loop gain of the opamp, but by a set of feedback resistors, allowing for more flexibility.

The input signal is fed straight to the positive input of the amplifier, causing the input impedance to be practically equal to the input impedance of the opamp at audio frequencies. The negative feedback and therefore gain Av is set by the ratio of resistors R1 and R2 and is always greater or equal to one.

A special case of the non-inverting amplifier is the unity gain buffer, where instead of the feedback network the negative input is connected directly to the output.

This configuration is used in active audio filters, opamp headphone amplifiers and wherever there is a need for a high input impedance buffer stage. This circuit can be compared to a common-collector transistor amplifier configuration. An Inverting amplifier differs from the non-inverting amplifier due to much lower input impedance equal to the value of R1 And the output signal in an inverting amplifier is inverted with respect to the input signal.

The negative feedback and therefore gain Av is set by the ratio of resistors R2 and R1. The inverting configuration allows for gains both higher and lower than one.

How to build Headphone Amplifier

Similar to the other opamp circuits the voltages on both the inputs turn out to be the same due to the opamp properties. Hence if the positive input is grounded, the negative input will also be grounded or at 0 volts. Now the feedback voltage from the output combines with the input voltage and since these voltages are of opposite polarities the resulting voltage is zero volts, explaining the low input impedance.

Overall both the inverting and non-inverting amplifiers can provide good performance, the only difference is of input impedance. The low input impedance of the inverting amplifier is useful where a set input impedance is needed, for example in systems that use transmission lines that have a set impedance or LC filters. The non-inverting amplifier is useful where a high input impedance is necessary, for example in stages following active filters, oscillators, audio amplifiers, DC amplifiers used in voltmeters, etc.

Another advantage of the inverting amplifier is that the gain can be lower than one, unlike the non-inverting amplifier with its gain being always higher than one. All the circuits provided above only shows the feedback resistors. One might be tempted to think that this is all you need for an opamp to work with a single supply, like using one 9V battery or 5V from the USB.Let's explore the basic DNA of an audio amplifier.

This internal structure not only describes the majority of audio amps today, but also the innards of most op amps today. The design of these amplifiers share 3 common building blocks. Designers optimize the gain, linearity or power in various stages depending on the requirements - from a cheap headphone amplifier to a high performance W sound system. And this gives rise to the vast number of different types of audio amplifiers and op amps running around the universe today. We'll build an audio amplifier and follow the signal through the structure.

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Finally, you'll get a chance to vary components to see their effect on performance. By the way, there's enough literature on the design and analysis of audio amps to choke a horse. We'll try to hit the essential points. The basic amplifier above is a great place to start. But wait, there's more!

Operational Amplifier Basics with 6 Circuit Examples

In other topics, we'll explore each stage and enhance it. With the help of some hands-on SPICE simulations, you'll understand every component, its role, and how to make a reasonable design choice about it.

In a nutshell, here's the three fundamental building blocks of audio amplifiers and op amps. This is also a trans-conductance stage: voltage in, current out. The transconductance gm1 of Q1, Q2 set the gain of this stage.

Unfortunately, the output is a current! No problem, the next stage gets us back to voltage. Most of our voltage gain happens here. We also place an important component here - the dominant pole capacitor CC. It determines the main pole low-pass filter of the amplifier. Why is CC needed? It keeps the amplifier from oscillating, helps present a low impedance to the next stage and linearizes this stage reduces distortion with its local feedback. The Gain Stage also shifts the signal from the negative rail up to the the next stage - the output buffer.

So why include it? It let's you drive relatively low-impedance loads without effecting the gain. Hanging a load directly on RC3 would kill its voltage gain.Who does not like the rumbling tone of a distorted electric guitar?

It is a key part of many important genres of music, especially in blues and rock music genres and is also frequently used in hard rock, metal or the punk music genre.

In this project, we will build a basic distortion pedal for guitars using a simple circuit. You can also check out the Arduino Guitar Tuner Circuit if you are looking for more guitar-related projects. Before we get into details, distortion pedals are one of the most used guitar effect pedals in music electronic and therefore, it is essential to learn how distortion pedals work.

The distortion pedal produces a distorted sound on the musical notes. Generally, A Distortion pedal circuit is used in between the guitar audio source and the Power Amplifier. A simple block diagram of a guitar with a distortion circuit looks like this below. Distortion pedals are made using a minimum of the two most important things, namely the preamplifier section and the diode clipping circuit. The Audio preamplifier section adds up the gain to the input signal and the diode clipping section clips or chops out the positive and negative peak of the audio signal.

Often, distortion pedals are also called as overdrive or fuzz pedals. In this article, we are going to build a transistor-based Distortion circuit.

The components that are required for constructing the basic distortion pedal circuit are. In the below image, a basic distortion pedal schematic using a transistor is shown. The transistor acts like a basic preamplifier.

The K resistor is used as a collector resistor and the two capacitors are used for the audio input and audio output related purposes. The capacitors will block any DC and only pass the AC signal. The capacitor's value can be selected from. The selection of the transistor is essential for this project. In the above circuit, we used BC transistors. This transistor provides pretty good gain to the input signal.

NPN Transistor BC337 as a Switch

One can use other transistors as well. Two diodes D1 and D2 create a diode clipping circuit. This is the place where the distorted sound is created. Let's assume that the input signal is an AC sinusoidal signal that looks like the below image. It is a perfect sinusoidal wave. Now a diode clipping circuit like the one that is used in the schematic, chops off or clips the sinusoidal wave as per the diodes forward voltage. The clipped sinusoidal wave will look like the below image.

The diode D1 will be reverse biased with respect to the output and clips the negative peak of the output signal. Similarly, the diode D2 will be forward-biased with respect to the output clip and clips the positive peak of the output signal.

Therefore if we compare these input and output signal, it will look like the below image. But how will this affect in distorted sound? That is due to the speaker's response to the sinusoidal wave. When the sinusoidal wave goes positive the speaker diaphragm moves forward, when it goes negative the speaker diaphragm moves backward.

But the Forward and Backward movement of the speaker goes smoothly due to the proper sinusoidal wave response.BC is another good transistor that is having many good features in its small TO package. It is also a must to have transistor in your lab, one of a good feature of this transistor is its mA collector current that is rarely found in this package transistors.

BC is a NPN transistor with good characteristics, this transistor can be used in audio frequency driver stages, low power audio amplifier stages and wide variety of general purpose functions for example amplification and switching purposes.

This little TO transistor is packed with lot of good features which makes it suitable for used in many electronic circuits. The max load this transistor can handle is mA which is enough to drive many loads in an electronic circuits.

The maximum voltage this transistor allow through its collector to emitter is 45V that is a good feature which makes it suitable to use in circuits which require more than 24V. The max gain this transistor can provide is that is also a good feature that makes it suitable to use in audio frequency amplification circuits.

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BC can be used in variety of electronic circuits and projects, due to its high maximum characteristics you can use it in small audio amplification stages and at the output stage of low power audio amplifiers, its high gain feature also allows it to be used in audio preamplifier stages. To safely run this transistor in your circuit for long term do not operate it directly in circuit which are using more than 45V.

Also use a suitable resistor base resistor to limit its base current to required level. July 10, December 11, July 1, Your email address will not be published. Save my name, email, and website in this browser for the next time I comment. Leave a Reply Cancel reply Your email address will not be published.

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bc337 amplifier circuit

We use cookies to ensure that we give you the best experience on our website. If you continue to use this site we will assume that you are happy with it. Ok Privacy policy.The BC is an NPN transistor with a maximum gain ofcommonly used in low power audio applications.

It can also switch loads upto 45V and mA hence also used as general purpose transistor. The Transistor can provide a maximum gain hfe of Apart from the gain value other parameters are similar for all the three part numbers.

The transistor also has a high collector current of upto mA and a decent collector emitter voltage of 45V and the base trigger voltage is only 5V. This makes the transistor suitable to be used in general purpose switching circuits. Due to its low base trigger voltage it can be easily controlled by digital circuits like microcontroller circuits. So, if you are looking for a transistor for audio amplification then you might consider the BC Also look into the more commonly used 2N Transistor if you are looking for a replacement for BC to switch loads.

If you are designing a PCD or Perf board with this component then the following picture from the Datasheet will be useful to know its package type and dimensions. Subscribe to stay updated with industry's latest Electronics components and news. Component Datasheet.

BC337 Transistor Pinout, Equivalent, Uses, Features & Applications

BC Datasheet. Tags NPN Transistor.

bc337 amplifier circuit

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