An Introduction to the Amplifier Tutorial

Not all amplifiers are the same and are therefore classified according to their circuit configurations and methods of operation. In “Electronics”, small signal amplifiers are commonly used devices as they have the ability to amplify a relatively small input signal, for example from a Sensor such as a photo-device, into a much larger output signal to drive a relay, lamp or loudspeaker for example.

There are many forms of electronic circuits classed as amplifiers, from Operational Amplifiers and Small Signal Amplifiers up to Large Signal and Power Amplifiers. The classification of an amplifier depends upon the size of the signal, large or small, its physical configuration and how it processes the input signal, that is the relationship between input signal and current flowing in the load.

The type or classification of an amplifier is given in the following table.

Classification of Amplifiers

Type of Signal Type of
Configuration
Classification Frequency of
Operation
Small Signal Common Emitter Class A Amplifier Direct Current (DC)
Large Signal Common Base Class B Amplifier Audio Frequencies (AF)
  Common Collector Class AB Amplifier Radio Frequencies (RF)
    Class C Amplifier VHF, UHF and SHF
Frequencies

Amplifiers can be thought of as a simple box or block containing the amplifying device, such as a Transistor, Field Effect Transistor or Op-amp, which has two input terminals and two output terminals (ground being common) with the output signal being much greater than that of the input signal as it has been “Amplified”.

Generally, an ideal signal amplifier has three main properties,  Input Resistance or  ( Rin ),  Output Resistance or  ( Rout ) and of course amplification known commonly as Gain or ( A ). No matter how complicated an amplifier circuit is, a general amplifier model can still be used to show the relationship of these three properties.

Ideal Amplifier Model

introduction to the amplifier

 

The difference between the input and output signals is known as the Gain of the amplifier and is basically a measure of how much an amplifier “amplifies” the input signal. For example, if we have an input signal of 1 volt and an output of 50 volts, then the gain of the amplifier would be “50”. In other words, the input signal has been increased by a factor of 50. This increase is called Gain.

Amplifier gain is simply the ratio of the output divided-by the input. Gain has no units as its a ratio, but in Electronics it is commonly given the symbol “A”, for Amplification. Then the gain of an amplifier is simply calculated as the “output signal divided by the input signal”.

Amplifier Gain

The introduction to the amplifier gain can be said to be the relationship that exists between the signal measured at the output with the signal measured at the input. There are three different kinds of amplifier gain which can be measured and these are: Voltage Gain ( Av ), Current Gain ( Ai ) and Power Gain ( Ap ) depending upon the quantity being measured with examples of these different types of gains are given below.

Amplifier Gain of the Input Signal

amplifier block

Voltage Amplifier Gain

Amplifier Voltage Gain

Current Amplifier Gain

Amplifier Current Gain

Power Amplifier Gain

Amplifier Power Gain

 

Note that for the Power Gain you can also divide the power obtained at the output with the power obtained at the input. Also when calculating the gain of an amplifier, the subscripts v, i and p are used to denote the type of signal gain being used.

The power Gain or power level of the amplifier can also be expressed in Decibels, (dB). The Bel is a logarithmic unit (base 10) of measurement that has no units. Since the Bel is too large a unit of measure, it is prefixed with deci making it Decibels instead with one decibel being one tenth (1/10th) of a Bel. To calculate the gain of the amplifier in Decibels or dB, we can use the following expressions.

  •   Voltage Gain in dB:    av  =  20 log Av
  •   Current Gain in dB:    ai  =  20 log Ai
  •   Power Gain in dB:      ap  =  10 log Ap

Note that the DC power gain of an amplifier is equal to ten times the common log of the output to input ratio, where as voltage and current gains are 20 times the common log of the ratio. Note however, that 20dB is not twice as much power as 10dB because of the log scale.

Also, a positive value of dB represents a Gain and a negative value of dB represents a Loss within the amplifier. For example, an amplifier gain of +3dB indicates that the amplifiers output signal has “doubled”, (x2) while an amplifier gain of -3dB indicates that the signal has “halved”, (x0.5) or in other words a loss.

The -3dB point of an amplifier is called the half-power point which is -3dB down from maximum, taking 0dB as the maximum output value.

Example No1

Determine the Voltage, Current and Power Gain of an amplifier that has an input signal of 1mA at 10mV and a corresponding output signal of 10mA at 1V. Also, express all three gains in decibels, (dB).

The Various Amplifier Gains:

amplifier gain

Also in Decibels (dB):

amplifier gain in decibels

Then the amplifier has a Voltage Gain of 100, a Current Gain of 10 and a Power Gain of 1,000.

Generally, amplifiers can be sub-divided into two distinct types depending upon their power or voltage gain. One type is called the Small Signal Amplifier which include pre-amplifiers, instrumentation amplifiers etc. Small signal amplifies are designed to amplify very small signal voltage levels of only a few micro-volts (μV) from sensors or audio signals.

The other type are called Large Signal Amplifiers such as audio power amplifiers or power switching amplifiers. Large signal amplifiers are designed to amplify large input voltage signals or switch heavy load currents as you would find driving loudspeakers.

Power Amplifiers

The Small Signal Amplifier is generally referred to as a “Voltage” amplifier because they usually convert a small input voltage into a much larger output voltage. Sometimes an amplifier circuit is required to drive a motor or feed a loudspeaker and for these types of applications where high switching currents are needed Power Amplifiers are required.

As their name suggests, the main job of a “Power Amplifier” (also known as a large signal amplifier), is to deliver power to the load, and as we know from above, is the product of the voltage and current applied to the load with the output signal power being greater than the input signal power. In other words, a power amplifier amplifies the power of the input signal which is why these types of amplifier circuits are used in audio amplifier output stages to drive loudspeakers.

The power amplifier works on the basic principle of converting the DC power drawn from the power supply into an AC voltage signal delivered to the load. Although the amplification is high the efficiency of the conversion from the DC power supply input to the AC voltage signal output is usually poor.

The perfect or ideal amplifier would give us an efficiency rating of 100% or at least the power “IN” would be equal to the power “OUT”. However, in reality this can never happen as some of the power is lost in the form of heat and also, the amplifier itself consumes power during the amplification process. Then the efficiency of an amplifier is given as:

Amplifier Efficiency

Amplifier Efficiency

Ideal Amplifier

We can know specify the characteristics for an ideal amplifier from our discussion above with regards to its Gain, meaning voltage gain:

  • The amplifiers gain, ( A ) should remain constant for varying values of input signal.
  • Gain is not be affected by frequency. Signals of all frequencies must be amplified by exactly the same amount.
  • The amplifiers gain must not add noise to the output signal. It should remove any noise that is already exists in the input signal.
  • The amplifiers gain should not be affected by changes in temperature giving good temperature stability.
  • The gain of the amplifier must remain stable over long periods of time.

Amplifier Classes

The classification of an amplifier as either a voltage or a power amplifier is made by comparing the characteristics of the input and output signals by measuring the amount of time in relation to the input signal that the current flows in the output circuit. We saw in the Common Emitter transistor tutorial that for the transistor to operate within its “Active Region” some form of “Base Biasing” was required. This small Base Bias voltage added to the input signal allowed the transistor to reproduce the full input waveform at its output with no loss of signal.

However, by altering the position of this Base bias voltage, it is possible to operate an amplifier in an amplification mode other than that for full waveform reproduction. With the introduction to the amplifier of a Base bias voltage, different operating ranges and modes of operation can be obtained which are categorized according to their classification. These various mode of operation are better known as Amplifier Class.

Audio power amplifiers are classified in an alphabetical order according to their circuit configurations and mode of operation. Amplifiers are designated by different classes of operation such as class “A”, class “B”, class “C”, class “AB”, etc. These different Amplifier Classes range from a near linear output but with low efficiency to a non-linear output but with a high efficiency.

No one class of operation is “better” or “worse” than any other class with the type of operation being determined by the use of the amplifying circuit. There are typical maximum efficiencies for the various types or class of amplifier, with the most commonly used being:

  • • Class A Amplifier   –   has low efficiency of less than 40% but good signal reproduction and linearity.
  • • Class B Amplifier   –   is twice as efficient as class A amplifiers with a maximum theoretical efficiency of about 70% because the amplifying device only conducts (and uses power) for half of the input signal.
  • • Class AB Amplifier   –   has an efficiency rating between that of Class A and Class B but poorer signal reproduction than class A amplifiers.
  • • Class C Amplifier   –   is the most inefficient amplifier class as only a very small portion of the input signal is amplified therefore the output signal bears very little resemblance to the input signal. Class C amplifiers have the worst signal reproduction.

Class A Amplifier Operation

Class A Amplifier operation is where the entire input signal waveform is faithfully reproduced at the amplifiers output as the transistor is perfectly biased within its active region, thereby never reaching either of its Cut-off or Saturation regions. This then results in the AC input signal being perfectly “centered” between the amplifiers upper and lower signal limits as shown below.

Class A Output Waveform

class-A amplifier waveform

 

In this configuration, the Class A amplifier uses the same transistor for both halves of the output waveform and due to its biasing arrangement the output transistor always has current flowing through it, even if there is no input signal. In other words the output transistors never turns “OFF”. This results in the class A type of operation being very inefficient as its conversion of the DC supply power to the AC signal power delivered to the load is usually very low.

Generally, the output transistor of a Class A amplifier gets very hot even when there is no input signal present so some form of heat sinking is required. The DC current flowing through the output transistor (Ic) when there is no output signal will be equal to the current flowing through the load. Then a Class A amplifier is very inefficient as most of the DC power is converted to heat.

Class B Amplifier Operation

Unlike the Class A amplifier mode of operation above that uses a single transistor for its output power stage, the Class B Amplifier uses two complimentary transistors (either an NPN and a PNP or a NMOS and a PMOS) for each half of the output waveform. One transistor conducts for one-half of the signal waveform while the other conducts for the other or opposite half of the signal waveform. This means that each transistor spends half of its time in the active region and half its time in the cut-off region thereby amplifying only 50% of the input signal.

Class B operation has no direct DC bias voltage like the class A amplifier, but instead the transistor only conducts when the input signal is greater than the base-emitter voltage and for silicon devices is about 0.7v. Therefore, at zero input there is zero output. This then results in only half the input signal being presented at the amplifiers output giving a greater amount of amplifier efficiency as shown below.

Class B Output Waveform

class-B amplifier waveform

 

In a class B amplifier, no DC current is used to bias the transistors, so for the output transistors to start to conduct each half of the waveform, both positive and negative, they need the base-emitter voltage Vbe to be greater than the 0.7v required for a bipolar transistor to start conducting.

Then the lower part of the output waveform which is below this 0.7v window will not be reproduced accurately resulting in a distorted area of the output waveform as one transistor turns “OFF” waiting for the other to turn back “ON”. The result is that there is a small part of the output waveform at the zero voltage cross over point which will be distorted. This type of distortion is called Crossover Distortion and is looked at later on in this section.

Class AB Amplifier Operation

The Class AB Amplifier is a compromise between the Class A and the Class B configurations above. While Class AB operation still uses two complementary transistors in its output stage a very small biasing voltage is applied to the Base of the transistor to bias it close to the Cut-off region when no input signal is present.

An input signal will cause the transistor to operate as normal in its Active region thereby eliminating any crossover distortion which is present in class B configurations. A small Collector current will flow when there is no input signal but it is much less than that for the Class A amplifier configuration. This means then that the transistor will be “ON” for more than half a cycle of the waveform. This type of amplifier configuration improves both the efficiency and linearity of the amplifier circuit compared to a pure Class A configuration.

Class AB Output Waveform

class AB amplifier waveform

 

The class of operation for an amplifier is very important and is based on the amount of transistor bias required for operation as well as the amplitude required for the input signal. Amplifier classification takes into account the portion of the input signal in which the transistor conducts as well as determining both the efficiency and the amount of power that the switching transistor both consumes and dissipates in the form of wasted heat. Then we can make a comparison between the most common types of amplifier classifications in the following table.

Power Amplifier Classes

Class A B C AB
Conduction
Angle
360o 180o Less than 90o 180 to 360o
Position of
the Q-point
Centre Point of
the Load Line
Exactly on the
X-axis
Below the
X-axis
In between the
X-axis and the
Centre Load Line
Overall
Efficiency
Poor
25 to 30%
Better
70 to 80%
Higher
than 80%
Better than A
but less than B
50 to 70%
Signal
Distortion
None if Correctly
Biased
At the X-axis
Crossover Point
Large Amounts Small Amounts

Badly designed amplifiers especially the Class “A” types may also require larger power transistors, more expensive heat sinks, cooling fans, or even an increase in the size of the power supply required to deliver the extra power required by the amplifier. Power converted into heat from transistors, resistors or any other component for that matter, makes any electronic circuit inefficient and will result in the premature failure of the device.

So why use a Class A amplifier if its efficiency is less than 40% compared to a Class B amplifier that has a higher efficiency rating of over 70%. Basically, a Class A amplifier gives a much more linear output meaning that it has, Linearity over a larger frequency response even if it does consume large amounts of DC power.

In this Introduction to the Amplifier tutorial, we have seen that there are different types of amplifier circuit each with its own advantages and disadvantages. In the next tutorial about Amplifiers we will look at the most commonly connected type of transistor amplifier circuit, the Common Emitter Amplifier. Most transistor amplifiers are of the Common Emitter or CE type circuit due to their large gains in voltage, current and power as well as their excellent input/output characteristics.


 

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21 Responses to “Introduction to the Amplifier”

  1. Johanus Dagius

    I see that you “corrected” the Class C blurb to read “most inefficient“. That’s wrong.

    As your table above still correctly shows, class C amplifiers are among the most “efficient” of all, approaching 100%, but are highly “non-linear” so cannot be used for audio signal amplification. Used exclusively for RF amplification of constant amplitude carrier signals.

    So your blurb should read:
    “• Class C Amplifier – is the most efficient amplifier class because only a very small portion of the input signal is required to be amplified. So it is not linear, and can only be used to amplify sinusoidal RF signals (CW and FM), not amplitude modulated (AM and SSB) audio signals.

    Actually, you h

    Reply
  2. Dipen

    I want to design amplifier for 80db around. My frequency is 235Khz and amplitude 2 to 50mV around. so please give me design tips for cascading amplifier and selection of part No.

    Reply
  3. Ciprian

    You said that “Class C Amplifier – is the most inefficient amplifier class as only a very small portion of the input signal is amplified”.

    I don’t agree with that ! I think you had a misspelling or something. Class C is the most efficient in terms of power transfer (from the power supply to the load) and has the worst signal distorsions.

    Regards,
    Ciprian
    http://www.hobbytronica.eu

    Reply
    • Wayne Storr

      For a Class-C amplifier, the Q point of the characteristics curve is set well beyond cut-off and as such the transistor conducts for less than 180degs (less than 50% compared to Class-A). The conversion efficiency can theoretically reach 100% but the distortion is very high and as such cannot be used as normal audio amplifiers because of the high distortion. As a result Class-C amplifiers are mainly used in radio frequency (RF) circuits where an additional resonant circuit may be used to filter the output waveform.

      Reply
  4. jay

    hello, I would like to ask about the signal output for Class A amps, isn’t it 180 degrees out of phase?

    Reply
    • Wayne Storr

      Hello Jay, for a single stage common emitter amplifier the output signal would indeed by inverted by 180 degs compared to the input signal.

      Reply
  5. John

    Sir I need some advice on connecting speakers to different amplifiers.
    I have this issue ie. I constructed an 1/2watt amplifier using the lm386 chip
    As per :
    http://hackaweek.com/hacks/?p=131
    Now when I tried to connect a 2.7 ohm – 3 watt speaker to it I’m not getting a clear sound. After trying different capacitor values at input and at output and I couldn’t achieve a clarity obtained from a 4ohm speaker.
    I’m poor at electronics and I’m learning…..
    Please help me with this ie determining and matching impudences of speakers.
    Thanking you.

    Reply
  6. ramesh

    sir please explain this doubt
    in my home if all appliances are off except one 100w bulb and in that streetfrom power generation line, one transformer(step down) is connected to 10 houses and all houses are also not drawing any current (ie they went to vacation).so literally 11 kw transformer is connected to one bulb ,but bulb or fuse is not blown in this circumstances .i want to ask why?because only one load is connected to transformer and it should draw all current because voltage is constant(network analysis).please explain .thank you

    Reply
    • Wayne Storr

      I don’t see what relevance this has to Amplifiers but anyway, 11kW is the maximum rated value of the transformer, true that if no load is connected to its secondary then there will be no current drawn but secondary voltage will still be present. Likewise, if the secondary is shorted there would be no voltage but maximum current.

      When you open a tap in your house does ALL the water in the mains pipework come out of the tap, NO!, only the amount you need. So if only one 100W lamp is connected then the transformer supplies ONLY 100W of power and the remainder is unused.

      Reply
    • Jay

      Ramesh, you need to understand about current and power. If your bulb is 100W (say 100V), then it DRAWS 1A current (W=VI). If the transformer is 11KW (say 100V again), it is CAPABLE of delivering 110A current. But this 110A current is delivered when it is DEMANDED only! not always. When your bulb connected to this transformer, it draws only 1A current ONLY. The transformer will not PUSH currents to the bulb. It just delivered what requested.

      But on the otherhand, if you try to drain more than 110A current from this transformer, which is above its capacity, there may be voltage drop, excess heat generation and destruction of the Transformer.

      Let me give an example; you have a 100ml cup and 11000ml container full of juice. what your cup fills to it at a time is 100ml and no matter how hard the container begs, it can not force the cup to take more than 100ml at a time. But it is always good (if you can manage) to have a big container, so you can fill more cups at the same time.

      Hope you got your answer.

      Reply
  7. Shilpa Rajan

    Wayne,

    Please check : Class C Amplifier

    • Class C Amplifier – is the most efficient amplifier class as only a very small portion of the input signal is amplified therefore the output signal bears very little resemblance to the input signal. Class C amplifiers have the worst signal reproduction.

    Would you like to change the word “efficient” to “inefficient” in the above paragraph?

    Thanks

    Reply
  8. Shilpa Rajan

    Hi Wayne,

    Would you like to consider adding Class D amps as well?

    Thanks!

    Reply
  9. Ricky

    this is very useful work.
    but what is the purpose of the two diodes in the class AB amplifier and the the purpose of the capacitor
    thank you for the good work.

    Reply
  10. Satyaban Ukil

    Sir I am an old man of 55 have a very simple and basic request which is how to read a schematic step by step. That is first from which way the current is moving and through which component and finally where it goes. Does it flow to all the components at a time and one after another. If illustrations are given then it should help me a lot as I find great differences between the schematic layout and component layout on a breadboard or PCB. Thanks and Regards

    Regards
    Satyaban
    satyaukil@gmail.com

    Reply

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