Saturday, 9 May 2015

DEFINE CURRENT


Current:

Current can be defined as the motion of charge through a conducting material. The unit of current is
Ampere whilst charge is measured in Coulombs.

Definition of an Ampere:

“The quantity of total charge that passes through an arbitrary cross section of a conducting material per unit second is defined as an Ampere.”
Mathematically,      
                                                                           I=Q/t
or
                                                                            Q=It
where,
Q is the symbol of charge measured in Coulombs (C),I is the current in amperes (A) and t is the time in seconds (s).
The current can also be defined as the rate of charge passing through a point in an electric circuit i.e.
                                                                          I=dQ/dt


A constant current (also known as direct current or DC) is denoted by the symbol I whereas a time-
varying current (also known as alternating current or AC) is represented by the symbol i or  i(t).
Current is always measured through a circuit element.

Figure 2.1 demonstrates the use of an ampere-meter or ammeter in series with a circuit element,
R,to measure the current through it.

Figure 2.1:An ammeter is connected in series to measure current,I, through the element,R.

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DC AMPLIFIERS

Fundamental Specifications:

The fundamental specifications of dc amplifiers are as follows:
  - input/output signal range,
  - offset and offset drift,
  - single or balanced supply,
  - input bias current,
  - open loop gain,
  - integral linearity,
  - voltage and current noise.

DC Amplifier:


As shown in the below diagram, the direct coupled amplifier (DC) is consist of two transistors Q1 and Q2 , a voltage divider base bias resistor network (R1, R2) which is provided on the transistor Q1 base two collector resistors Rc1and Rc2, the transistor Q2 is self biased, we also use tow emitter by pass resistors RE1and RE2. The direct-coupled amplifier is operated with out the using of frequency sensitive component like capacitor, inductor and Transformer etc. The direct coupled amplifier amplify the A.C signal with frequency as low a fraction of Hertz (Hz).

First of all when we applied a +ve half cycle at the I/P of Q1 transistor, which is already biased through the divider bias network. The +ve half cycle forwarded bias the transistor Q1 which start the conduction and give an inverted and amplified O/P  at the collector . As we know that,

VCE= Vcc - IcRc


This amplified -ve signed is provided to the base of Q2 transistor, which is self-bias (because they are connected in cascade condition). The base  of Q2 transistor  is a reversed  and did not  conduct,  the O/P of transistor Q2 is amplified  signal  (inverting to I/P of Q2) when the Q2 did not  conduct and the voltage  drop across collector  emitter  will be zero, therefore  the VCC is equal  to IcRc.

The O/P equal  to the voltage  drop  across the collector  resistors.

Applications:


-Pulse amplifier.
-Differential Amplifier.
-Regulator circuits of electronic power supply.
-Computer circuitry.
-Jet engine control.
-Electronic instruments.
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AC AMPLIFIERS

AC Amplifiers:

Altering of a voltage or current signal size as it is passed through a system is called an amplitude control.An amplifier is a circuit for the amplitude control provision. Except for early relatively inefficient electromechanical amplifiers, electronic amplifier development started with the invention of the vacuum tube.Classes of amplifiers.Amplifiers are classified according to the polarity and properties of the output current or voltage. Their characteristics cover one, two, or four quadrants on the axes plane. The ac amplifiers and dc amplifiers are distinguished. The fundamental specifications of ac amplifiers are listed on their data sheets; usually they include.
- small-signal and large-signal bandwidths,
- voltage and current band noise,
- harmonic distortion level,
- input and output impedances,
- current and voltage gains.
It is common knowledge that amplifiers are divided into some general classes - A, B, C, etc., depending on the type of service in which they are to be used.


A class A amplifier is one which operates in the transistor’s active region so that the output wave shapes of current are practically the same as those of the existing input signal at all times. Fig. 2.9 illustrates the typical transfer graphs of the collector current versus the base current. For the class A amplifier (Fig. 2.9,a), if the input signal is sinusoidal, the output signal is also sinusoidal. Consequently, the low clipping is the main advantage of this mode of operation. For this reason, the amplifiers of such kind are known as linear amplifiers.Low efficiency (30 to 45%) is the main drawback of the class A amplifier. 
For this reason, it is commonly used in low-power applications and preamplifiers.A class B amplifier operates with a negative bias approximately equal to cutoff. Its base voltage is more negative than in the class A amplifier. Therefore, the output current is almost zero when the alternating input signal is removed or negative (Fig. 2.9,b). With a sinusoidal signal applied, the output consists of a series of half-sine waves. A bottom part of this half-wave is distorted, and the border of this distortion is called a cutoff zone.The amplifiers of such kind are known as pulse amplifiers with high clipping. Efficiency of the class B amplifier is higher (45 to 70%) than in the class A amplifier. For this reason, they are used as the balanced output stages. More often, the intermediate class AB is selected, the clipping of which is much less.
A class C amplifier operates with a negative bias essentially less than cutoff. It passes the current during the part of the positive alternation only. The output current has narrow width and its shape distortion is maximal (Fig. 2.9,c). Its high efficiency (70 to 90%) is the primary considerations at radio frequencies higher than 20 kHz. The class C amplifiers are preferable in power amplifiers with resonance load, for example, transmitters.A class D amplifier uses transistors as switches where the only modes are switch on and switch off. It is used in different switching circuits.
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Thursday, 7 May 2015

WHAT IS THYRISTOR ?


Thyristors:

Thyristor name is derived from the Greek “thyra” and means “door”, that is allowing something to pass through. The main group of thyristors is composed by SCR, and others are the special-purpose devices.


Structure:

silicon-controlled rectifier (SCR) consists of a four-layer silicon wafer with three pn junctions.
It has four doped regions, the anode (A), the cathode (C), and the gate (G). The gate is the control lead. The SCR is triggered into conduction by applying a gate-cathode voltage, which causes a specific level of gate current. The device is returned to its non-conducting state by either anode current interruption or forced commutation.When the SCR is turned off, it stays in a non-conducting state until it receives another trigger. Therefore, the SCR can be termed as one operation thyristor-or 
rectifier thyristor.The structure, biasing circuit, and possible symbols of thyristors are shown in Fig. 1.48. First of them displays the anode-side SCR with an  n-gate lead, the second is the cathode-side thyristor with a  p-gate lead, and the last is the most common device. High-voltage high-power thyristors sometimes also have a fourth terminal, called an auxiliary cathode,used for connection to the triggering circuit. This prevents the main circuit from interfering with the gate circuit. 
Thyristors are commonly used in adjustable ac rectifier circuits, especially in power units up to 100 MVA. Their frequency capabilities are not high, in fact lower than 10 kHz. 

Output characteristics:

 Fig. 1.49 illustrates the output curves and idealized output characteristics of a thyristor. The device has two operating regions: non-conducting and conducting. The current–voltage output characteristics for different gate currents show the forward bias. The output characteristic of a 
thyristor in the reverse bias is very similar to the same curve of the diode with a small leakage current.Using the same arguments as for diodes, the thyristor can be represented by the idealized characteristic in analyzing the circuit-desired topologies.

When it is non-conducting, the thyristor operates on the lower line in the forward blocking state (off 
state) with a small leakage current. The thyristor is in off state until no current flows in the gate. The 
short firing pulse below the breakover voltage from the gate driver  triggers the thyristor. This current pulse may be of triangle, rectangle, saw-tooth, or trapezoidal shape.When a thyristor is supplied by ac, the moment of a thyristor firing should be adjusted by shifting the control pulse relative to the starting point of the positive alternation of anode voltage. This delay is called a 
control angle or firing angle.In dc circuits, the use of thyristors is complicated due to their turning on/off.After the pulse of the gate driver is given, the thyristor breaks over and switches along the dashed line to the conducting region. The dashed line in this graph indicates an unstable or temporary condition.The device can have current and voltage values on this line only briefly as it switches between the two stable operating regions. Once turned to the on state and the current higher than the 
holding current,the thyristor remains in this state after the end of the gate pulse.When the thyristor is conducting, it is operating on the upper line. The current (up to thousands of amperes) flows from the anode to the cathode and a small voltage drop (1 to 2 V) exists between them. If the current tries to decrease to less than the holding border, the device switches back to the non-conducting region.
Turning off by gate pulse is impossible. Thyristor turns off when the anode current drops under the 
value of the holding current.


Input characteristics:

Fig. 1.50 illustrates the input characteristics of the thyristor. The curves show the relation between the gate current and the gate voltage. This relation has a broad coherence area with a width that depends on the temperature and design properties of the device.

The gate current has an effect upon the form of the characteristic. The value of the breakover voltage is the function of the gate current. The more is the gate current the lower is the voltage level required to switch on the thyristor. Maximum breakover voltage of a thyristor reaches up to thousands of volts. If the applied voltage exceeds the breakover level, SCR triggers without the gate pulse. This prohibited mode should be avoided.
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DEFINE TRANSISTORS


Transistors:

A transistor regulates current or voltage flow and acts as a switch or gate for electronic signals. A transistor consists of three layers of a semiconductor material, each capable of carrying a current. A semiconductor is a material such as germanium and silicon that conducts electricity in a "semi-enthusiastic" way. It's somewhere between a real conductor such as copper and an insulator (like the plastic wrapped around wires).

The semiconductor material is given special properties by a chemical process called doping. The doping results in a material that either adds extra electrons to the material (which is then called N-type for the extra negative charge carriers) or creates "holes" in the material's crystal structure (which is then called P-type because it results in more positive charge carriers). The transistor's three-layer structure contains an N-type semiconductor layer sandwiched between P-type layers (a PNP configuration) or a P-type layer between N-type layers (an NPN configuration).

A small change in the current or voltage at the inner semiconductor layer (which acts as the control electrode) produces a large, rapid change in the current passing through the entire component. The component can thus act as a switch, opening and closing an electronic gate many times per second. Today's computers use circuitry made with complementary metal oxide semiconductor (CMOS) technology. CMOS uses two complementary transistors per gate (one with N-type material; the other with P-type material). When one transistor is maintaining a logic state, it requires almost no power.

Transistors are the basic elements in integrated circuits (ICs), which consist of very large numbers of transistors interconnected with circuitry and baked into a single silicon microchip or chip.

Common Features of Transistors:

The word “transistor” was coined to describe the operation of a “transfer resistor”. First, a point contact transistor was produced. It included two diodes placed very closely together such that the current in either diode had an important effect upon the current in the other diode. By the proper biasing the diodes, it was possible to obtain power amplification of electric signals between the diode common layer, which lead was called a base,and other layers. One of the leads of this device was designated as an emitter, the corresponding diode was biased in the forward direction, the other was   
a collector and its diode was biased in the reverse direction. Power amplification was obtained by virtue of the fact that the few variations in the base current caused a large variation in the emitter-collector current. The point-contact transistor had certain drawbacks:

- High sensitivity to temperature, either ambient or self-generated;

- Production problems, i.e., a difficulty to reproduce the same electrical qualities in close tolerance for mass production.

-Low amplification, especially at high frequencies.

Intensive research has been done to diminish or remove these drawbacks. As a result, developers have produced semiconductor materials that are not so sensitive to temperature, inexpensive, operate at high frequencies, have low power dissipation, and internal noise of the transistor. A device, which is more stable both mechanically and electrically, has been constructed by forming junctions rather than point contacts. General classes of transistors that are used in electronics today are as follows:


- Bipolar junction transistors (BJT).
- Junction field-effect transistors (JFET).
- Metal-oxide semiconductor field-effect transistors (MOSFET) up to some kilowatts, hundreds amperes, and tenths gigahertz.
- Insulated-gate bipolar transistors (IGBT) up to thousands of kilowatts, some kiloamperes, 
and hundreds kilohertz.

More powerful devices have been built on the thyristors though IGBTs have the potential to  
replace them.

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Wednesday, 6 May 2015

DEFINE ZENER DIODE


Zener diode:

 A Zener diode sometimes called breakdown diode or stabilitrone,is designed to operate in the reverse breakdown, or Zener, region, beyond the peak inverse voltage rating of normal diodes. This reverse breakdown voltage is called the Zener or, reference voltage, which can range between –2,4 V and –200 V (Fig. 1.12). The Zener effect causes a “soft” breakdown whereas the avalanche effect causes a 
sharper turnover. Both effects are used in the Zener diode. The manufacturer predetermines the Zener and avalanche voltages. 


A significant parameter of the Zener diode is the temperature coefficient that is the breakdown voltage deviation during the temperature rise or fall. The temperature coefficient of the Zener diode changes from negative to positive near –6 V. Because of this, by selecting the current value the designer may minimize the instability of the device. In all types of devices, the output levels are affected by variations in the load. Lower percentage values, approaching 0%, indicate better regulation. The Zener diode is the backbone of voltage regulators, circuits that hold the load voltage constant despite the large changes in line voltage and load resistance. When used as a voltage regulator, the Zener diode is reverse biased so that it will operate in the breakdown region with highly stable Zener voltage. In this region, changes in current through the diode have no effect on the voltage across it. The Zener diode establishes a constant voltage across the load within a range of output voltages and currents. Out of this range, the voltage drop remains constant and the current flow through the diode will vary to compensate the changes in load resistance.A power Zener diode is called an avalanche diode.It can withstand kilovolts voltages and currents of some thousands of amperes.
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POWER DIODE AND ITS CHARACTERISTICS


Power Diode:

A power diode is more complicated in structure and operational characteristics than the small-signal 
diode. It is a two-terminal semiconductor device with a relatively large single pn junction, which consists of a two-layer silicon wafer attached to a substantial copper base. The base acts as a heat sink, a support for the enclosure and one of electrical leads of the device. The extra complexity arises from the modifications made to the small-signal device to be adapted for power applications. These features are common for all types of power semiconductor devices.

Characteristics:

In a diode, large currents cause a significant voltage drop. Instead of the conventional exponential output relationship for small-signal diodes, the forward bias characteristic of the power diode is approximately linear. This means the voltage drop is proportional both to the current and to ohmic resistance. The maximum current in the forward bias is a function of the area of the pn junction. 
Today, the rated currents of power diodes are thousands of amperes and the area of the pn junction may be tens of square centimeters. The structure and the method of biasing of a power diode are displayed in Fig. 1.9. The anode is connected to the   layer and the cathode to the p substrate layer n. In the case of power diode, an additional n layer exists between these two layers. This layer termed as a drift region can be quite wide for the diode. The wide lightly doped region adds significant ohmic resistance to the forward-biased diode and causes larger power dissipation in the diode when it is conducting current.

Forward biasing:

 Most power is dissipated in a diode in the forward-biased on-state operation.For small-signal diodes, power dissipation is approximately proportional to the forward current of the diode. For power diodes, this formula is true only with small currents. For large currents, the effect of ohmic resistance must be added. In a high frequency switching operation,significant switching losses will appear when the diode goes from the off-state to the on-state, or vice versa. Real operation currents and voltages of power diodes are essentially restricted due to power losses and the thermal effect of power dissipation. Therefore, in power devices cooling is very important.

Reverse biasing:


In the case of reverse-biased voltage, only the small leakage current flows through the diode. This current is independent of the reverse voltage until the breakdown voltage is reached. After that, the diode voltage remains essentially constant while the current increases dramatically. Only the resistance of the external circuit limits the maximum value of current. Large current at the breakdown voltage operation leads to excessive power dissipation that should quickly destroy the diode. Therefore, the breakdown operation of the diode must be avoided.To obtain a higher value of breakdown voltage, the three measures could be taken. First, to grow the breakdown voltage, lightly doped junctions are required because the breakdown voltage is inversely proportional to the doping density. Second, the drift layer of high voltage diodes must be sufficiently wide. It is possible to have a shorter drift region (at the same breakdown voltage) if the depletion layer is elongated. In this case, the diode is called   a punch-through diode.The third way to obtain higher breakdown voltage is the boundary control of the depletion layer. All of these technological measures will result in the more complex design of power diodes.

Switching:

 For power devices, switching process is the most common operation mode. A power diode requires a finite time interval to switch over from the off state to the on state and backwards. During there transitions, current and voltage in a circuit vary in a wide range. This process is accompanied with energy conversion in the circuit components. A power circuit contains many components that can 
store energy (reactors, capacitors, electric motors, etc.). Their energy level cannot vary instantaneously because the power used is restricted. Therefore, switching properties of power devices are analyzed at a given rate of current change, as shown transients in Fig. 1.10.


The most essential data of power switching are the forward voltage overshoot U(F max) when a diode turns on and the reverse current peak value I(R max) when a diode turns off.

Summary:

Power diode is adapted for switching power applications. In addition to bulk resistance, it has high ohmic resistance. To withstand the essential losses that appear when the diode goes from the off state to the on state and backward, cooling is very important. To obtain a higher value of breakdown voltage, some measures are usually taken, such as lightly doped junctions, sufficiently wide drift layer, and the boundary control of the depletion layer. These measures result in a more complex design of power diodes but shorten the reverse recovery time and increase their lifetime.

Special-Purpose Diodes:

Rectifier diodes are used in the circuits of 50 Hz to 50 kHz frequencies. They are never intentionally 
operated in the breakdown region because this may damage them. They cannot operate properly under abnormal conditions and high frequency. Devices of other types have been developed for such kind of operations.
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