lecture 0 intro to devices

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Introduction to Power Electronic Devices Power Converters Dr. U. T. Shami Lecture -1

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Page 1: Lecture 0 Intro to Devices

Introduction to Power Electronic Devices

Power Converters

Dr. U. T. Shami

Lecture -1

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Reference of Slide Contents

Reading material of the slides presented in this lecture can be found from the following books:

Chapter -2 and 3ofPower ElectronicsConverters and Regulators (Third Edition)ByBranko L. Dokić • Branko Blanuša

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Diodes and TransistorsIn power electronic circuits of the pulse DC/DC or DC/AC voltage converters, the switching elements are transistors (bipolar and unipolar) and diodes.

In the analysis of a basic circuit, transistors and diodes have been considered as ideal switches (zero on resistance, infinite off-resistance, and instantaneous transition from one state to the other).

However, they are not ideal switches but have real parameters, in both the static and dynamic modes of operation.

The influence of these parameters on the characteristics of pulse converters is considerable, particularly on the efficiency factor.

For this reason, in this chapter, a description is given of the basic switching characteristics of transistors (bipolar and unipolar) and diodes.

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Diode as a SwitchThe static characteristic of a p-n junction diode is nonlinear and is determined by

where Is is the reverse saturation current, md is the correction factor (md = 2 for small currents—in the vicinity of the knee of the characteristic and md = 1 at higher currents), ϕt is the temperature potential.The static characteristic consistsof three regions:

conduction region (low-resistance),

cut off (high-resistance),

Breakdown region.

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Diode as a SwitchA diode can be used as a switch because its resistance can be controlled by the applied voltage.

When a diode is forward biased and if Vd > VDt, where VDt is the conduction threshold voltage, the diode is on (conducting). Then its resistance is small (from 10 to 100 Ω). Since the threshold voltage of Si diodes is VDt = (0.5–0.6) V, in the conduction region Vd mϕt, and exp(Vd/mdϕt) 1, so the current ≫ ≫is

where IDQ is the diode current at the quiescent operating point Q. Any increase of the diode current IDQ decreases the dynamic resistance. For instance, for IDQ = 1 mA, rd = 26 Ω and for IDQ = 26 mA, rd = 1 Ω. It has been assumed that ϕt = 26 mV and md = 1.

It should be emphasized that rd is the p-n junction resistance.

The dynamic diode resistance is

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A conducting diode can be approximated, with a satisfactory accuracy, by a straight line of the slope determined by RD and a voltage source VDt

Diode as a Switch

On the other hand, in the majority of diode applications as a switch, the resistance of the driving circuit, which determines the current IDQ in the quiescent operating point Q, is much higher than RD so that the voltage variation across the diode is negligible.

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Diode as a SwitchWhen a diode is reverse biased, i.e., VAK < 0, and if |VAK| > mdφt, then exp(VD/mdφt) 1 and the current through the diode is equal to the reverse ≪saturation current IDF = −IS. Namely, already at VAK = −0.2 V from (2.1) it follows that ID = −0.98IS. This means that at very small reverse voltages the cathode-anode current is saturated at −IS.

At reverse bias, the concentration of charge carriers in the depleted region drops well below the equilibrium concentration. Consequently, recombination is decreased and generation prevails. Owing to the generation of electron–hole pairs a reverse current proportional to the volume of the depleted region Sd and the rate of generation of pairs G = ni/(2τo) arises, i.e.,

where S is the p-n junction area, d is the width of the transition region, ni is theintrinsic concentration of free charge carriers, τ0 is the lifetime of carriers in thetransition region.

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2.1.1 The Temperature CharacteristicsThe basic static parameters of a diode as a switch are the reverse current IR when diode is not conducting and the forward bias voltage VD when it is conducting. In many applications the temperature sensitivities of these parameters are of considerable influence on the temperature sensitivities of the functional parameters of the circuits incorporating diodes.

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2.1.1 The Temperature Characteristics

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2.1.2 Dynamic Diode Characteristics

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2.1.3 Schottky Diodes

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2.2 Bipolar Transistor as a Switch

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2.2.1 The Cut Off Region

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2.2.2 The Saturation Region

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2.2.2 The Saturation Region

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2.2.2 The Saturation Region

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2.2.2 The Saturation Region

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2.2.3 Static Transfer Characteristic

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2.2.3 Static Transfer Characteristic

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2.2.4.1 Transistor Turn On

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2.2.4.1 Transistor Turn OFF

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2.2.4.3 Optimum Drive

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2.2.4.4 Speed Up Capacitor

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2.2.5 Non-saturated Switch

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2.2.5 Non-saturated Switch

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Explanation of BAKERS clamp

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2.2.5 Non-saturated Switch

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BAKERS Clamp

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BAKERS Clamp: Application

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2.2.7 Inductively Loaded Switch

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2.2.7.1 Transistor Protection

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2.2.7.1 Transistor Protection

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2.2.7.1 Transistor Protection

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2.2.7.1 Transistor Protection

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