1. EGN 3373 Introduction to Electrical Systems I A Systems Approach to Electrical Engineering Graphics Adapted from “Physical, Earth, and Space Science”, Tom Hsu, cpoScience.

2. Objectives: 1.Understand diode operation and select diodes for various applications 2.Use the ideal diode model to analyze nonlinear circuits 3.Analyze and design simple voltage-regulator circuits 4.Use the constant voltage model Application 1.Most common application is rectification (converts ac to dc) e.g. automotive alternator, voltage multipliers, power conversion 2.Voltage protection (voltage spikes) e.g. stepper motor 3.Combination circuits, e.g. logic gates, temperature gauge 4.More diodes - Used to regulate voltage (Zener diodes), electronically tune radio and TV receivers (varactor diodes), generate radio frequency oscillations (tunnel diodes), or produce light (light emitting diodes - LED)Zener diodesvaractor diodesradio frequencyoscillationstunnel diodeslight emitting diodes Chapter 8 - Diodes

3. Solid-State Electronics 3 Electronics – electrical devices and circuits containing active elements capable of controlling the flow of current If current is thought of as the flow of electrons, the name “electronics” makes perfect sense.

4. Solid-State Electronics 4 For many years, the active components in electronic circuits were thermionic devices called vacuum tubes. Vacuum tubes used electric current to heat a metal filament, which gave off free electrons. The negatively-charged electrons traveled through a vacuum to a positively-charged plate.

5. Solid-State Electronics 5 Plate (+) Filament Cathode (-) The filament produces free electrons. They collect on the cathode. The plate, which is more positively- charged than the cathode, will attract the electrons, thus establishing a positive current flow from plate to cathode. Current cannot flow in the opposite direction. This “one-way valve” is called a diode. electrons + current

6. Solid-State Electronics 6 Adding a grid and applying a voltage to it gives additional control capability. This tube is called a triode. Multiple grids give additional versatility (tetrodes, pentodes, etc.) Plate (+) Filament Cathode (-) Grid

7. Solid-State Electronics 7 Today, vacuum tubes are used only for niche applications (such as very high quality audio amplifiers) or where voltages and powers are very high (like radar). Most electronic applications are implemented using devices that operate in the solid state, not the gaseous state.

8. Solid-State Electronics 8 Vacuum tubes work very well, but have some inherent issues: 1.They require LOTS of power to produce the heat needed to liberate free electrons. 2.They can be miniaturized to the size of a small light bulb, but modern devices require miniaturization several THOUSANDS of times smaller than that. 3.Because of the degradation of the filament, their useful life is shorter than we would like.

9. Solid-State Electronics 9 Solid state devices address these issues. 1.Solid-state devices consume small amounts of power. 2.Solid-state devices can be minaturized to a very high degree – millions of devices per square centimeter. 3.Solid-state devices have long lifetimes – for some devices, many tens if not hundreds of years.

10. The P-N Junction 10 Silicon semiconductor crystalline material P-Type silicon doped with impurities containing an excess of positive charge carriers (boron) N-Type silicon doped with impurities containing an excess of negative charge carriers (arsenic)

11. The P-N Junction 11 Depletion or space-charge region keeps p-type and n-type materials separated The voltage built up across the depletion region of silicon is about 0.7 volts. Depletion Region or Space-Charge Region ++++++++++ ----------

12. The P-N Junction 12 Forward-Biased (V A > V K ) VAVA VKVK “Kathode” – German for “cathode” Bias voltage makes depletion region narrower. Current overcomes the barrier voltage and flows from anode to cathode. (Holes flow from left to right; electrons flow from right to left.)

13. The P-N Junction 13 Reverse-Biased (V K > V A ) VAVA VKVK “Kathode” – German for “cathode” Bias voltage makes depletion region wider. Current cannot overcome the barrier voltage so no current flows.

14. The P-N Junction 14 VAVA VKVK “Kathode” – German for “cathode” A single P-N junction forms a diode.

15. This thermionic valve or vacuum tube is known as the diodediode A diode is a two-terminal device. Diodes have two active electrodes. The diode allows an electric current to pass in one direction (forward biased condition) and blocks the current in the opposite direction (the reverse biased condition). Thus, the diode acts like an electronic version of a check valve.check valve Early Diode Structure of a vacuum tube diode Chapter 8 - Diodes

16. The P-N Junction 16 When charge carriers cross the depletion region, they lose energy. The energy loss results in the release of a photon. If the photon has a wavelength in the range of visible light, the diode is a “light-emitting diode” or LED. We can also make infrared, ultraviolet, and laser diodes. The first LED; used today for TV remote controls CD, DVD, and Blu-Ray players

17. Analogy: Diodes allow current from the alternator to charge the battery when the engine is running, but when the engine stops, the diode prevents the battery from discharging. The diode is analogous to a one- way valve in a fluid flow system. The diode allows an electric current to pass in one direction (forward biased condition) and blocks the current in the opposite direction (the reverse biased condition). Chapter 8 - Diodes

18. Linear vs. Non-Linear Elements R, L, C … linear (IV curve) Diodes, transistors … non-linear (IV curve)

19. Diodes – What are they ? Diode or a “p-n” junction Non-linear Semiconductor device

20. Diodes - Applications TYPES … – Light emitting … LED’s (OLEDs) – Photodiodes (solar cells !) – Zener – Tunnel APPLICATIONS – Rectifiers – Voltage regulators – Varactors

21. The diode allows an electric current to pass in one direction (forward biased condition) and blocks the current in the opposite direction (the reverse biased condition). As in the automobile battery after being charged via an alternator. Forward Biased For v D > 0 at small amouts, i D has large value and is the forward current Diode is ON Reverse Biased For v D < 0 i D has very small value almost zero current, and is the reverse current Diode is OFF Diodes

22. The Ideal Diode

23. Ideal Diode Model IDEAL (on-off) DIODE MODEL: – V D > 0 Volts (forward bias); “short-circuit” – V D < 0 Volts (reverse bias): “open-circuit”

24. Ideal Diode – simple model to approximate diode behavior (complex circuits) 1.Perfect conductor with zero voltage drop in the forward direction, v = 0 or SHORT circuit (i D >0 Diode ON) 2. In the reverse direction, the ideal diode is an OPEN circuit, I = 0 (v D <0, Diode OFF) Use when we want a basic understanding of the states, not exact analysis Ideal Diode Model

25. 1.Assume state of Diode, either ON (i.e. SHORT) or OFF (i.e OPEN) 2.Analyze the circuit to determine the current through the diodes assumed to be ON and the voltage across the diodes assumed to be off 3.Check to see if the result is consistent with the assumed state for each diode. Current must flow in the forward direction for diodes assumed to be on. Futhermore, the voltage across the diodes assumed to be off must be positive at the cathode (i.e. reverse bias) 4.If the results are consistent with the assumed states, the analysis is finished. Otherwise, return to step 1 and choose a different combination of diode states. Step by Step Analysis using Ideal Diode Ideal Diode Model

30. R

31. What is the correct assumption for D 3 and D 4 ? Ideal Diode Model

32. The correct assumption is that D 3 is off and D 4 is on. Equivalent Circuit Ideal Diode Model

33. Diode Example Find I for: – R=1 KΩ – R=10 KΩ – Use Ideal diode model

34. Diode Example Find I for: – R=1 KΩ – R=10 KΩ – Use Ideal diode model

35. Constant Voltage Model IDEAL (on-off) DIODE MODEL: – V D > V γ Volts (forward bias); ???? – V D < V γ Volts (reverse bias): “open-circuit” V D =V γ + -

36. Diode Voltage V D = V AK > 0 – … means forward bias – … it also means that V A > V K V D = V AK < 0 – … means reverse bias – … it also means that V A < V K +VD-+VD- A K IDID

37. Diode Example Find I for: – R=1 KΩ – R=10 KΩ – Use constant Voltage model

38. Diode Example Find I for: – R=1 KΩ – R=10 KΩ – Use constant Voltage model

39. Diode Example Find V and I … Use “ideal diode model”

40. Diode Example Find V and I … Use “ideal diode model”

41. Diode Example Find V and I … Use “ideal diode model”

42. Diode Example

44. Zener Diode Used in Voltage regulators Typically operated in “reverse bias” (breakdown region) Designed for “predictable” breakdown voltages

45. Zener Diode Model What are the appropriate “forward and “reverse” bias models ?

46. Application: widely used as voltage references (regulators) and as shunt regulators to regulate the voltage across small circuits. Zener diode continues to conduct when voltage reaches the diode’s reverse breakdown voltage. Predetermined reverse bias breakdown voltage. Zener Diode Zener Diodes operate in the reverse breakdown region with sufficiently large voltage and current of large magnitude. If the power dissipated does not raise the device T too high, operation in this region can occur and is not destructive. Zener Diode Model

47. Zener Diode - Example Find V OUT for all V IN – V BR =5.6 V – V Υ =0.7 V

48. Zener Diode - Example Find V OUT for all V IN – V BR =5.6 V – V Υ =0.7 V

49. AC-DC Conversion Device

50. Subsystem … AC-DC

51. One popular application of the diode: Rectification Rectification is the conversion of alternating current (AC) to direct current (DC) by a device that only allows one-way flow of electrons, exactly like a semiconductor diode does. The simplest kind of rectifier circuit is the half- wave rectifier. It only allows one half of an AC waveform to pass through to the load. (Figure below)below Rectifier Circuits

52. Half-wave rectification is a very simple way to reduce power to a resistive load. Some two-position lamp dimmer switches apply full AC power to the lamp filament for “full” brightness and then half-wave rectify it for a lesser light output. (Figure below) below In the “Dim” switch position, the incandescent lamp receives approximately one- half the power it would normally receive operating on full-wave AC. Because the half-wave rectified power pulses far more rapidly than the filament has time to heat up and cool down, the lamp does not blink. Instead, its filament merely operates at a lesser temperature than normal, providing less light output.

53. Half-Wave Rectifier – with a sinusoidal source and resistive load R L Rectifier Circuits – convert ac to dc When the V s > 0 the diode is in the forward-bias region. If an ideal diode is assumed, V s appears across the load. For actual diode, the output is offset by the turn on voltage across the diode, 0.7V

54. Half-Wave Rectifier – with a sinusoidal source and resistive load R L Rectifier Circuits – convert ac to dc When v s (t) <0, the diode is reverse biased = OFF, no current flows

55. Half-Wave Rectifier Only the POSITIVE HALF-cycles of the v s appear across the load. Important Aspect – Peak Inverse Voltage (PIV) PIV = absolute value of V D min *Breakdown spec. should be > than magnitude of PIV; Here PIV = V m If PIV <V ZK ), then our junction diodes will remain in either forward or reverse bias for all time t. The rectifier will operate “properly”! If ZK PIV > V ZK ), then our junction diodes will breakdown. The rectifier will NOT operate properly!

56. Full-Wave Rectifier

57. Another full-wave rectifier design is built around a four-diode bridge configuration. Full-wave bridge rectifier.

58. Full-Wave Rectifier Current directions for the positive and negative half-cycles for the full-wave bridge rectifier circuit are shown in Figures below. Regardless of the polarity of the input, the current flows in the same direction through the load. That is, the negative half-cycle of source is a positive half-cycle at the load. The current flow is through two diodes in series for both polarities.