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HolisticTuition Home Form 5 Physics Next > The study of matter 1 End CashPlants Chapter 4: Electronics HolisticTuition Physics: Chapter 4 Home Objectives: (what you will learn) < Back Next > 2 End CashPlants 1) uses of Cathode Ray Oscilloscope 2) understanding semiconductor diodes 3) understanding transistors 4) analysing logic gates HolisticTuition Home Maltese-cross Tube Thermionic emission = emission of electrons from hot metal surface in vacuum Cathode rays = electrons moving at high speeds after acceleration through high potential difference < Back Next > 3 End CashPlants A Maltese-cross tube is used to show the first two properties of cathode rays. Properties: 1. electrons moving at high speeds in straight lines 2. cause fluorescent material to emit light 3. deflected by magnetic field 4. deflected by electric field HolisticTuition Home Maltese-cross Tube “Maltese Cross” Crookes Tube Invented in the 1880s by William Crookes during his investigations into the nature of cathode rays. < Back Next > It demonstrates that radiant matter is blocked by metal objects. 4 End CashPlants The direction of deflection of cathode rays by magnetic field is found with Fleming’s left-hand rule. HolisticTuition Home Cathode Ray Tube The oscilloscope is capable of following changes that occur within billionths of a second. It is widely used throughout industry and in laboratories to test and adjust electronic equipment, and to follow rapid oscillations in electric voltages. < Back Next > 5 End CashPlants The Cathode Ray Tube (CRT) Special converters attached to oscilloscope can convert mechanical vibrations, sound waves, and other forms of oscillatory motion into electrical impulses that can be observed on the face of CRT. HolisticTuition Home Cathode Ray Tube < Back Next > 6 End CashPlants The Cathode Ray Tube (CRT) HolisticTuition Home Cathode Ray Oscilloscope The Cathode Ray Oscilloscope (C.R.O.) is divided into 3 parts: • Electron gun • Deflection system • Fluorescent screen < Back Next > 7 End CashPlants HolisticTuition Home < Back Next > doctronics Cathode Ray Oscilloscope Electron gun: • The cathode emits electrons when heated • The grid controls the number of electrons reaching anodes – control with brightness knob • The anode focus electrons into fine beam – control with focus knob • The potential difference between anode and cathode accelerates electrons to high velocity Deflection system: • Y-plates: electric field deflects electrons vertically • X-plates: electric field deflects electrons horizontally Fluorescent screen: • When fast electrons hit fluorescent screen, their kinetic energy is converted into light – a spot of light is seen on the screen • The walls of C.R.O. after anode is coated with graphite and grounded to keep out external electric field Kinetic energy of electrons emerging from anode = eV ½ mv2 = eV 8 End CashPlants Velocity, v = 2eV m where e = charge of electron, m = mass of electron HolisticTuition Home Cathode Ray Oscilloscope Uses of C.R.O. 1. Measure potential difference • Switch off time-base • Connect voltage to be measured to Y-input • d.c. voltage: if x = deflection of light spot, voltage = xn volts • a.c. voltage: 2 x (peak voltage, V0) = ln < Back r.m.s. voltage, Vrms = Next > V0 √2 1 = √2 ln volts 2 x l 9 End CashPlants Given: Y-sensitivity = n V per division HolisticTuition Home < Back Next > Cathode Ray Oscilloscope 2. Measure short time interval • Switch on time-base; one horizontal division = time interval, T • Pulse A represents sound detected by microphone • Pulse B represents the echo • Say, time interval between A and B is 3 divisions = 3T • If d = distance of wall from microphone Distance travelled 2d Speed of sound, v = = Time taken 3T wall d microphone A B d 3 divisions 10 End CashPlants 3. Display waveform • Connect input voltage to Y-input • Switch on time-base • Adjust frequency to a steady trace formed on screen • The trace or waveform is the graph of voltage V against time t HolisticTuition Semiconductor diodes Home Semiconductors have resistance between that of metals and insulators; e.g. carbons, germanium, silicon Pure semiconductor: negative charge carriers = positive charge carriers or free electrons = holes < Back Next > Doped semiconductor (with added impurity): n-type: free electrons > holes (impurity of valency 5; arsenic or phosphorus) p-type: holes > free electrons (impurity of valency 3, indium or gallium) Semiconductor diode p-n junction p 11 n + End CashPlants structure – band – + symbol – + actual diode HolisticTuition Home Semiconductor diodes Ideal diode • Allows current through when connected in forward bias • Stops current when connected in reverse bias (infinite resistance) < Back Next > + current + 12 Forward bias End CashPlants + no current + Reverse bias HolisticTuition Home Semiconductor diodes A diode is used as a rectifier to convert a.c. to d.c. VD < Back Next > a.c. V R VR Half-wave rectification Current only flows through the diode during the positive half cycle (as shown by +V). 13 End CashPlants The voltage across the load, VR is direct voltage and the current is d.c. HolisticTuition Home Semiconductor diodes A capacitor, C is connected across load, R to smoothen voltage, VR. < Back VD Next > a.c. V C R smoothing capacitor 14 End CashPlants VR HolisticTuition Home Semiconductor diodes 2 diodes are used in a simple full-wave rectification. < Back Next > 4 diodes are used in a bridge full-wave rectification. 15 End CashPlants HolisticTuition Home Transistors Transistor is an electronic device containing at least 3 layers of semiconductor and electrical contacts, used in a circuit as amplifier, detector, or switch. B E B: base Next > End CashPlants Some samples of the actual transistors C B n-p-n transistor < Back 16 C E p-n-p transistor C: collector E: emitter Structure of an n-p-n transistor HolisticTuition Home Transistors Transistor as a current amplifier The base current Ib controls the collector current Ic Ic is many times larger than Ib. When Ib = 0, Ic = 0 < Back Next > When Ib changed, it is amplified by the transistor, producing larger change in Ic. Ic C B µA Ib 17 End CashPlants E mA HolisticTuition Home Transistors Transistor as a switch The transistor can be used as a switch to switch on a lamp, L. The light-dependent resistor (LDR) has resistance of 2 kΩ in bright light and 20 kΩ in the dark. During the day, resistance R1 is much less than resistance R2. So the potential difference across LDR is much smaller than across R2. < Back Next > The base current Ib is small, the collector current Ic is small, and the relay is not activated. The lamp L is off. The reverse happens when in the dark. R1 increases to maximum, potential difference across LDR increases, and Ib increases. The transistor amplifies the increase resulting in large Ic, thus activating relay and lamp L is switched on. 18 End CashPlants Other devices may be used in place of LDR for other functions. HolisticTuition Logic Gates Home Logic gates = switching circuits used in computers and electronic devices A logic gate has one or more inputs but only one output. < Back Next > Its action is summarized by an equation in Boolean algebra, or with a truth table. NOT logic gate It is also called the inverting buffer. Truth table A 19 End CashPlants X Boolean equation X=A Input Output HolisticTuition Logic Gates Home AND and NAND logic gates AND NAND < Back Next > 20 End CashPlants Input A B 0 0 0 0 1 0 1 1 A B A B X=A•B X=A•B Output AND NAND 0•0=0 0=1 0•1=0 0=1 1•0=0 0=1 1•1=1 1=0 Making a NAND gate out of transistors and resistors HolisticTuition Logic Gates Home OR and NOR logic gates OR NOR < Back B A X=A+B X=A+B B Next > 21 A End CashPlants Input A B 0 0 0 1 1 0 1 1 Output OR NOR 0•0=0 0=1 0•1=1 1=0 1•0=1 1=0 1•1=1 1=0 HolisticTuition Summary Home What you have learned: < Back 22 End CashPlants 1. Uses of Cathode Ray Oscilloscope 2. Semiconductor diodes 3. Transistors 4. Logic gates Thank You