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applied physics uos first lecture
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PHYS-101 Applied Physics Credit Hours: 03 Basic Electronics Solid State by B.L Therraja Course Content:
1. Zero Reference Level, Chassis Ground, Ohm‘s Law, Formula Variations of Ohm‘s Law, Graphical Representation of Ohm‘s Law, Linear Resistor, Non Linear Resistor, Cells in Series and Parallel.[Ch 1] 2. Resistive Circuits. [Ch 2] 3. Resistors (5.1-15), Inductors (5.19-21) Capacitors (5.35-48) .[Ch 5] 4. Energy Sources. [Ch 6] 5. Magnetism and electromagnetism [Ch 7]. 6. Solid State. Atomic structure, Electron distribution of different atoms, Energy bands in solids, Bonds in solids, Conduction in solids, Conductors, Semiconductors and types of semiconductors, Insulators, Majority and Minority charge carriers, Mobile charge carriers and immobile ions, Drift current in good conductors. [Ch 12] 7. P-N Junction. Formation of depletion layer, Junction or barrier voltage, Forward biased P-N Junction, Forward V/I Characteristics, Reverse biased P-N Junction, Re-verse Saturation Current, Reverse V/I Characteristics, Junction breakdown, Junction Capacitance. [Ch 13] 8. Optoelectronics Devices. Spectral response of human eye, Light Emitting Diode (LED), Photo- emissive Devices, Photomultiplier Tube, Photovoltaic Devices, Bulk type Photoconductive cells, Photodiodes, P-N junction Photodiode, PIN Photodiode, and Avalanche Photodiode. [Ch 16] 9. DC Power Supplies. Unregulated and Regulated Power Supply, Steady and Pulsating DC Voltages, Rectifiers (17.5-17.8), Filters (17.9-17.2), Voltage Multipliers (17.24-17.30), Silicon Controlled Rectifier SCR (17.33-17.37) [Ch 17] 10. The Basic Transistor. Transistor Biasing, Transistor Circuit Configuration. [Ch 18] 11. Modulation and Demodulation. Carrier Waves, Modulation, Demodulation or Detection, Comparison between Amplitude Modulation (AM) and Frequency Modulation (FM). [Ch 30] 12. Integrated Circuits. Advantages of ICs and Drawbacks of ICs, Scale of Integration, Classification of ICs by function, Linear and Digital Integrated Circuits, IC Terminology, Fabrication of IC Components, Popular Application of ICs, Operational Amplifier. [Ch 31] 13. Fiber Optics. Structure of Optical Fibers, Classification of Optical Fibers, Fiber Characteristics, Choice of Wavelength, Optical Fiber cable, Application of Fiber Optic Communication. [Ch 38] Zero Reference Level In electronic circuits, the measurement of the Voltage or Electro Motive Force can only be done with relative to a reference level or reference point. For example, when we say a Battery is of 3V means the difference in the Voltage or EMF of the positive terminal to the Zero Reference Level which is the negative terminal normally is 3V voltage as shown in the figure. The following fig below show that the voltage at point C is 12 V, the voltage at point B is 6 V and at point A is 0V (ZRL).
Chassis Ground in Circuits: It is a common practice to mount electronic components to a conducting metal sheet or a non-conducting plastic board with printed wires (Printed Circuit Board – PCB). When the chassis or PCB is used for building the circuit it is a common practice to regard the conducting body of the chassis or PCB as the common ground. The following symbols are used. Chassis grounding makes the return of current easier and efficient, because chassis is a good conductor it provides a good path for the return of current from various components in a circuit. As the chassis is grounded so it is considered to be in Zero Reference Level and all voltage measurements in the circuit are done with respect to the chassis. Example Voltage Source There are two types of voltage sources, D.C and A.C. Battery is the D.C voltage source and generator is an A.C source.
Resistance is the opposition to flow of current, represented by R. Ohm’s Law Georg Ohm found that, at a constant temperature, the electrical current flowing through a fixed linear resistance is directly proportional to the voltage applied across it, and also inversely proportional to the resistance. This relationship between the Voltage, Current and Resistance forms the basis of Ohms Law and is shown below. Ohms Law Relationship By knowing any two values of the Voltage, Current or Resistance quantities we can use Ohms Law to find the third missing value. Ohms Law is used extensively in electronics formulas and calculations so it is “very important to understand and accurately remember these formulas”. To find the Voltage, (V) V=Ix RV(volts)=I(amps)x R(Ω)) To find the Current, (I) I=V ÷ RI(amps)=V(volts)÷R(Ω)) To find the Resistance, (R) R=V ÷ IR(Ω))=V(volts)÷I(amps) The three quantities of V, I and R have been superimposed into a triangle (affectionately called the Ohms Law Triangle ) giving voltage at the top with current and resistance below. This arrangement represents the actual position of each quantity within the Ohms law formulas. Ohms Law Triangle Transposing the standard Ohms Law equation above will give us the following combinations of the same equation:
Graphical representation of Ohm’s law Linear and Non-linear resistors Linear resistors, one whose value remain same i.e. it does not depend on applied voltage. The voltage and current (I-V) characteristics of such a resistor is a straight line.it means the current and voltage are directly proportional. For non-linear resistors voltage and current (V-I) characteristics is not a straight line. The voltage and current values vary depending upon other factors like temperature and light, but they may not be linear. Tungsten filament bulb is the example. Graphical Representation of non-linear resistors.
Cells Cells generate electricity and also derives chemical reactions. One or more electrochemical cells are batteries. Every cell has two terminals namely:
If E is the overall emf of the battery combined with n number cells and E1, E2, E 3 ,
Cells in Parallel Connection Cells are in parallel combination if the current is divided among various cells. In a parallel combination, all the positive terminal are connected together and all the negative terminal are connected together. Such a combination is used when more current is required. In this case the total current is equal to sum of currents of all cells. If emf of each cell is identical, then the emf of the battery combined by n numbers of cells connected in parallel, is equal to the emf of each cell. The resultant internal resistance of the combination is,