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Engineering Science EAB_S_127 Electricity Chapter 1
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Electrical Energy Energy cannot be created or destroyed, however, it may be converted from one form into another. In the next four lectures we are going to investigate electrical energy and its application, from basic concepts to electric circuits. A cell is a device that can generate electricity, more precisely, it is a device that converts stored chemical energy into electrical energy An electrolyte causes EMF or Voltage to appear across the terminals of the cell
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Conventional Current In reality the flow of current relates to the movement of charged particles (i.e. electrons) which are in fact negatively charged through conductive material (e.g. metal wires) However, historically scientists have considered the flow of current from high to low potential (voltage) This is considered “Conventional Current” and most scientists and engineers use this and not “electron flow”.
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Charge and Voltage Cells have two principle parameters, the Charge stored, Q and the terminal Voltage, V. Charge is measured in Coulombs [C] Voltage is measured in Volts [V] Voltage is the Energy Stored per Coulomb of Charge Where W = Energy Stored in Joules [ J ] and Q = Charge Example: A cell uses 1500 Joules of energy to generate 1000 Coulombs of charge, what is its voltage?
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Current and Charge The smallest charge is a single electron which has 1.6x10 -19 Coulombs The rate of flow of electrical charge is termed ‘Current’ Where Q = Charge [C] and t = time [s] Current is measured in Amps [A] Example: If 1000C of electrons travel through a wire in 100s, what is the current in A and mA?
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Resistance Resistance is the property of a material to “resist” the flow of current Conductors have low resistivity per unit area Insulators have high resistivity per unit area The flow of current through a resistive material causes a potential difference (or voltage) to develop across it Fixed external resistors are very useful circuit components and are made from materials with a known resistivity per unit area
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Voltage Divider Example Given that V = 10 and the voltage at V B = 3 what are the voltages V AB and V BC ? A + V=10V - C V BC VCVC Figure for Question 1.2 A cell and two resistors in series I VBVB B V AB VBVB VAVA
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Electrical Power Electrical power, P, is given by the amount of electrical energy converted (or absorbed) per unit time in Watts [W] Hence Where E = Energy [ J] absorbed, t = time [s], Q = Charge [C] and I = Current [A] Example: A DC motor consumes 2000J of electrical energy per second when it is in use. Find: a) the power consumed by the motor b) given that the motor requires 200V to operate deduce the electric current flowing through the motor.
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Internal Resistance of Cells All the materials inside cells have some resistance The resistance inside a cell is called its “internal resistance”, this is denoted by r, and causes a voltage loss when loaded by an external resistance + V - External resistor, R r VRVR VLVL I +- +-
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Internal Resistance and Voltage Drop Example: A cell V has an internal voltage 1.8 V and the lost voltage V L is 0.3 V (dropped across its internal resistance). What is the terminal voltage V across an external resistor? + V =1.8V - External resistor, R r VRVR V L =0.3V I +- +-
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Connecting Cells in Series In order for cells to be connected in series the positive terminal of Cell 1 must connect to the negative terminal of Cell 2 The voltage across Cell 1 V BC = 15 V, and the voltage across Cell 2 is V AB = 15 V. If we set V C = 0, then the voltage across two cells V AC is? Figure 1.4 Two cells in series Cell 1 VBVB + - + - Cell 2 V AB V BC VCVC VAVA
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Connecting Cells in Parallel In practice two (or more) cells with the same voltage can be connected in parallel The voltage across the connected cells is the same as that across any single one of them The current available from the connected cells is then multiplied by the number of cells (as the internal resistance is effectively reduced)
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