current electricity - schoolphysics · 2012. 1. 22. · current electricity. resistance....
TRANSCRIPT
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Current Electricity
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Resistance
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Resistivity
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E.M.F and internal resistance
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Potential round a circuit
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Potential and energy
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Free electron motion in a wireThe free electrons in a metal have three distinct velocities associated with them:(a) a random velocity ( about 105 ms-1)(b) a velocity with which electrical energy is transferred along the wire (about 108 ms-1)(c) a drift velocity of the electrons as a whole when a current flows through the wire(this depends on the applied voltage but is usually a few mms-1 for currents of a fewamps in normal connecting leads).
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Potential divider
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Charge flow and electric current
• Electric charge in a solid is carried by particles called electrons. One electron has a very tiny charge and so for practical measurement of electric charge we use units called COULOMBS.
• A coulomb (C) is an AMOUNT of electric charge in just the same way that a litre is an AMOUNT of water.
• One coulomb is the charge of roughly six million million million electrons!
• The movement of this charge round a circuit is called the electric current.
• Electric current is the rate of flow of charge round a circuit. The current at a point in the circuit is the amount of charge that passes that point in one second.
• A current of 1 A is flowing in a circuit if a charge of 1 coulomb passes any point in the circuit every second.
• Electric current is measured in AMPERES (AMPS, symbol A).
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Kirchhoff’s rules (1)
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Kirchhoff's rules 2
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Resistors in series and parallelResistors in series
The current (I) flowing through R1 and R2 is the same and so the potential differencesacross them are V1 = IR1 and V2 = IR2
Resistors in series: R = R1 + R2
Resistors in parallel:
The potential difference (V) across each of the two resistors is the same, and the current(I) flowing into junction A is equal to the sum of the currents in the two branches.
Resistors in parallel: 1/R = 1/R1 + 1/R2
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Resistance networks (1)Twelve resistors in the form of a cube.
The problem is to find the resistance (R) between the points A and B on each cube. Each arm of the cube has a resistance r.
We can take any path through the network between the points A and B. Such a path could be ACDB.
IR = i/3 r + i/6 r + i/3 r = I 5/6 r Therefore: Total resistance (R) = 5/6 r
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Resistance and temperature
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Electrical power
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Electrical symbols
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Resistance and Ohm’s Law
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Variable resistor (rheostat)
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Series and parallel circuits
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Electrical energy
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Current and electron flow