WHAT IS CURRENT? • • • • • • • Electrons are charge carriers Unit of charge is the Coulomb (C) Current is the rate of flow of charge 1C of negative charge = total charge carried by 6.242×1018 electrons Charge of 1 electron = 1/ 6.242×1018 = 1.6×10-19C Charge can either be positive or negative Electric current exists when there is a net transfer of charge in a material. For example: If you inject electrons into a copper wire, they travel through the wire and emerge at the other end → current in the wire • Current = rate at which charge is transferred • Unit of Current = Ampere (Amp) • 1A = rate of flow of charge of 1C in 1 second i.e. • Current (I) = Charge (Q) / Time (s) 1. Current, Voltage and Resistance 1 WHAT IS VOLTAGE? • • • • • • • • To establish a flow of charge through a conductor, we need to exert a force on the electrons that carry the charge This is called electromotive force (emf) To sustain flow, electrons need a destination such as the positive and negative terminals of a battery Unit of EMF is the volt Named after Alessandra Volta The greater the voltage of a source of EMF, the greater the current it can produce EMF is also called electric potential, which is the same as talking about the ability (potential) of a voltage source to produce current We say E volts across the voltage source or component Symbol for voltage source and its terminals + • _ 1. Current, Voltage and Resistance 2 WHAT IS RESISTANCE? • • • • • • • • • It is the measure to the extent to which a material interferes with, or resists, the flow of current through it A conductor (metals) has small resistance, an insulator (rubber, wood) has high resistance Semi-conductors (e.g. silicon) not as conductive as metals, more conductive than insulators – form the basis for modern electronic devices such as diodes, transistors and integrated circuits Unit of resistance is the Ohm (George Ohm) - R The symbol of the Ohm is Ω For a perfect conductor, its resistance is 0 Ω A perfect insulator has a resistance of ∞ Ω Conventional current needs a complete path to flow There must be a destination that will accept electrons, and there must also be a source of electrons E + - I R 1. Current, Voltage and Resistance 3 RESISTIVITY • Resistance of a material depends on its length l, cross sectional area A, and its resistivity ρ which is dependent on the material R=ρ • • • l A Good conductors have low resistivity. Poor conductors have high resistivity. Example Find the resistance of 6.5m of wire with a diameter of 0.6mm, and a resistivity of 430nΩm. Example Find the diameter of a wire with resistivity of 50nΩm needed for a resistance of 15Ω. 1. Current, Voltage and Resistance 4 LINEARITY • • • • An electrical device is linear if its V v I graph is a straight line Many circuit analysis techniques can only be applied to circuits composed of linear devices, such as resistors. Graph of a linear component such as a resistor, where the gradient ∆V / ∆I = R The voltage across a device is directly proportional to the current through it V ∆V / ∆I = R I 1. Current, Voltage and Resistance 5 OHM’S LAW • • • • • • • The greater the voltage at a source, the greater the current it can produce Current produced in a resistor is directly proportional to the voltage of the source Resistance reduces the flow of current Current is inversely proportional to resistance, i.e. the greater the resistance, the less the current For a fixed resistance R, the current I increases with an increase in the voltage V at the source This is Ohm’s Law, which is a linear relationship V = IR; I = V/R; R = V/I V + 24V - I 8Ω ∆V /∆I = R I Question: How much voltage is necessary to create a flow of 0.24C in 0.8s through a resistance of 500 Ω? 1. Current, Voltage and Resistance 6 THE VOLTMETER • • • • • Used to measure voltage across a component Always connected in parallel to a component The voltmeter in the first three circuits will always read 6V The voltmeter in the forth circuit reads -6V Voltmeters have black (negative or common) and red (positive) terminals + 6V + V - + 6V + V R - - + 6V + - R V - 6V + - R V + 1. Current, Voltage and Resistance 7 THE AMMETER • • • Used to measure current To measure current flowing in a resistance, you must disconnect the resistance and insert the ammeter in such a way so that all the current flowing in the resistance also flows through the ammeter, i.e. in series with the resistance The ammeter in these circuits will read 3A + 3A 24V 8Ω - 8Ω + + 24V A - - + A + 24V - 8Ω 1. Current, Voltage and Resistance 8 MULTIMETERS • In the lab, multimeters are used to carry out measurements of voltage, current and resistance – depending on the mode selected Ammeter connections mA/20A range Voltmeter/resistance measurement connection Ground connection – return path back to multimeter 1. Current, Voltage and Resistance 9