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electromotive force
the energy converted into electrical energy from other forms per unit charge in driving a charge round a complete circuit
OR the electrical power supplied by the source per unit current
potential difference
work done per unit charge on moving a positive charge between two points along the path of the current → electrical energy converted into other forms per unit charge passing across two points
conventional current flows from higher to lower potential (opp for electron flow)
current
direct current: flow of charge carriers
when battery connected across ends of conductor, delocalised electrons drift towards positive terminal of battery → produces direct current
electron flow is opposite to direction of conventional current
conventional current (I): rate of flow of positively charged particles
on circuit diagrams, conventional current is indicated
I = Δq/Δt = Ne/Δt
resistance
ratio of potential difference across the conductor to the current flowing through it
due to frequent collisions of drifting electrons with vibrating ions in the lattice
when accelerated by potential difference (electric field), free electrons gain KE, but some energy transferred to ions when collide → electrons slow down, limits current flow
to determine: place ammeter in series to measure current through, voltmeter in parallel to measure pd across
ohm’s law
current through a metallic conductor is directly proportional to the pd across it, IF temperature and other physical conditions are constant
to keep temp constant, immerse in constant temperature water bath
ohmic conductors have constant V/I ratio
heating effect
ohmic @ small current, low temp → R constant, linear constant gradient
non-ohmic @ large current, high temp: lattice ions vibrate more vigorously, collide more frequently with electrons → R increase, V > I
electric power
work done per unit time to move electric charge across potential difference
internal resistance
all sources of emf have internal resistance → some energy used to overcome
ε = I(R+r) = VR + Vr
terminal pd = ε – Ir = IR = VR
electrical energy converted to other forms in one full circuit
VR < ε → lost voltage is pd across r (accounts for loss of efficiency)
treat internal resistor as another resistor in series (constant I)
VR = ε only if ideal cell (r=0) OR circuit is open (I=0)
I-V characteristics of electrical components
ohmic resistor: R constant → gradient constant
filament lamp: I increase, temp increase, R increase → V/I increase so I/V gradient decrease
thermistor: I increase, temp increase, R decrease → V/I decrease so I/V gradient increase
diode: forward biased → exponential graph
negative I, R infinite → I/V = 0
positive I, R = 0, I/V = infinite