# Electric Current

4.0 / 5

- Created by: teague sheldon
- Created on: 28-12-12 20:18

## Charge, Current and Potential Difference

An electric current is defined as the rate at which charged particles pass through a point in a circuit.

- Current is measured in coulombs per second or amperes.
- In metals, the charged particles are electrons which move from the negative to the positive terminals in d.c supply.
- In circuit diagrams, the charged particles move from +ve to -ve, which is known as conventional current.
- Current = change in charge / change in time

1 of 18

## Charge, Current and Potential Difference (cont)

- A potential difference is what makes a current flow.
- A potential difference is the electrical energy transfered/converted per unit of charge passing between 2 points.
- P.D is measured in joules per coulomb, or volts. Potential difference = Energy / Charge.
- A charged particle gains energy when it passes through a cell, and it releases this gained energy when it passes through a component in the circuit.
- Thus both the cell and a component have a p.d across them when charge flows in a circuit.

2 of 18

## Charge, Current and Potential Difference (cont)

- Resistance is the opposition charged particles face when they flow around a circuit.
- The potential difference needed to make a current flow in a circuit depends on the resistance of circuit.
- The bigger the resistance, the more potential difference (energy per coulomb) is required to make a certain current flow.
- Resistance = potential difference / current
- It is measured in ohms.

3 of 18

## Current/Voltage Characteristics

- The effect of varied potential difference on the current through a component can be investigated using a variable p.d cell connected to an ammeter, switch and component in series, with a voltmeter in parallel to the component.
- By varying and recording the supply p.d, a range of current values can be recored for the component.
- The battery is reversed and the supply p.d is varied over the same range.
- An I/V characteristics curve for that component can be plotted from the results.

4 of 18

## Current/Voltage Characteristics (cont)

- In a resistor or wire, a proportional straight line is plotted.
- The proportionality between current and p.d means that the conductor follows Ohm's law.

5 of 18

## Current/Voltage Characteristics (cont)

- For a semiconductor diode, the shape of the graph depends on the direction the current is flowing.
- When the diode is forward biased (facing direction of convectional current), between 0-0.7V the diode offers a large resistance to the current.
- From 0.7V onwards the resistance of the diode falls rapidly and a large current flows, shown by a steep rise in the graph.
- When the diode is reversed biased, the diode offers high resistance until the breakdown voltage, where the diode is destroyed and a large current flows.

6 of 18

## Current/Voltage Characteristics (cont)

7 of 18

## Current/Voltage Characteristics (cont)

- When the p.d across a filament lamp is steadily increased, the graph becomes less and less steep.
- The p.d and the current are not proportional because the increasing current heats the filament lamp.
- An increase in temperature increases the resistance of the filament and so decreases the rate of increase of current with p.d.

8 of 18

## Current/Voltage Characteristics (cont)

9 of 18

## Current/Voltage Characteristics (cont)

- Ohm's law states that the current in a conductor is directly proportional to the p.d across it, provided that the temperature and other physical conditions remain the same.
- A proportional I/V characteristics graph shows that a component obeys Ohm's law (wires and resistors).
- These are called Ohmic conductors, while components that do not obey Ohm's law are called non-Ohmic conductors.

10 of 18

## Resistivity

- The 2 factors that affect the resistance of a conductor are its length and its cross-sectional area.
- Resistance is proportional to length.
- Resistance is inversely proportional to cross-sectional area.
- The resistivity of a conductor=

(cross sectional area x resistance of conductor) / length of conductor. - The resistivity is a constant of the material from which the conductor is made.
- Its units are ohm metres.

11 of 18

## Resistivity (cont)

- Resistivity of a wire can be measured using a battery, a switch, an ammeter, and a 100cm piece of wire under test taped to a ruler, all in series. Add a voltmeter in parallel to the wire on the ruler.
- Record the p.d and current for the full 100cm of wire.
- Vary the length of the wire that it across the voltmeter from 100-30cm, recording the current and votlage throughout.
- Calculate the resistance for each recorded length.

12 of 18

## Resistivity (cont)

- Measure the diameter of the wire using a micrometer, and use this value to calculate the cross-sectional area of the wire.
- Plot resistance against length (y=mx+c).
- The gradient is the resistivity/cross-sectional area, so the resistivity can be calculated.

13 of 18

## Resistivity (cont)

- Temperature always affects conduction, no matter wha the material (conductor, semiconductor ect)
- In conductors, as the temperature increases the resistance increases.
- Metal conductors (wires and resistors) contain +ve ions as well as free electrons. The electrons collide with the ions as they try to carry charge through, causing a resistance.

14 of 18

## Resistivity (cont)

- As temperature increases, the +ve ioons and electrons have more kinetic energy, so the +ve ions vibrate more (greater amplitude), and electrons move faster.
- Both of these increase the number of collisions of the charge carriers with the +ve ions (frequency), so resistance increases.
- The resistance does not change greatly, so in small circuits we consider wires and restitors ohmic conductors.

15 of 18

## Resistivity (cont)

- In a thermistor, the resistance decreases significantly as temperature increases.
- A thermistor is made from semiconductor material and so there are few free electrons to produce a current.
- As temperature increases, extra electrons are released from the semiconductor ions due to increased thermal energy.
- This makes the thermistor far more conducting and far less resistive.

16 of 18

## Resistivity (cont)

17 of 18

## Resistivity (cont)

- When the temperature of a conductor approaches absolute zero, the electrical resistance disappears completely.
- This occurs at a specific temperature for a material known as the critical temperature.
- At and below this temperature, no energy is transferred to the conductor as a current passes through it.
- This is called a superconductor.

18 of 18

## Related discussions on The Student Room

- explain how the terms potential and potential difference are linked. »
- Stuck with current & resistance »
- d.c. shunt motor »
- Physics P2 / P3 - PREDICTIONS »
- Fuse vs earth wire. Which is more effective? »
- Theory of Kirchhoff's law help! »
- GCE A and As level Physics Topical Past Papers 1976 to 2003 Download »
- IB physics help »
- what do a.c. and d.c. mean? »
- GCSE Physics (19/05) The Motor Effect »

## Similar Physics resources:

4.5 / 5

3.0 / 5

0.0 / 5

4.5 / 5

0.0 / 5

0.0 / 5

3.5 / 5

0.0 / 5

0.0 / 5

1.0 / 5

## Comments

No comments have yet been made