Electromagnetism
under construction
The various syllabus statements cover very different quantities of material. I'm sorry there aren't any pictures yet. You need to read this page in conjunction with block 6 of the syllabus specification. xxx represents a page number in England, (3rd edition).
See below the table for a general introduction that applies to most of these syllabus statements. Points relating to particular syllabus statements are given in the hyperlinks, but those hyperlinks will assume that you have the general introduction at your fingertips.
1 | use the following units: ampere (A), volt (V), watt (W) 258-259 |
2 | recall that magnets repel and attract other magnets, and attract magnetic substances 258-259 |
3 | recall the properties of magnetically hard and soft materials 262-263 |
4 | understand the term ‘magnetic field line’ 258-261 |
5 |
understand that magnetism is induced in some materials when they are placed in a magnetic field ) 262-263 |
6 |
sketch and recognise the magnetic field pattern for a permanent bar magnet and that between two bar magnets 258-259 |
7 | know how to use two permanent magnets to produce a uniform magnetic field pattern 260-261 |
8 | recall that an electric current in a conductor produces a magnetic field round it 260-261 |
9 | describe the construction of electromagnets 262-263 |
10 |
sketch and recognise magnetic field patterns for a straight wire, a flat circular coil and a solenoid when each is carrying a current 260-261 |
11 |
appreciate that there is a force on a charged particle when it moves in a magnetic field as long as its motion is not parallel to the field - |
12 |
recall that a force is exerted on a current-carrying wire in a magnetic field, and, how this effect is applied in simple d.c. electric motors and loudspeakers 264-265, 268-269 |
13 |
predict the direction of the resulting force when a wire carries a current perpendicular to a magnetic field 264-265 |
14 |
recall that the force on a current-carrying conductor in a magnetic field increases with the strength of the field and with the current 264-265 |
15 |
recall that a voltage is induced in a conductor when it moves through a magnetic field or when a magnetic field changes through a coil; also recall the factors which affect the size of the induced voltage 270-272 |
16 |
describe the generation of electricity by the rotation of a magnet within a coil of wire and of a coil of wire within a magnetic field; also describe the factors which affect the size of the induced voltage 273-275 |
17 |
recall the structure of a transformer, and understand that a transformer changes the size of an alternating voltage by having different numbers of turns on the input and output sides 276-277 |
18 |
explain the use of step-up and step-down transformers in the large-scale generation and transmission of electrical energy 276-277, 278-279 |
19 |
recall and use the relationship between input (primary) and output (secondary) voltages and the turns ratio for a transformer secondary turns input (primary) voltage/output (secondary) voltage = primary turns / secondary turns Vp/Vs = np / ns 276-277, 278-279 |
20 |
recall and use the relationship input power = output power V p Ip = Vs Isfor 100% efficiency 276-277, 278-279 |
General introduction
You need to grasp three basic ideas:
Basic idea | Rule used | Notes |
current ® magnetic field | Right hand grip rule | thumb ® current, fingers ® field |
current + magnetic field ® motion | Left hand Motor rule |
First finger
®
Field seCond finger ® Current thuMb ® Motion (or THumb ® THrust) |
motion + magnetic field ® induced current | Right hand Dynamo rule |
Which rule to use ?
All currents produce magnetic fields. The strength of the field at any given instant is proportional to the size of the current at that instant, and also to the number of turns of wire on your coil. If you have two equal currents in roughly the same place, but flowing in opposite directions, then their magnetic fields cancel: this happens, for instance, in a two-core cable connecting a device to a supply, regardless of whether the supply is d.c. or a.c. It also happens in an RCCB, used nowadays where fuses used to be employed. Use the right hand grip rule to determine the direction of the field produced by the current.
An electromagnet* placed near to a magnet** will be attracted to, repelled by or deflected by the magnetic field. This is the principle of the electric motor. If you start with a current and a magnet, and get motion as a result, then you should use the Left hand Motor rule. Notice that L and M come next to each other in the alphabet. This rule applies to obvious things like electric motors, but also to less obvious situations like loudspeakers (where the initial current comes from an amplifier and the resulting movement makes a sound wave) and electric bells (in which the resulting movement causes a hammer to hit a gong). Notice that the 'magnet' referred to above might itself be an electromagnet.
* or a current-carrying wire
** which might itself be another electromagnet or even another current carrying wire
Induced currents occur when you change the magnetic environment of a coil of wire. For example
Take a magnet away from a wire
Bring a magnet close to a wire
Wave a magnet around near a wire
Twist a wire coil in a magnetic field
Move a wire in a magnetic field
Vary the current in an electromagnet that happens to be nearby
In the first five of these cases you start with motion and get a current as a result, so everything is the other way round to the situation in the preceding paragraph. The appropriate rule to use here is the Right hand Dynamo rule.
In deciding which rule to use, it's the bits in purple and yellow that you have to think about.
Faraday's Law
This law is enormously useful, and you need to learn it word-perfectly
The induced emf is proportional to the rate of change of magnetic flux linkage. |
'emf' stands for 'electro-motive force', which effectively means 'electron-moving force'. Bizarrely, it is measured in volts. The emf then generates an induced current, whose size depends on the resistance of the coils and whatever is connected to them, as well as on the size of the emf itself.
Using the law to explain why there is an induced emf.
You have to show that all three coloured phrases apply. So you have to state the law and then establish that
there is some magnetism present, either from an electromagnet or a permanent magnet
there is some linkage: i.e. that magnetic field lines are threaded through some coils of wire
there is some change of linkage, for example by rotating the coil, rotating the magnet, dropping the coil, dropping the magnet, altering the strength of an electromagnet be switching it on or off, or by supplying it with a.c., etc. Notice that a d.c. electromagnet close to a stationary coil doesn't satisfy the rate of change condition.
Using the law to explain how to increase or decrease the induced emf.
Changing any one of the three coloured phrases will change the emf, because of the 'is proportional to' bit. Thus, to double the emf in a generator you could
double the strength of the magnet (magnetic flux)
double the number of turns on the coil (linkage)
double the speed of rotation (rate of change).