4.1 Force on a Current-carrying Conductor in a Magnetic Field
A current-carrying conductor in a magnetic field experiences a force; its direction depends on the current direction and the magnetic field direction. (p.137)
Catapult field: the resultant field from the interaction of the conductor's field and the permanent magnet's field. (p.138)
Fleming's left-hand rule: index finger = magnetic field (N to S), middle finger = current, thumb = force/motion. (p.139)
Force increases with larger current and stronger magnetic field. (p.141)
A current-carrying coil in a magnetic field rotates due to a pair of equal, opposite forces. (p.142)
The commutator and carbon brushes of a d.c. motor reverse the current every half rotation so the coil keeps turning one way. (p.144)
Motor speed increases with greater current (voltage), stronger magnetic field and more coil turns. (p.146)
Brushless motor: coil stationary, magnet rotates; no brush friction, no sparking, quieter. (p.147)
4.2 Electromagnetic Induction
Electromagnetic induction is the production of an induced e.m.f. in a conductor when there is relative motion between conductor and magnetic field, or the conductor is in a changing magnetic field. (p.153)
Induced e.m.f. increases with faster relative motion, more solenoid turns and stronger magnetic field. (p.155)
Faraday's law: the magnitude of induced e.m.f. is directly proportional to the rate of cutting of magnetic flux. (p.155)
Fleming's right-hand rule (straight wire): thumb = motion, fore finger = magnetic field, middle finger = induced current. (p.157)
Lenz's law: the induced current flows in a direction that opposes the change of magnetic flux that causes it. (p.159)
D.c. generator uses a split-ring commutator; a.c. generator uses two slip rings. (p.160)
4.3 Transformer
A transformer works with a.c.; the changing flux in the soft iron core induces an a.c. voltage in the secondary coil. (p.163)