Induced Emf (DP IB Physics)
Revision Note
Induced Emf
Electromagnetic induction is a phenomenon which occurs when an e.m.f. is induced due to relative movement between a conductor and a magnetic field
This could occur when:
a conductor moves relative to a magnetic field
a magnetic field varies relative to a conductor
When a conductor cuts through magnetic field lines:
the free electrons in the conductor experience a magnetic force
this causes work to be done as charges in the conductor become separated
mechanical work is transferred to the charges as electric potential energy
a potential difference is created between the ends of the conductor, or in other words, an e.m.f. is induced
This induced e.m.f. is defined as:
The amount of work done per unit charge in separating the charges to the ends of a conductor
If the ends of the conductor are connected to a closed circuit, an induced current will be able to flow
Therefore, we can define electromagnetic induction as:
The process in which an e.m.f or current is induced in a closed circuit due to changes in magnetic flux
To induce a current in a straight current-carrying conductor in a magnetic field
it must be placed in a perpendicular field, so when it moves it cuts the magnetic field lines
the closed circuit must be positioned outside of the field, so the e.m.f. is induced across the conductor in the field only, and not the entire circuit (which would mean no current flow)
Conducting rod moving perpendicular to a magnetic field directed into the page
The induced e.m.f in the conductor, as it moves through the magnetic field, is:
Where:
ε = induced e.m.f. (V)
B = magnetic flux density (T)
L = length of the conductor in the field (m)
v = velocity of the conductor travelling through the field (m s–1)
This equation shows that the size of the induced e.m.f increases if:
the length of the conductor in the field is increased
the magnetic field strength is increased
the conductor cuts through the field lines faster
Coiling a wire to form many loops or turns, will also increase the size of the induced e.m.f.
For a coil moving through a magnetic field, the induced e.m.f. is:
Where N = number of turns on the coil
The phenomenon of EM induction can be demonstrated using a magnet and a coil, or a wire and two magnets
Experiment 1: Moving a magnet through a coil
When a coil is connected to a sensitive voltmeter, a bar magnet can be moved in and out of the coil to induce an e.m.f
A bar magnet is moved through a coil connected to a voltmeter to induce an e.m.f
The expected results are...
When the bar magnet is not moving, the voltmeter shows a zero reading
When the bar magnet is held still inside, or outside, the coil, the rate of change of flux is zero, so, there is no e.m.f induced
When the bar magnet begins to move inside the coil, there is a reading on the voltmeter
As the bar magnet moves, its magnetic field lines ‘cut through’ the coil, generating a change in magnetic flux (ΔΦ)
This induces an e.m.f within the coil, shown momentarily by the reading on the voltmeter
When the bar magnet is taken back out of the coil, an e.m.f is induced in the opposite direction
As the magnet changes direction, the direction of the current changes
The voltmeter will momentarily show a reading with the opposite sign
Increasing the speed of the magnet induces an e.m.f with a higher magnitude
As the speed of the magnet increases, the rate of change of flux increases
An e.m.f is induced only when the bar magnet is moving through the coil
Factors that will increase the magnitude of the induced e.m.f are:
Moving the magnet faster through the coil
Adding more turns to the coil
Increasing the strength of the bar magnet
Experiment 2: Moving a wire through a magnetic field
When a long wire is connected to a voltmeter and moved between two magnets, an e.m.f is induced
Note: there is no current flowing through the wire to start with
A wire is moved between two magnets connected to a voltmeter to induce an e.m.f
The expected results are...
When the wire is not moving, the voltmeter shows a zero reading
When the wire is held still inside, or outside, the magnets the rate of change of flux is zero so there is no e.m.f induced
As the wire moves between the magnets, an e.m.f is induced within the wire
This is shown momentarily by the reading on the voltmeter
As the wire moves through the magnetic field, it ‘cuts through’ the magnetic field lines, generating a change in magnetic flux
When the wire is moved back out of the field, an e.m.f is induced in the opposite direction
As the wire changes direction, the direction of the current changes
The voltmeter will momentarily show a reading with the opposite sign
Factors that will increase the magnitude of the induced e.m.f are:
Increasing the length of the wire
Moving the wire between the magnets faster
Increasing the strength of the magnets
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