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In addition to the revision notes for Induction and Energy Transfers on this page, you can also access the following Magnetism learning resources for Induction and Energy Transfers
Tutorial ID | Title | Tutorial | Video Tutorial | Revision Notes | Revision Questions | |
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16.10 | Induction and Energy Transfers |
In these revision notes for Induction and Energy Transfers, we cover the following key points:
Induction results in a transfer of energy between the parts of a system. If the energy lost due to radiation is neglected, we say that the faster the magnet is moved, greater the work done by the external force in a certain time and therefore, greater the rate of energy transfer in the loop. This means the power of this energy transfer is greater when the magnet moves faster.
The moving direction of magnet is not important; as long as the magnet is moving, it transfers energy to the coil.
The magnetic flux produced when we move a coil inside a uniform magnetic field can change in two ways:
The magnitude of the induced emf in the coil is
where w is the width of the rectangular coil and v is its moving velocity.
Giving that the magnetic force produced in a current carrying wire is
we obtain for the magnetic force induced in the coil
The last equation means that if the magnetic force Fm is constant, the moving speed v of the coil is constant as well. This is because the other parameters such as the magnetic field B, the width of loop w and the resistance R are all constants.
The rate of work (i.e. the mechanical power) done by the external force F when moving the coil inside a uniform magnetic field is
As for the rate of thermal energy produced in the coils, we have:
The above two equations give the same value. This means the work done for pulling the loop through a magnetic field is transferred entirely to the loop in the form of thermal energy.
The circular currents produced when we replaced the rectangular frame with a solid rectangular plate are known as eddy currents (eddy = whirlpool).
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