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Welcome to our Physics lesson on Induction and Energy Transfer, this is the first lesson of our suite of physics lessons covering the topic of Induction and Energy Transfers, you can find links to the other lessons within this tutorial and access additional physics learning resources below this lesson.
It is a known fact (from Lentz law) that when a magnet is moving towards or away from a coil, a resistive effect in the form of magnetic force is produced in the coil - an effect which is in the opposite direction to the external force exerted on the coil - in order to move the magnet. This external force does positive work on the system, resulting in an increase in the energy of the system. The current induced in the coil produces a resistance in it, resulting in the delivering of a certain amount of thermal energy. In other words, the energy produced due to the magnet's motion (mechanical energy) is converted into thermal energy of the coil. All this process occurs without any direct contact, but through induction. Therefore, we say "induction results in a transfer of energy between the parts of a system." We have discussed this feature of induction when explaining the methods of energy transfer in Section 13, more precisely in the tutorial 13.4.
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.
In the figure above, the magnetic flux through the solenoid (coil) is changing because when the magnet gets closer to the coil (direction 1), more magnetic field lines enter the area of coil compared to the case when the magnet moves away from the coil (position 2). In other words, the flux changes because the magnetic field produced by the moving magnet changes.
The same effect is obtained when we move a rectangular coil (as the one shown in the figure below) in the left-right and vice-versa direction.
During this process, the magnetic flux can change in two ways:
The two situations described above, basically represent the same phenomenon - the change in magnetic flux in the coil. However, the setup shown in the last figure (the rectangular coil moving relative to a uniform magnetic field) offers a great advantage regarding the calculation of work done to move the coil out of the magnetic field, as the field lines here are parallel and uniformly distributed, unlike those produced when a bar magnet moves towards or away the solenoid. Therefore, we will consider only the second setup described above when calculating the amount of mechanical work done during this process.
You have reached the end of Physics lesson 16.10.1 Induction and Energy Transfer. There are 6 lessons in this physics tutorial covering Induction and Energy Transfers, you can access all the lessons from this tutorial below.
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