Magnetically Induced Electromotive Force
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The magnitude of the electromotive force is proportional to the rate of change of the field. The sense of the induced electromotive force depends on the direction of the rate of the change of the field. Equipment required The tube-coil arrangement, mounted vertically, as shown in Figure 1.
Magnetic Flux, Induction, and Faraday’s Law
Carrying out the experiment Drop the magnet through the coil, making sure you catch it before it hits the floor! The north and south poles are not marked on the magnets. Investigate Faraday's second law by changing the position of the coil and therefore changing the speed the magnet will drop past the coil. Think about how this will affect the induced EMF.
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Keeping the north pole facing down, drop the magnet and see if you are are correct. Investigate Faraday's third law by dropping the magnet with the south pole facing down. Think about how the induced EMF will change - try it and see if you are correct.
Electromagnetic induction - Wikipedia
Analyzing the results A typical trace is shown below using PicoScope 6 as illustrated in Figure 2. The galvanometer is used to detect any current induced in the coil on the bottom. It was found that each time the switch is closed, the galvanometer detects a current in one direction in the coil on the bottom. You can also observe this in a physics lab.
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Each time the switch is opened, the galvanometer detects a current in the opposite direction. Interestingly, if the switch remains closed or open for any length of time, there is no current through the galvanometer. Closing and opening the switch induces the current. It is the change in magnetic field that creates the current. More basic than the current that flows is the emf that causes it.
A-level Physics/Forces, Fields and Energy/Electromagnetic induction
The current is a result of an emf induced by a changing magnetic field , whether or not there is a path for current to flow. An experiment easily performed and often done in physics labs is illustrated in [link].
An emf is induced in the coil when a bar magnet is pushed in and out of it. Emfs of opposite signs are produced by motion in opposite directions, and the emfs are also reversed by reversing poles. The same results are produced if the coil is moved rather than the magnet—it is the relative motion that is important. The faster the motion, the greater the emf, and there is no emf when the magnet is stationary relative to the coil. The method of inducing an emf used in most electric generators is shown in [link].
A coil is rotated in a magnetic field, producing an alternating current emf, which depends on rotation rate and other factors that will be explored in later sections. Note that the generator is remarkably similar in construction to a motor another symmetry.
So we see that changing the magnitude or direction of a magnetic field produces an emf. Experiments revealed that there is a crucial quantity called the magnetic flux , , given by. Any change in magnetic flux induces an emf.
This process is defined to be electromagnetic induction. Units of magnetic flux are. Thus magnetic flux is , the product of the area and the component of the magnetic field perpendicular to it. All induction, including the examples given so far, arises from some change in magnetic flux. For example, Faraday changed and hence when opening and closing the switch in his apparatus shown in [link]. This is also true for the bar magnet and coil shown in [link]. When rotating the coil of a generator, the angle and, hence, is changed.