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9. Electromagnetic Induction
Electromagnetic Induction If an electric current produces a magnetic field, then a magnet should be able to generate an electric current. A current is produced in a wire when there is relative motion between the wire and a magnetic field. Such a current is called an induced current . This effect is called electromagnetic induction (discovered by Michael Faraday). The strength of the current depends on the magnetic field strength and the wireβs speed. Magnetic flux
Magnetic flux, π·π·, represents a quantity of magnetic force lines passing through a given area. The number of magnetic force lines increases if we have a stronger field or if the area enclosed is larger. οΏ½β, perpendicular to the plane of the loop Therefore, π·π· = π΅π΅β₯ π΄π΄. Where π΅π΅β₯ is the component of B In SI units, flux is measured in webers (Wb) and is calculated from π·π· = π΅π΅β₯ π΄π΄ with B measured in Tesla and A in meters squared. It is important to note that only the component of the magnetic field perpendicular to the area is used in the calculation. Thus, in general, π·π· = π΅π΅π΅π΅ cos ππ where ππ is the angle between the magnetic field and the normal to the area. R
Suppose we have a magnetic field going through a surface. Then the perpendicular component of the magnetic field going through the surface times the area of the surface is called the magnetic flux. General Expression: οΏ½β. πππ΄π΄β ππ = β« π΅π΅
Simple case 1: uniform π΅π΅β₯ surface: π·π· = π΅π΅π΅π΅ Simple case 2: surface is closed: Ξ¦ = 0 3.
Faradayβs Law
ππππ
ππ = β ππππ The emf induced in any loop or circuit is equal to the negative rate of change of the magnetic flux through that loop.
Fig. 1. Voltmeter reading gives rate of change of the number of lines linking the loop.
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Lenzβs Law
ππππ
ππ = β ππππ The direction of the induced emf is such as to create a current which will oppose the change in the flux.
Faradayβs Law: General Form
Fig.2. Motion as shown produces clockwise current which makes B field opposing the increase.
οΏ½ πΈπΈοΏ½β . ππππβ = β
πΆπΆ
β Ξ΅
ππ οΏ½β. πππ΄π΄β οΏ½ π΅π΅ ππππ πΆπΆ
β Ο
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