1. Electromagnetism Topic 12.1 Electromagnetic Induction

2. Induced Electromotive Force (e.m.f.) What is electromagnetic induction? What is electromagnetic induction? The diagram shows a copper rod connected to an ammeter: The diagram shows a copper rod connected to an ammeter: There is no battery in the circuit. There is no battery in the circuit.

3. What happens when you move the copper rod downwards, to cut across the horizontal magnetic field? What happens when you move the copper rod downwards, to cut across the horizontal magnetic field? The pointer on the meter makes a brief `flick' to the right, showing that an electric current has been induced. The pointer on the meter makes a brief `flick' to the right, showing that an electric current has been induced.

4. What happens when you move the rod upwards? What happens when you move the rod upwards? The meter again gives a `flick', but this time to the left. The meter again gives a `flick', but this time to the left. You have now induced a current in the opposite direction. You have now induced a current in the opposite direction.

5. If you hold the rod stationary, or if you move the rod along the field lines, there is no induced current. If you hold the rod stationary, or if you move the rod along the field lines, there is no induced current.

6. Why does electromagnetic induction occur? When you move the copper rod, its free electrons move with it. When you move the copper rod, its free electrons move with it. But when a charge moves in a magnetic field it experiences a force on it But when a charge moves in a magnetic field it experiences a force on it (the B Q v force). (the B Q v force). You can use Flemings Left hand Rule to show that the force on each electron is to the left as shown in the diagram You can use Flemings Left hand Rule to show that the force on each electron is to the left as shown in the diagram (Remember that an electron moving down has to be treated like a positive charge moving up. (Remember that an electron moving down has to be treated like a positive charge moving up.

8. So electrons accumulate at one end of the rod, making it negative. So electrons accumulate at one end of the rod, making it negative. This leaves the other end short of electrons and therefore positive. This leaves the other end short of electrons and therefore positive. There is now a voltage (potential difference) across the ends of the moving rod. There is now a voltage (potential difference) across the ends of the moving rod. If the ends of the moving rod are joined to form a complete circuit, the induced voltage causes a current to flow round the circuit as shown by the flick of the ammeter. If the ends of the moving rod are joined to form a complete circuit, the induced voltage causes a current to flow round the circuit as shown by the flick of the ammeter.

9. The induced voltage is a source of electrical energy ‑ an e.m.f The induced voltage is a source of electrical energy ‑ an e.m.f When a conductor is moving in a magnetic field like this, an e.m.f is induced, even if there isn't a complete circuit for a current to flow. When a conductor is moving in a magnetic field like this, an e.m.f is induced, even if there isn't a complete circuit for a current to flow.

10. Formula for a Straight Conductor Consider a conductor of length l that moves with velocity v perpendicular to a magnetic flux density or induction B as shown in the figure. Consider a conductor of length l that moves with velocity v perpendicular to a magnetic flux density or induction B as shown in the figure.

11. When the wire conductor moves in the magnetic field, the free electrons experience a force because they are caused to move with velocity v as the conductor moves in the field. When the wire conductor moves in the magnetic field, the free electrons experience a force because they are caused to move with velocity v as the conductor moves in the field. F = e v B F = e v B

12. This force causes the electrons to drift from one end of the conductor to the other, and one end builds ‑ up an excess of electrons and the other a deficiency of electrons. This force causes the electrons to drift from one end of the conductor to the other, and one end builds ‑ up an excess of electrons and the other a deficiency of electrons. This means that there is a potential difference or emf between the ends. This means that there is a potential difference or emf between the ends. Eventually, the emf becomes large enough to balance the magnetic force and thus stop electrons from moving. Eventually, the emf becomes large enough to balance the magnetic force and thus stop electrons from moving.

13. evB = eE ( from F = evB and F = eE) evB = eE ( from F = evB and F = eE) Therefore E = Bv Therefore E = Bv If the potential difference (emf) between the ends of the conductor is ε then If the potential difference (emf) between the ends of the conductor is ε then ε = E L (from E = V/d) ε = E L (from E = V/d) By substitution we have By substitution we have ε = B v L ε = B v L

14. Magnetic Flux The magnetic flux (Φ) through a region is a measure of the number of lines of magnetic force passing through that region. The magnetic flux (Φ) through a region is a measure of the number of lines of magnetic force passing through that region. Φ = AB cos θ Φ = AB cos θ where A is the area of the region and θ is the angle of movement between the magnetic field and a line drawn perpendicular to the area swept out. where A is the area of the region and θ is the angle of movement between the magnetic field and a line drawn perpendicular to the area swept out. The unit of magnetic flux is the weber Wb. The unit of magnetic flux is the weber Wb.

15. For a single conductor in the magnetic flux density, it can be seen that For a single conductor in the magnetic flux density, it can be seen that ε = - ΔΦ/ Δt (the rate of change of flux density) ε = - ΔΦ/ Δt (the rate of change of flux density) For N number of conductors as in the case for a solenoid, the term flux ‑ linkage is used. For N number of conductors as in the case for a solenoid, the term flux ‑ linkage is used. Then Then ε = - N Δ (Φ/ Δt) ε = - N Δ (Φ/ Δt) This is Faraday’s Law This is Faraday’s Law The minus sign shows us that the emf is always produced so as to oppose the change in flux. The minus sign shows us that the emf is always produced so as to oppose the change in flux.

16. Time-changing Magnetic Flux Therefore the production of an emf is produced by a time changing magnetic flux. Therefore the production of an emf is produced by a time changing magnetic flux. This could be due to the wire or coil moving through a magnetic field This could be due to the wire or coil moving through a magnetic field Or by an increasing or decreasing magnetic field of an electromagnet next to a wire or coil. Or by an increasing or decreasing magnetic field of an electromagnet next to a wire or coil.

17. Faraday’s Law We know that an e.m.f. is induced when there is a change in the flux linking a conductor. We know that an e.m.f. is induced when there is a change in the flux linking a conductor. Faraday's law makes the connection between the size of the induced e.m.f. and the rate at which the flux is changing. Faraday's law makes the connection between the size of the induced e.m.f. and the rate at which the flux is changing. It states that: It states that: the magnitude of the induced e.m.f is directly proportinonal to the rate of change of magnetic flux or flux linkage. the magnitude of the induced e.m.f is directly proportinonal to the rate of change of magnetic flux or flux linkage.

18. Linking For a single conductor in the magnetic flux density, it can be seen that For a single conductor in the magnetic flux density, it can be seen that ε = - ΔΦ/ Δt (the rate of change of flux density) ε = - ΔΦ/ Δt (the rate of change of flux density) And ε = B v l And ε = B v l Therefore - ΔΦ/ Δt = B v l Therefore - ΔΦ/ Δt = B v l

19. Lenz’s Law Faraday's law tells us the size of the induced e.m.f., but we can find its direction using Lenz's law Faraday's law tells us the size of the induced e.m.f., but we can find its direction using Lenz's law The direction of the induced e.m.f is such that it will try to oppose the change in flux that is producing it. The direction of the induced e.m.f is such that it will try to oppose the change in flux that is producing it.

21. Lenz's law is illustrated in the diagrams: As you move the N ‑ pole into the coil, an e.m.f. is induced which drives a current round the circuit as shown. Lenz's law is illustrated in the diagrams: As you move the N ‑ pole into the coil, an e.m.f. is induced which drives a current round the circuit as shown. Now use the right ‑ hand grip rule Now use the right ‑ hand grip rule Can you see that the current produces a magnetic field with a N ‑ pole at the end of the coil nearest to the magnet? Can you see that the current produces a magnetic field with a N ‑ pole at the end of the coil nearest to the magnet? So the coil repels the incoming magnet, and in this way the induced current opposes the change in flux. So the coil repels the incoming magnet, and in this way the induced current opposes the change in flux.

22. Why is the current reversed as you move the N ‑ pole out? Why is the current reversed as you move the N ‑ pole out? By Lenz's law, the coil needs to attract the receding N ‑ pole By Lenz's law, the coil needs to attract the receding N ‑ pole

23. Lenz's law is a result of the conservation of energy. If you move the magnet into the coil, you feel the repulsive force. Lenz's law is a result of the conservation of energy. If you move the magnet into the coil, you feel the repulsive force. You have to do work to move the magnet against this force. You have to do work to move the magnet against this force. And so energy is transferred from you (or the system that is moving the magnet) to the electrical energy of the current. And so energy is transferred from you (or the system that is moving the magnet) to the electrical energy of the current.