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Physics 4 – March 20, 2018 P3 Challenge – A uniform magnetic field of B = 3.5 mT is directed into the page. An electron approaches this field from the.

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Presentation on theme: "Physics 4 – March 20, 2018 P3 Challenge – A uniform magnetic field of B = 3.5 mT is directed into the page. An electron approaches this field from the."— Presentation transcript:

1 Physics 4 – March 20, 2018 P3 Challenge – A uniform magnetic field of B = 3.5 mT is directed into the page. An electron approaches this field from the left at v = 3.2 x 105 m/s. Determine the magnitude and direction of the force on the electron. Get out p241 #37-46 for Hmk Check

2 Objectives/Agenda/Assignment
Ch 11.1 Induction Assignment: p442 #1-13 Agenda: HMK review Induced motional EMF Magnetic flux Faraday’s Law Lenz’s Law

3 Motional Electromotive Force (EMF)
We’ve seen that a current carrying wire creates a magnetic field. The opposite cause and effect can also occur. A magnetic field can cause charges in a wire to move. How? By moving a wire segment through a magnetic field.

4 Motional Electromotive Force (EMF)
Right hand rule shows that the magnetic field pushes protons up and electrons down when the rod is moved to the right. The result is a separation of charge, which is a potential difference V… an induced EMF while the rod is moving.

5 Magnitude of induced EMF 
 = BvL where B is the magnetic field (T), v is the speed of the wire moving through the field, and L is the length of the wire located within the field. Called a motional EMF because it requires motion to create the EMF. It must continue moving to keep the EMF. In practice, it’s often the magnet that moves relative to a fixed wire, e.g. a fixed magnet moving in a solenoid.

6 Magnitude of induced EMF 
If there are multiple loops of wire, you can multiply this EMF by the number of loops, N, to find the overall EMF of the solenoid.  = BvLN Both of these forms are in the data packet

7 Power of Induced EMF Connecting this EMF to a simple circuit, you can determine the current through a resistor, R. IR = BvL then solve for I = BvL/R The now current carrying wire generates a force F = BIL = B(BvL/R)L = B2vL2 /R Recall Power = Fv = W/t Power of the force generated by the induced EMF: P = (B2vL2 /R)v = B2v2L2 /R Remembering  = BvL , P= 2/R This is equivalent to P = V2/R we saw before in Ch 5.2.

8 Induced EMF Observation of this system show larger currents with: Greater relative speed, v Stronger magnetic field, B Higher number of turns, N Greater area of loop, A Max value when magnet and turns are perpendicular,  Something more than just the Magnetic field strength, B is operating here that involves A and 

9 Magnetic Flux,  The amount of magnetism flowing normally (perpendicular) over an area is called the magnetic flux, . The magnitude of magnetic flux is  = BAcos where  is the angle relative to the normal to the area. Unit = weber Wb, 1 Wb = 1 T m2

10 Magnetic Flux,  Only the component of the magnetic field lines perpendicular to the plane of the area contribute to the magnetic flux. Useful analogies: Hair within a rubberband or noodles in a loop => magnetic field lines within a given area. Flux is the number of hair, noodles or field lines. When the magnetic field passes through many loops of a solenoid, it is call a magnetic flux linkage and  = NBAcos

11 Faraday’s Law The induced EMF is equal to the rate of change of the magnetic flux linkage:  = N /t. Known as Faraday’s law.  = BAcos and  is the angle to the normal to the area Note: A changing flux creates an induced EMF, not necessarily a current. For a current it has to be placed in a circuit with a resistor. Ex: The magnetic field through a single loop of area 0.20 m2 is changing at a rate of 4.0 T/s. What is the induced EMF?

12 Lenz’s Law The induced EMF will be in such a direction as to oppose the change in the magnetic flux that created the current. Pretend the loop is a solenoid with one turn and use the Right Hand Grip rule to determine the direction of a magnetic field for the current carrying wire loop that will oppose the “change direction” Label B direction, label change in B direction, ID B direction created by current, and finally ID the direction of the current. Consider a loop in a field directed into board a) increasing, b) decreasing Consider a loop in a field directed out of board a) increasing b) decreasing

13 Exit slip and homework Exit Slip – What is the magnetic flux linkage for a 3.5 mT magnetic field is present through a solenoid with 50 turns and a 6.25 cm radius? What’s due? (homework for a homework check next class) P442 #1-13 What’s next? (What to read to prepare for the next class) Read 11.2 AC Power, p


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