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Applications of Inductors and Capacitors Section 6.3
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Applications of Inductors and Capacitors Section 6.3.

Dec 20, 2015

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Page 1: Applications of Inductors and Capacitors Section 6.3.

Applications of Inductors and Capacitors

Section 6.3

Page 2: Applications of Inductors and Capacitors Section 6.3.

• The magnetic field• Electromagnetism• Applications of Electromagnetism• Electromagnetic Induction

Page 3: Applications of Inductors and Capacitors Section 6.3.

Magnetic Field

• Flux lines are used to represent the strength and the direction of the field.• The flux lines are always drawn from the north pole to the south pole.

Page 4: Applications of Inductors and Capacitors Section 6.3.

Flux Lines of magnets

Unlike Poles Attract

Like Poles Repel

Page 5: Applications of Inductors and Capacitors Section 6.3.

How materials become magnetized

• Ferromagnetic Materials such as iron and nickel become magnetized when Placed in the magnetic field of a magnet• Objects become magnetized (i.e. they become magnets themselves) under the Influence of the permanent magnetic field and become attracted to the magnet.• When removed from the magnetic field, the objects tends to lose its magnetism.• Ferromagnetic materials have minute magnetic domains created within theiratomic structure.

Page 6: Applications of Inductors and Capacitors Section 6.3.

Application 1: Magnetic switch

When the magnet is near the switch mechanism, the switch is closed.When the magnet is moved away, the spring pulls the arm open.

Page 7: Applications of Inductors and Capacitors Section 6.3.

Electromagnetism

Page 8: Applications of Inductors and Capacitors Section 6.3.

Magnetic Field

Note: The field is stronger closer to the conductor and becomes weakerwith increasing distance from the conductor.

Page 9: Applications of Inductors and Capacitors Section 6.3.

Right-Hand Rule

Thumb: Points in the direction of currentFingers: point in the direction of the magnetic lines of force.

Page 10: Applications of Inductors and Capacitors Section 6.3.

Cumulative magnetic force

Page 11: Applications of Inductors and Capacitors Section 6.3.

Application #1: Electromagnet

When the coil of wire is connected to a battery, there is current. A magnetic field is established.

Page 12: Applications of Inductors and Capacitors Section 6.3.

Application #2

Page 13: Applications of Inductors and Capacitors Section 6.3.

Solenoid

A basic solenoid consists of three parts: (Section 10-3)1. Coil2. A stationary iron core3.A sliding core (plunger) is attached to the stationary core with a spring.

Applications: opening and closing valves and automobile door locks.

Page 14: Applications of Inductors and Capacitors Section 6.3.

Steps:1.In the rest state, the plunger is extended.2.The solenoid is energized by current through the coil, which sets up an electromagnetic field that magnetizes both iron cores.3. The south pole of the stationary core attracts the north pole of the movable coil causing it to slide inward, thus retracting the plunger and compressing the spring.4.When the current is cut off, the magnetic fields collapse and the force of the Compressed spring pushes the plunger back out.

Magnetic fields in the core points from right to left.

Page 15: Applications of Inductors and Capacitors Section 6.3.

Application #3

A relay is used to open or close electrical contacts.

Page 16: Applications of Inductors and Capacitors Section 6.3.

When there is no coil current, the iron armature is held against the upper contact by the spring, thus providing continuity from terminal 1 to terminal 2.

When energized with coil current, the armature is pulled down by the attractive force of the electromagnetic field and makes connection with the lower contact,providing continuity from terminal 1 to terminal 3.

Page 17: Applications of Inductors and Capacitors Section 6.3.

Application #4Reed Relay

• Reed is made of ferrous material. • When there is no coil current, the reeds are in the open position.• Where there is current, the reeds make contact because they are magnetizedand attract each other.

Page 18: Applications of Inductors and Capacitors Section 6.3.

Application #5: Meter Movement

Page 19: Applications of Inductors and Capacitors Section 6.3.

Current in: crowded flux lines above, resulting in downward force on the right.Current out: crowded flux lines below, resulting in upward force on the left.

Page 20: Applications of Inductors and Capacitors Section 6.3.

Electromagnetic Induction

Page 21: Applications of Inductors and Capacitors Section 6.3.

Faraday’s observation

• A changing magnetic field can induce a voltage in a conductor.

Page 22: Applications of Inductors and Capacitors Section 6.3.

Faraday’s First Observation

The amount of voltage induced in a coil is directly proportional to the rate of change of the magnetic field with respect to the coil.

Page 23: Applications of Inductors and Capacitors Section 6.3.

Faraday’s second observation

The amount of voltage induced in a coil is directly proportional to the numberof turns of wire in a coil.The induced current generates a voltage across the input resistance of the voltmeter.

Page 24: Applications of Inductors and Capacitors Section 6.3.

Lenz’ law

http://hyperphysics.phy-astr.gsu.edu/HBASE/electric/farlaw.html#c2

When an emf is generated by a change in magnetic flux according to Faraday's Law, the polarity of the induced emf is such that it produces a current whose magnetic field opposes the change which produces it.

Page 25: Applications of Inductors and Capacitors Section 6.3.

Effective Inductance/Capacitance

Page 26: Applications of Inductors and Capacitors Section 6.3.

Series Inductance

Page 27: Applications of Inductors and Capacitors Section 6.3.
Page 28: Applications of Inductors and Capacitors Section 6.3.

Series Capacitance

Page 29: Applications of Inductors and Capacitors Section 6.3.

Parallel Capacitance