applications of inductor section 6.4. magnetic field applications of electromagnetism transformer

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Applications of Inductor Section 6.4

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Page 1: Applications of Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

Applications of Inductor

Section 6.4

Page 2: Applications of Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

• Magnetic Field• Applications of Electromagnetism• Transformer

Page 3: Applications of Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

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 Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

Flux Lines of magnets

Unlike Poles Attract

Like Poles Repel

Page 5: Applications of Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

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 Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

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 Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

Electromagnetism

Page 8: Applications of Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

Magnetic Field

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

Page 9: Applications of Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

Right-Hand Rule

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

Page 10: Applications of Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

Cumulative magnetic force

Page 11: Applications of Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

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 Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

Application #2

Page 13: Applications of Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

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 Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

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 Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

Application #3

A relay is used to open or close electrical contacts.

Page 16: Applications of Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

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 Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

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 Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

Application #5: Meter Movement

Page 19: Applications of Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

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 Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

A transformer

Page 21: Applications of Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

Polarity of transformer

IB

Bind

B

Bind

I

I

Page 22: Applications of Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

Symbols of transformer

Page 23: Applications of Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

Dot Convention (Section 6.4)

When the reference direction for a current enters the dotted terminal of a coil,the reference polarity of the voltage that it induces in the other coil is positive at its dotted terminal.

Page 24: Applications of Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

How to use Dot Convention in Circuit Analysis

i2 leaves the dotted terminal, therefore, the induced voltage across L1 is negative.

i1 enters the dotted terminal, therefore, the induced voltage across L2 is positive.

i2 leaves the dotted terminal.

Page 25: Applications of Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

A Procedure for Determine Dot Markings

Page 26: Applications of Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

Example

Page 27: Applications of Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer
Page 28: Applications of Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

Practice for Determining Dot Markings

Page 29: Applications of Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

Alternate Technique for Determining Polarity Marks

Page 30: Applications of Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

• We will revisit transformer in Chapter 9.

Page 31: Applications of Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

Example 6.6

Page 32: Applications of Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

Derivation of L1 and M

Page 33: Applications of Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

Derivation of L2 and M

Page 34: Applications of Inductor Section 6.4. Magnetic Field Applications of Electromagnetism Transformer

Energy Storage